CHAPTER 2 BELT DRIVES SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 151
CHAPTER 2
BELT DRIVES SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 251
APPLICATIONS OF BELT DRIVES
VEHICLES
INDUSTRIAL
AUTOMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 351
Another method widely used in engineering practice in transmitting powerbetween shafts is belt drive system
Basic arrangement of a belt drive system consists of driver sheave driven sheaveand belting material such as ropes rubber bands or chain
The operation of belt drives depends fully on the friction generated from contactsurface between the belt and sheaves Thus any slip occurrence on the contactsurface will reduce the efficiency of the power transmitted
The choice of type of belt to be used is important so that the required power can bedelivered efficiently Some of the factor to be considered in selecting a suitable belttype to be used for a particular application is
- Speed of driver and driven sheaves
- Required velocity ratio- Distance between the driver sheave and driven sheave- Workspace constraint- Total power to be transmitted
INTRODUCTION TO BELT DRIVE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 451
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 551
BELT DRIVE ARRANGEMENTS
Compound Belt Drives
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 251
APPLICATIONS OF BELT DRIVES
VEHICLES
INDUSTRIAL
AUTOMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 351
Another method widely used in engineering practice in transmitting powerbetween shafts is belt drive system
Basic arrangement of a belt drive system consists of driver sheave driven sheaveand belting material such as ropes rubber bands or chain
The operation of belt drives depends fully on the friction generated from contactsurface between the belt and sheaves Thus any slip occurrence on the contactsurface will reduce the efficiency of the power transmitted
The choice of type of belt to be used is important so that the required power can bedelivered efficiently Some of the factor to be considered in selecting a suitable belttype to be used for a particular application is
- Speed of driver and driven sheaves
- Required velocity ratio- Distance between the driver sheave and driven sheave- Workspace constraint- Total power to be transmitted
INTRODUCTION TO BELT DRIVE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 451
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 551
BELT DRIVE ARRANGEMENTS
Compound Belt Drives
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 351
Another method widely used in engineering practice in transmitting powerbetween shafts is belt drive system
Basic arrangement of a belt drive system consists of driver sheave driven sheaveand belting material such as ropes rubber bands or chain
The operation of belt drives depends fully on the friction generated from contactsurface between the belt and sheaves Thus any slip occurrence on the contactsurface will reduce the efficiency of the power transmitted
The choice of type of belt to be used is important so that the required power can bedelivered efficiently Some of the factor to be considered in selecting a suitable belttype to be used for a particular application is
- Speed of driver and driven sheaves
- Required velocity ratio- Distance between the driver sheave and driven sheave- Workspace constraint- Total power to be transmitted
INTRODUCTION TO BELT DRIVE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 451
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 551
BELT DRIVE ARRANGEMENTS
Compound Belt Drives
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 451
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 551
BELT DRIVE ARRANGEMENTS
Compound Belt Drives
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 551
BELT DRIVE ARRANGEMENTS
Compound Belt Drives
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 651
BELT DRIVE ARRANGEMENTS
Stepped Cone Pulley
Step or cone pulley is used forchanging speed of driven shaftwhile the driver shaft runs atconstant speed
This is achieved by shifting thebelt from one part of the step to
the other
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 751
TYPES OF BELT AND MATERIAL
Flat belt ndash Most commonly used in factories workshops Used when moderatepower is to be transmitted Limitation for centre distance is not more than 8meter
V-Belts ndash Commonly used in factories workshops and is used when great
amount of power is to be transmitted when the centre distance is near to eachother
Circular belt Rope ndash Used when great amount of power is to be transmittedwhen centre distance for both pulleys are more than 8 meter apart
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 851
Material used for belts must be strong durable and flexible It must have highcoefficient of friction micro The material used are
1 Leather belt
2 Rubber belt
3 Cotton fabric belts
The coefficient of friction of belts depends upon factors such as belt materialpulley material slip of belt and speed of belt Table shows some of micro value for
belt and pulley material
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 951
VELOCITY RATIO FOR BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1051
SLIP IN BELT DRIVE SYSTEM
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1251
ANGLE OF LAP
It is the enclosed angle in which the belt and surface of pulley are in contact
It is important for determining the right setting of driver and driven pulley toguarantee an effective power transmission
For Open belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1351
For Cross belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1451
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Open Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1551
OVERALL LENGTH OF BELT DRIVE SYSTEM
For Cross Belt arrangement
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1651
Belt tension in a belt drive system can be expressed in terms of ratio betweentension on the tight side and the slack side of the same belt when it was operating
In order for the belt to produce torque on the wheel (whether or not it is rotating)there must be tension in both ends
The tension in one end must be greater than the tension in the other hand Let thetension T+dT is larger than T where dT is the small increment in tension Consideran elementary length of the belt on the pulley
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1751
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1851
BELT RATIO
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 1951
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2051
BELT RATIO FOR VEE BELT SYSTEM
For Vee Belt system the samederivation technique can be
applied to get the Belt Ratio forVee Belt system
The wedging effect of the beltincreases the reaction forcebetween the pulley and the belt
Total reaction force R is R=2R rsquo sin β
Previously dT =microRrsquo but for Vee Belt dT = 2 microRrsquo
Thus
sinsin2
22 R R
RdT
For complete derivation integrating between the limits as previous approach
sin
2
1e
T
T
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2151
Case Study CVT vs Gears Technology
Traditional car manufacturer uses gears as the primary drive train These gearswill have interlocking toothed wheels that help transmit and modify rotary motion
and torque A combination of planetary gears creates all of the different gearratios that the transmission can produce When this type of transmission cyclesthrough its gears the driver can feel jolts as each gear is engaged
Continuously Variable Transmissions(CVT) dont have a gearbox with set ofgears
The most common type of CVToperates on an ingenious pulley
system that allows an infinite variabilitybetween highest and lowest gears withno discrete steps or shifts
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2251
Case Study CVT vs Gears Technology
The simplicity and steeples nature of CVT make them an ideal transmissionfor a variety of machines and devices not just cars CVT have been usedfor years in power tools and drill presses Theyve also been used in avariety of vehicles including tractors and motor scooters
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2351
So whats different about these CVT-based cars -- cars like the Saturn Vue theAudi A4 and A6 the Nissan Murano and the Honda Insight
The animation below which compares the acceleration of a car with a CVT to onewithout can give a good feel for the experience
PLAY THE ANIMATION
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2451
Example 1
Two pulleys one 450mm dia and the other 200 mm dia on parallel shaft 195mapart are connected by a crossed belt Find the length of the belt required andthe angle of contactlap between the belt and each pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2551
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2651
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2751
Example 2
A compound belt drive will have these properties
a) Find the speed of follower pulley D in terms of above properties
b) Find the speed of follower pulley D in terms of above properties if thethickness of belt and slip is taken into consideration Assume S is thetotal slip for all pulley
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2851
Solution
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 2951
POWER TRANSMISSION OF BELT DRIVES
The tension in a belt pulley increases with torque and power The maximum powerthat a pulley system can transmit is limited by the strength of the belt material
If this is a problem then more than one belt should be used to share the loadFor power to be delivered to the driven pulley thus the driver pulley will pull the belt(tight side) and delivers it to the other side (slack side) Thus the tight side will havetension greater than the slack side
Thus the effective driving force is the difference between tight and slack side
tension (T1-T2)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3051
MAXIMUM POWER WITH NO BELT SLIP
v
e
T P
sin
1
11
For Vee Belt power is
Watt
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3151
EFFECT OF CENTRIFUGAL FORCE
C O C G O C
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3251
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3351
EFFECT OF CENTRIFUGAL FORCE
EFFECT OF CENTRIFUGAL FORCE
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3451
EFFECT OF CENTRIFUGAL FORCE
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3551
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Earlier we have shown that how to achieve maximum power at no slip condition(ideal condition) However in practice centrifugal force effect exist for high speedapplication system of belt drive This will cause slippage likely to occur since
centrifugal force tends to lift the belt off the pulley
So how do we maximize the full power of the belt drive system by takingconsideration on the centrifugal effect
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3651
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3751
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Example 3 A leather belt with cross sectional area of 2250mm2 is used to drive a cast ironpulley 900 mm in diameter at 336 rpm If the angle of lap is 120deg and the stressin the tight side is 2 MPa find
a) Effective tension on the tight side of belt
b) Centrifugal force acting on the belt
c) Effective tension on the slack side of the belt
d) Power capacity of the belt
The density of the leather is 980 kgm3 and the coefficient of friction is
035
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3851
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
Solution
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 3951
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4051
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4151
MAXIMUM POWER WITH CENTRIFUGAL EFFECT INCLUDED
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4251
INITIAL TENSION OF BELT DRIVES
INITIAL TENSION OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4351
INITIAL TENSION OF BELT DRIVES
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4451
CREEP OF BELT DRIVES
When power is transmitted by a belt or rope there is always a difference betweenthe peripheral speed of the driving pulley and that of driven pulley Because ofdifferent tensions on the two sides of the pulley the stretch in the belt will be
different
Consider one metre length of belt when unstressed Because of tension T 1 onthe tight side the length of the belt is (1 + x1) metre where x1 is the stretchSimilarly due to tension T2 on the slack side the length of the belt is (1 + x2) metre where x2 is the stretch Obviously x1 is greater than x2
A length (1 + x1) metre has approached the driver but only (1 + x2) metre hasmoved off the driver Thus the length of belt that leaves the driver pulley is lessthan that which has approached it
Thus there is some relative motion of the belt on the pulley and the belt is saidto creep The effect of creep in belt is to reduce the speed of the follower andreduce the power output
CREEP OF BELT DRIVES
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4551
CREEP OF BELT DRIVES
E ample 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4651
Example 4
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4751
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4851
Example 5
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 4951
Example 5
Design a rubber belt to drive a dynamo generating 20 kW of power at 2250 rpmand fitted with a pulley 200 mm diameter Assume dynamo efficiency to be 85The data given are
Allowable stress for belt = 21 MPa
Density of rubber belt = 1000 kgm3
Angle of lap for dynamo pulley = 165deg
Coefficient of friction between belt and pulley = 03
Solution
GROUP PROJECT 1
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5051
GROUP PROJECT 1
DESIGN PROJECT 1
Design a belt drive that can transmit 110 kW power for a system consisting of twopulleys of diameter 09 m and 12 m center distance of 36 m belt speed of 20ms coefficient of friction 03 a slip of 12 at each pulley and the belt drive iscapable to carry an overload torque of 866 Nm You can assume the safe stressof the belt is around 15 to 25 MPa You must design the belt system by finding
- Type of belt drive to be use
-Speed for driver and driven pulley
-Required design torque to compensate the extra loading of 866 Nm
-Angle of lap
-Length of belt required
-The sizing of belt (cross sectional area)
-Centrifugal force effect (if exist)
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151
832019 35050627 Belt Drive Chapter 2
httpslidepdfcomreaderfull35050627-belt-drive-chapter-2 5151