Lecture 16 1/23 Physics 111 Lecture 16 (Walker: 7.3-4) Work & Power March 6, 2009 Lecture 16 2/23 Energy • Forms of energy: – Mechanical • Kinetic, Potential; focus for now – Thermal – Chemical – Electromagnetic – Nuclear • Energy can be transformed from one form to another – Essential to the study of physics, chemistry, biology, geology, astronomy • Can be used in place of Newton’s laws to solve certain problems more simply • Energy units: SI Unit - Joule (J); Calorie (food calorie) = 4.2 kJ; Kilowatt-hour = 3.6 MJ
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Lecture 16 1/23
Physics 111Lecture 16 (Walker: 7.3-4)
Work & PowerMarch 6, 2009
Lecture 16 2/23
Energy• Forms of energy:
– Mechanical• Kinetic, Potential; focus for now
– Thermal– Chemical– Electromagnetic– Nuclear
• Energy can be transformed from one form to another– Essential to the study of physics, chemistry,
biology, geology, astronomy• Can be used in place of Newton’s laws to solve certain
problems more simply• Energy units: SI Unit - Joule (J); Calorie (food
calorie) = 4.2 kJ; Kilowatt-hour = 3.6 MJ
Lecture 16 3/23
Kinetic Energy &The Work-Energy Theorem
Work-Energy Theorem: The total work done on an object is equal to its change in kinetic energy.
(7-7)
Lecture 16 4/23
Work and Kinetic Energy• An object’s kinetic
energy can also be thought of as the amount of work the moving object could do in coming to rest– The moving hammer
has kinetic energy and can do work on the nail
Lecture 16 5/23
Example: Work & KE-Rocket Launch150,000 kg rocket launched straight up. Rocket engine generates thrust of 4.0 x 106 N. Rocket’s speed at height 500 m? (Ignore air resistance and mass loss due to burned fuel.)
Lecture 16 6/23
6 9thrust thrust ( ) (4.0 10 N)(500 m) 2.0 10 JW F y= ∆ = × = ×
4 2grav ( ) ( ) (1.5 10 kg)(9.80 m/s )(500 m)W w y mg y= − ∆ = − ∆ = − × =
1 2 9thrust grav2 0 1.26 10 JK mv W W∆ = − = + = ×
2 1.30 m/sKvm∆
= =
= - 0.74 x 109 J
Lecture 16 7/23
Graphical Interpretation of WorkIf the force is constant, we can interpret
the work done graphically:
Lecture 16 8/23
Work Done by a Variable ForceIf the force takes on several successive
constant values, we can add the areas of each of the “blocks”:
Lecture 16 9/23
Work Done by a Variable ForceWe can then approximate a continuously
varying force by a succession of constant values.
Lecture 16 10/23
Example:Work Done by a Varying Force
A force varies with x as shown. Find work done byforce on a particle that moves from x = 0.0 m to x = 6.0 m.
ˆxF F x=r
totalW A=
1total 1 2 2(5.0 N)(4.0 m) (5.0 N)(2.0 m)
20.0 J 5.0 J 25.0 JW A A A= = + = +
= + =
Lecture 16 11/23
Work and SpringsThe force needed to stretch a spring an
amount x is F = kx.Therefore, the work done in stretching the spring is
(7-8)
Lecture 16 12/23
Spring Work by Average Force
1 22 fW k x=
Force needed to stretch spring distance x: F = kx
Average force during stretch from x = 0 to x = xf: ½kxf
Work done during stretch:
W = FAvg ∆x cosθ = (½kxf)xf = ½kxf2
Lecture 16 13/23
Question
A spring-loaded gun shoots a plastic ball with a speed of 4.0 m/s. If the spring is compressed twice as far, what is the ball’s speed?
a) 2.0 m/s b) 4.0 m/s c) 8.0 m/s d) 16.0 m/s e) 32.0 m/s
4.0 m/s
Lecture 16 14/23
Example: Work Done on Block by Spring4.0 kg block on frictionless surface is attached to horizontal spring with k = 400 N/m. Spring is initially compressed to 5.0 cm. (a) Find work done on block by the spring as block moves from x = x1 = -5.0 cm to its equilibrium position of x = x2 = 0 cm. (b) Find the speed of the block at x2 = 0 cm.
kg block. The other end is pulled by a motorized toy train that moves forward at 5.0 cm/s. Spring constant is k=50 N/m and the coefficient of static friction between the block and the surface is µs=0.6. Spring is in equilibrium at t=0 s when the train starts to move.
At what time does the block start to slip?
Lecture 16 17/23
net( ) ( ) ( ) 0x sp x s x sp sF F f F f= + = − =∑s s spf mg F k xµ= = = ∆
2(0.60)(2.0 kg)(9/80 m/s )(50 N/m)
0.235 m 23.5 cm
smgxk
µ∆ = =
= =
(23.5 cm) 4.7 s(5.0 cm/s)
xtv∆
= = =
Lecture 16 18/23
Power (P)Power is a measure of the rate at which work
is done. If work W done during time t:
(7-10)
SI power unit: 1 J/s = 1 watt = 1 W
Also: 1 horsepower = 1 hp = 746 W
Lecture 16 19/23
Power*If an object is moving at a constant speed in
the presence of friction, gravity, air resistance, and so forth, the power exerted by the driving force can be written:
(7-13)
Lecture 16 20/23
Human Basal Metabolism 80W
Lecture 16 21/23
Example: Power of a MotorA small motor operates a lift that raises a load of bricks weighing 500 N to height of 10 m in 20 s at constant speed. Lift weighs 300 N.
What is the power output of the motor?
W = F d cosθ = (800N)(10m) = 8000J
P = W/t = 8000J / 20s = 400 W
(400 W = 0.54 hp)
Lecture 16 22/23
Before Monday, read Walker 8.1-2
Homework Assignments #7b should be submitted using WebAssign by 11:00 PM on Monday, March 9.