Top Banner
9/20/2011 1 AUTOMOBILE ENGINEERING AUTOMOBILE ENGINEERING DYNAMICS OF ROAD VEHICLE -By Dr. S A Channiwala Example 1 : A two wheeler has a mass of 265 kg. It has a wheelbase of 1.24 m & ratio of x/y=1.2. If manufacture claims the vehicle to achieve the acceleration of 3 m/s 2 & height of CG is 0.7 m. Determine: i. Effort required on the rear wheel ii. Reactions R1&R2 iii. Load transfer iv. Time required to achieve a speed of 80 km/hr v. If the tyre of radius is 0.325 m, what is the theoretical power required?
33

Automobile(Mechanics of Road Vehicles)

Apr 18, 2015

Download

Documents

Avinash Kumar
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Automobile(Mechanics of Road Vehicles)

9/20/2011

1

AUTOMOBILE ENGINEERINGAUTOMOBILE ENGINEERING

DYNAMICS OF ROAD VEHICLE

-By Dr. S A Channiwala

Example 1 :

A two wheeler has a mass of 265 kg. It has awheelbase of 1.24 m & ratio of x/y=1.2. Ifmanufacture claims the vehicle to achieve theacceleration of 3 m/s2 & height of CG is 0.7 m.Determine:

i. Effort required on the rear wheel

ii. Reactions R1&R2

iii. Load transfer

iv. Time required to achieve a speed of 80 km/hr

v. If the tyre of radius is 0.325 m, what is the theoretical power required?

Page 2: Automobile(Mechanics of Road Vehicles)

9/20/2011

2

x y

L

mg

CG

H

Fi=ma

a=3 m/s2

A B

R2R1

P

Page 3: Automobile(Mechanics of Road Vehicles)

9/20/2011

3

Page 4: Automobile(Mechanics of Road Vehicles)

9/20/2011

4

VEHICLE MECHANICS

1.1 Laws of Equilibrium : If a body is in

Equilibrium then :-

(a) The resultant of all the forces acting on it is

zero.

And

(b) The resultant of all the couples and the

moments of all the forces taken about

any axis whatsoever is zero.

In the most general case, the laws of

equilibrium will enable us to write down

six equations,

Three by equating to zero the force along

the three axis

Three by taking moment about the

three axis

But the majority of problems do not require

the formulation of all six equation.

Page 5: Automobile(Mechanics of Road Vehicles)

9/20/2011

5

1.2 Weight/Force Distribution in Two wheeler :-

a b

L

R2R1

CGFront Rear

W

x

x

∑ Fy = 0, R1 + R2 = W ....... (i)

Taking moment about x-x,

……………(ii)

……………(iii)

Substituting (iii) in (i),

……………(iv)2*

*[1 ]W b b

R W WL L

= − = −

1 * *R L W b=

1*W b

RL

∴ =

Page 6: Automobile(Mechanics of Road Vehicles)

9/20/2011

6

Example 2 :

A two wheeler has an unladden weight of 100.3 kg and a

wheel base of 1230mm. If the CG is displaced by 575 mm

from rear wheel axis. Determine the load shared by front and

rear wheels.

1* 983.943*0.575

459.971.230

W bR N

L= = =

20.575

*[1 ] 983.943*[1 ] 523.9731.230

bR W N

L= − = − =

Soln. :

W= 100.3 * 9.81 = 983.943 N

L = 1.230 m, b = 0.575 m

we know that:

Example 3 :

During experimental measurement of the height of

CG, the above two wheeler was kept on an inclined

surface at 15 ⁰ and the load distribution at front &

rear wheels was found to be 52.3 kg & 48 kg

respectively. Determine the height of CG of this

vehicle.

The mean tyre radius is 0.225 m. Also state the

limiting value of slope on which the vehicle will

be stable.

Page 7: Automobile(Mechanics of Road Vehicles)

9/20/2011

7

R2

R1

W

θ

θ

Taking moment about ‘A’,

2*cos * *sin * * *cosR L W H W aθ θ θ+ =

2*sin * * *cos *cos *W H W a R Lθ θ θ∴ = −

* s inW θ

2[ * ]* cot

RH a L

Wθ= −

2*cot * *cot

RH a L

Wθ θ= −

48*9.81[0.655 *1.23]* cot15 0.2477

983.943H m∴ = − =

………….. (1)

…………….. (2)

……………….. (3)

Ans.

Dividing by

Page 8: Automobile(Mechanics of Road Vehicles)

9/20/2011

8

Now R2COS θ is a reaction at rear wheel.

When this reaction tends to zero, the

vehicle becomes unstable & may over-

turn about pt. A.

2*cos * * *cos *sin *R L W a W Hθ θ θ= −

2*

*cos *cos * *sinW a W

R HL L

θ θ θ= −

Now Rewriting Equation no. (2)

Thus limiting value of ‘θ’ may be obtained as:

2*

* cos 0 * cos * * sinW a W

R HL L

θ θ θ= = −

( * cos * sin ) 0W

a HL

θ θ= − =

0W

L≠

*cos *sina Hθ θ=

0.655tan 2.644

0.2477L

a

Hθ = = =

lim] 69.28θ = °

[Note: In practice, this is

limited by road adhesion]

Page 9: Automobile(Mechanics of Road Vehicles)

9/20/2011

9

• These equations very clearly signifies two

facts:

(i) For better stability of vehicle, the CG

disposition must as further as possible

from front axle

(ii) CG must be as lower as possible.

Example 4 :

A bike driver takes his bike to weigh bridge

for determination of its correct CG, he

intends to take part in a bike race, when

front wheel alone enters the weigh bridge,

the load indicated is 78 kg when both

wheels are taken to weighbridge, the

indicated load is 170 kg.

Page 10: Automobile(Mechanics of Road Vehicles)

9/20/2011

10

Now he takes out front wheel from the bridge

on level road & raises the rear wheel by 10

cms on weighbridge. The load indicated is 88

kg. If wheel base is 1.208 m & tyre radius is

225 mm.

Determine

(i) CG Position.

(ii) Limiting value of slope on which vehicle

will be stable.

a b

L

W

CG

A B

R2R1

Case : 1

Page 11: Automobile(Mechanics of Road Vehicles)

9/20/2011

11

Data:Case : 1

R1 = 78 kg = 765.18 N

W= 170 kg = 1667.7 N

∑ Fy = 0; W = R1 + R2

R2 = 902.52 NNow taking moments about ‘A’,

R2*L = W*a

2* 902.52*1.2080.6537

1667.7

R La m

W∴ = = =

1.208 0.6537 0.5543b L a m∴ = − = − =

WW

A

B

R2

R1

θ

θ

LCOSθ

x

aCOSθh=0.10 m

Case : 2

Page 12: Automobile(Mechanics of Road Vehicles)

9/20/2011

12

Selecting AB as a moment arm and taking moment

about point ‘A’,

2* *cos *{ *cos ( )*sin }R L W a h rθ θ θ= − −

2* *cos * *cos *( )*sinR L W a W h rθ θ θ= − −

2( ) * co t * * co t

Rh r a L

Wθ θ− = −

Dividing by W*sinθ

2( * ) * cot

RH r a L

Wθ∴ = + −

863.280.225 (0.6537 *1.208) *cot

1667.7θ= + −

4.7585θ∴ =

cot 4.7585 12.0385∴ =

0.566H m∴ =

Now we know that Limiting value of slope,

0.6537tan

0.5666L

a

Hθ ==

tan 1.153Lθ =

49.08Lθ °=

0.100sin 0.08278

1.208

h

Lθ = = =Now

Page 13: Automobile(Mechanics of Road Vehicles)

9/20/2011

13

Weight Distribution in a Weight Distribution in a

ThreeThree--Wheeled VehicleWheeled Vehicle

a b

L

W

CG

A B

R2R3R1

C

C

R3

R2

H

R1

x

x

z

z

y yB=2c

Page 14: Automobile(Mechanics of Road Vehicles)

9/20/2011

14

∑ Fy = 0; W = R1 + R2 + R3 ……………… (i)

Now taking moments about x-x,

R1*L = W*b ……………… (ii)

Now taking moments about y-y,

R3*c = W*x +R2*c

R3 - R2 = ……………… (iii)

Now taking moments about z-z,

R2*L+ R3*L = W*a

R2 + R3 = ……………… (iv) *W a

L

*W x

c

1 2 3R W R R= − −

2 [ ]2

W a xR

l c= −

(iii) + (iv)

…………………. (v)

(iv) - (iii)

………………… (vi)

……………… (vii)

3 [ ]2

W x aR

c l= −

Page 15: Automobile(Mechanics of Road Vehicles)

9/20/2011

15

Example 5:

A three-wheeler has a wheelbase of

1524 mm and its CG is 900 mm behind

front wheel axle and 160 mm from the

longitudinal axis of vehicle on near

side. The track of rear wheel is 870

mm. Determine the wheel loads, if

total weight of the vehicle is 411 kg.

Sol.Given Data:

L=1.524 m

a=0.900 m

X=0.160 m, c= = 0.435 m

W=411 x9.81=4031.91 N

we know that,

0.870

2

22

[ ]W a x

Rl c

= −

24031.91 0.900 0.160

[ ] 449.024 45.7722 1.524 0.435

R N kg= − = =

Page 16: Automobile(Mechanics of Road Vehicles)

9/20/2011

16

32

[ ]W x a

Rc l

= −

4031.91 0.160 0.900[ ]

2 0.435 1.524= +

1932.025 196.944N kg= =

1 2 3R W R R= − −

4031.91 449.024 1932.025

1650.86 168.28N kg

= − −

= =

Example 6:

• It is required to determine the CG of a threewheeler experimentally when one of the nearsiderear wheel is taken to weigh bridge, the loadrecorded is 160 kg while when opposite rearwheel is taken to weigh bridge the load is foundto be 80 kg. When both the rear wheels weretaken on weighbridge and raised by 110mm theload recorded was 235 kg.

Determine (i) CG position

(ii) limiting slope for stability.

The wheelbase and rear wheel track for this vehicleare 1.6m and 1m respectively while total weightof the vehicle is 425kg. The wheel diameter is 250mm.

Page 17: Automobile(Mechanics of Road Vehicles)

9/20/2011

17

Solution:

• Given data:

= 160 kg = 1569.6 N

D = 0.250 m

W = 425 kg

L = 1.6 m

C =1/2 = 0.5 m

Raised condition: [R2 + R3]=235 kg=2305.35 N

3R

• For a three wheeler we know that :

22

[ ]W a x

Rl c

= −

4169.25784.8 [ ]

2 1.6 0.5

a x= −

4169.251569.6 [ ]

2 1.6 0.5

a x= +

32

[ ]W a x

Rl c

= +

784.8 = 1302.891*a – 4169.25*x …………. (1)

And

1569.6=1302.891*a + 4169.25*x …………. (3)

Page 18: Automobile(Mechanics of Road Vehicles)

9/20/2011

18

Adding (1) + (3)

2354.4 = 2605.782*a

a=0.9035 m

b= L-a = 1.6 - 0.9035 = 0.6965 m

(3) - (1)

784.8 = 8338.5 * x

x=0.0941 m

WW

A

B

R2,3

R1

θ

θx

h

h

r

Page 19: Automobile(Mechanics of Road Vehicles)

9/20/2011

19

Selecting A-B as moment arm & taking moments

about ‘A’,

2, 3* *cos *{ *cos ( )*sin }R L W a H rθ θ θ= − −

* *cos *( )*sinW a W H rθ θ= − −

Dividing by sinW θ

2, 3( ) *cot * * cot

RH r a L

Wθ θ− = −

2, 3[ * ]* cot

RH r a L

Wθ∴ = + −

Now0.11

sin 0.068751.6

h

Lθ = = =

3.942θ∴ =

2305.350.125 [0.9035 *1.6]*14.511

4169.25H∴ = + −

0.3977H m∴ =

0.9035tan 2.272

0.3977

a

Hθ∴ = = =

66.24Lθ∴ = °

Page 20: Automobile(Mechanics of Road Vehicles)

9/20/2011

20

Weight Distribution in a Four-wheeled

Vehicle:

LL

aa bb

CGCG

WW

R3,4R1,2

R2

R1 R3

R4

B c

d

x

B

dd cc

R1,3 R2,4

y = B/2 -x

H

y B/2 +

x WW

• Data Given:

W=1000 kg

L=2.3 m

B=1.3 m

a=1.3 m

b=1.0 m

x= 0.1 m

c=0.75 m

d=0.55 m

Page 21: Automobile(Mechanics of Road Vehicles)

9/20/2011

21

Taking moment about ‘A’,

3 4( ) * *R R L W a+ =

1 3( )* *R R B W c+ =

2 4( )* *R R B W d+ =

Taking moment about ‘C’,

Taking moment about ‘D’,

1 2( )* *R R L W b+ =

Taking moment about ‘B’,

3 4( ) *a

R R WL

+ =

1 2( ) *b

R R WL

+ =

2 4( ) *d

R R WB

+ =

1 3( ) *c

R R WB

+ =

From (i) to (iv),

Page 22: Automobile(Mechanics of Road Vehicles)

9/20/2011

22

From method of Superimposition:

• From (vi) to (viii)

• From (vi) to (vii)

• From (v) to (vii)

• From (vi) to (vii)

1 * *b c

R WL B

=

2 * *b d

R WL B

=

3 * *a c

R WL B

=

4 * *a d

R WL B

=

1 2460.7R N=

4 2345.8R N=

2 1804.5R N=

3 3198.9R N=

Page 23: Automobile(Mechanics of Road Vehicles)

9/20/2011

23

Example:2

A four wheeled vehicle has a wheel base of 2.36

m and mean track of 1.32 m. It is designed in

such a manner that front axle shares 48% of

vehicle load. The CG of this vehicle is displaced

by 0.075 m from longitudinal axis away from

driver side. Determine load distribution if

vehicle load is 790 kg under unladden

condition.

[Fiet-UNO]

L

a b

CG

W

R3,4R1,2

R2

R1 R3

R4

B = 1.32mC = 0.735m

d = 0.585m0.075m

B

d cR1,3 R2,4

Page 24: Automobile(Mechanics of Road Vehicles)

9/20/2011

24

• Given data:

L=2.36 m

B=1.32 m

W=790 kg = 7749.9 N

c = 0.735

1 2( ) 0.48* 3719.952R R W N+ = =

2

By= +

0.5852

Bd y m= − =

3 4 1 2( ) ( ) 4029.948R R W R R N+ = − + =

Taking moment about ‘A’,

3 4( ) * *R R L W a+ =

3 4( )* 4029.948*2.361.2272

7749.9

R R La m

W

+∴ = = =

2.36 1.2272 1.1328b L a m= − = − =

Page 25: Automobile(Mechanics of Road Vehicles)

9/20/2011

25

Now we know that:

1 * *b c

R WL B

=

1.1328 0.7357749.9* *

2.36 1.32=

2071.337 211.145N kgf= =

2 * *b d

R WL B

=

1.1328 0.5857749.9* *

2.36 1.32=

1648.615N=

168.055kgf=

Page 26: Automobile(Mechanics of Road Vehicles)

9/20/2011

26

3 * *a c

R WL B

=

1.2272 0.7357749.9* *

2.36 1.32=

2243.948N=

228.741kgf=

4 * *a d

R WL B

=

1.2272 0.5857749.9* *

2.36 1.32=

1785.9997 N=

182.059kgf=

Page 27: Automobile(Mechanics of Road Vehicles)

9/20/2011

27

1st check: W=∑R =790 kgf

2nd check:

3rd check:

------------------------------------------------------------

3 4 *a

R R WL

+ =

410.8 410.8=

2 4( ) *d

R R WB

+ =

350.114 350.114=

Example 3:• A four wheeled vehicle stands on a weighbridge

such that only front wheels are on the bridge.

The load recorded is 614 kgf. The vehicle is now

taken on weighbridge & the load was found to

be 1180 kg. The vehicle then was kept on a

weighbridge in such a way that its rear wheels

were on the weighbridge raised by 10 cms.

Page 28: Automobile(Mechanics of Road Vehicles)

9/20/2011

28

R2

R1

W

θ

θ

Case : 2

3 4

1 2

1

2

3

4

2 4

1 3

3 4

1 2

2 4

1 3

1 2 3

( )* *

( )* *

2460.7

1804.5

3198.9

2345.8

( )* *

( )* *

( ) *

( ) *

( ) *

( ) *

R W R R

R R L W a

R R L W b

R N

R N

R N

R N

R R B W d

R R B W c

aR R W

L

bR R W

L

dR R W

B

cR R W

B

= − −

+ =

+ =

=

=

=

=

+ =

+ =

+ =

+ =

+ =

+ =

Page 29: Automobile(Mechanics of Road Vehicles)

9/20/2011

29

cot 14.511

0.9035tan 2.272

0.3977

66.24L

a

H

θ

θ

θ

=

∴ = = =

= °

x y

L

mg

CG

H

Fi=ma

a=3 m/s2

A B

R2R1

P

Page 30: Automobile(Mechanics of Road Vehicles)

9/20/2011

30

x y

L

mg

CG

H

Fi=ma

a b

L

R2R1

CGFront Rear

W

Page 31: Automobile(Mechanics of Road Vehicles)

9/20/2011

31

R2

R1

W

θ

θ

a b

L

W

CG

A B

R2R1

Page 32: Automobile(Mechanics of Road Vehicles)

9/20/2011

32

WW

A

B

R2

R1

θ

θ

LCOSθ

x

aCOSθh=0.10 m

R2

R1

W

θ

θ

Page 33: Automobile(Mechanics of Road Vehicles)

9/20/2011

33

a b

L

W

CG

A B

R2R3R1

C

C

R3

R2

H

R1

x

x

z

z

y yB=2c

8 6 3 .2 80 .2 2 5 ( 0 .6 5 3 7 * 1 .2 0 8 ) * c o t

1 6 6 7 .7

0 .1 0 0s i n 0 .0 8 2 7 8

1 .2 0 8

4 .7 5 8 5

c o t 4 .7 5 8 5 1 2 .0 3 8 5

0 .5 6 6

2( * ) * c o t

h

L

H m

RH r a L

W

θ

θ

θ

θ

= + −

= = =

∴ =

∴ =

∴ =

∴ = + −