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Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy

Chapter 7 Work and Kinetic Energy

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Chapter 7 Work and Kinetic Energy. Reading and Review. Force and Work. a) one force b) two forces c) three forces d) four forces e) no forces are doing work. A box is being pulled up a rough incline by a rope connected to a pulley. How many forces are doing work on the box?. - PowerPoint PPT Presentation

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Page 1: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Chapter 7

Work and Kinetic Energy

Page 2: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Reading and Review

Page 3: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Force and Work

a) one force

b) two forces

c) three forces

d) four forces

e) no forces are doing work

A box is being pulled up a rough

incline by a rope connected to a

pulley. How many forces are

doing work on the box?

Page 4: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Force and Work

N

f

T

mg

displacementAny force not perpendicular

to the motion will do work:

N does no work

T does positive work

f does negative work

mg does negative work

a) one force

b) two forces

c) three forces

d) four forces

e) no forces are doing work

A box is being pulled up a rough

incline by a rope connected to a

pulley. How many forces are

doing work on the box?

Page 5: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Free Fall I

a) quarter as much

b) half as much

c) the same

d) twice as much

e) four times as much

Two stones, one twice the

mass of the other, are dropped

from a cliff. Just before hitting

the ground, what is the kinetic

energy of the heavy stone

compared to the light one?

Page 6: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Consider the work done by gravity to make the stone

fall distance d:

KE = Wnet = F d cos

KE = mg d

Thus, the stone with the greater mass has the greater

KE, which is twice as big for the heavy stone.

Free Fall I

a) quarter as much

b) half as much

c) the same

d) twice as much

e) four times as much

Two stones, one twice the

mass of the other, are dropped

from a cliff. Just before hitting

the ground, what is the kinetic

energy of the heavy stone

compared to the light one?

Follow-up: How do the initial values of gravitational PE compare?

Page 7: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

In the previous question, just

before hitting the ground, what is

the final speed of the heavy stone

compared to the light one?

a) quarter as much

b) half as much

c) the same

d) twice as much

e) four times as much

Free Fall II

Page 8: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

In the previous question, just

before hitting the ground, what is

the final speed of the heavy stone

compared to the light one?

a) quarter as much

b) half as much

c) the same

d) twice as much

e) four times as much

All freely falling objects fall at the same rate, which is g.

Because the acceleration is the same for both, and the

distance is the same, then the final speeds will be the same for

both stones.

Free Fall II

Page 9: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Work Done by a Variable Force

The force needed to stretch a spring an amount x is F = kx.

Therefore, the work done in stretching the spring is

Page 10: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Application: work by a spring

Hooke’s Law: F = - kx k = (3kg)(9.8 m/s2) / (3.9 cm)k = 760 N/m

Loaded spring: W = kx2/2 = (760 N/m) (0.04m)2/ 2

W = 0.61 J

How fast?: v = d/t = (0.020 m) (0.020 s) = 1 m/s

KE = mv2/2 = (1kg)(1m/s)2 / 2KE = 0.55 J

Kinetic Energy:

Page 11: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Power

Power is a measure of the rate at which work is done:

SI unit: J/s = watt, W

1 horsepower = 1 hp = 746 W

ave

WP

t

Page 12: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Power

Page 13: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Power

If an object is moving at a constant speed in the face of friction, gravity, air resistance, and so forth, the power exerted by the driving force can be written:

Question: what is the total work per unit time done on the object?

F x xP F Fv

t t

Page 14: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

a) energy

b) power

c) current

d) voltage

e) none of the above

Electric Bill

When you pay the electric

company by the kilowatt-hour,

what are you actually paying for?

Page 15: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

We have defined: Power = energy /

time

So we see that: Energy = power ×

time

This means that the unit of power ×

time (watt-hour) is a unit of energy !!

Electric Bill

When you pay the electric

company by the kilowatt-hour,

what are you actually paying for?

a) energy

b) power

c) current

d) voltage

e) none of the above

Page 16: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

A block rests on a horizontal frictionless surface. A string is attached to the block, and is pulled with a force of 45.0 N at an angle above the horizontal, as shown in the figure. After the block is pulled through a distance of 1.50 m, its speed is 2.60 m/s, and 50.0 J of work has been done on it. (a) What is the angle (b) What is the mass of the block?

Page 17: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Page 18: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

The pulley system shown is used to lift a 52 kg crate. Note that one chain connects the upper pulley to the ceiling and a second chain connects the lower pulley to the crate. Assuming the masses of the chains, pulleys, and ropes are negligible, determine (a) the force F required to lift the crate with constant speed, and(b) the tension in two chains

Page 19: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

(a) the force F required to lift the crate with constant speed, and(b) the tension in two chains

(a) constant velocity, a=0, so net force =0.

2T - (52kg)(9.8m/s2) = 0

T = 250 NF = -250 Ny

(b) upper pulley doesn’t move:Tch - 2Trope = 0 Tch = 500 N

lower pulley has constant accelerationTch -2Trope =0 Tch = 500 N

Mechanical Advantage!

Page 20: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

(a) how much power is applied to the box by the chain?(b) how much power is applied on the rope by the applied force?

What about work?

Trope = 250 NTchain = 500 NF = -250 Ny

(a) P = Fv = 500 N * vbox

(b)P = Fv = 250 N * vhand

hand moves twice as fast

hand moves twice as far

Page 21: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Chapter 8

Potential Energy and Conservation of Energy

Page 22: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Units of Chapter 8

• Conservative and Nonconservative Forces

• Potential Energy and the Work Done by Conservative Forces

• Conservation of Mechanical Energy

• Work Done by Nonconservative Forces

• Potential Energy Curves and Equipotentials

Page 23: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-1 Conservative and Nonconservative Forces

Conservative force: the work it does is stored in the form of energy that can be released at a later time

Example of a conservative force: gravity

Example of a nonconservative force: friction

Also: the work done by a conservative force moving an object around a closed path is zero; this is not true for a nonconservative force

Page 24: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-1 Conservative and Nonconservative Forces

Work done by gravity on a closed path is zero:

Page 25: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-1 Conservative and Nonconservative Forces

Work done by friction on a closed path is not zero:

Page 26: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-1 Conservative and Nonconservative Forces

The work done by a conservative force is zero on any closed path:

Page 27: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-2 The Work Done by Conservative Forces

If we pick up a ball and put it on the shelf, we have done work on the ball. We can get that energy back if the ball falls back off the shelf; in the meantime, we say the energy is stored as potential energy.

(8-1)

Page 28: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-2 The Work Done by Conservative Forces

Gravitational potential energy:

Page 29: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Is it possible for the

gravitational potential

energy of an object to

be negative?

a) yes

b) no

Sign of the Energy II

Page 30: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Is it possible for the

gravitational potential

energy of an object to

be negative?

a) yes

b) no

Gravitational PE is mgh, where height h is measured relative to

some arbitrary reference level where PE = 0. For example, a

book on a table has positive PE if the zero reference level is

chosen to be the floor. However, if the ceiling is the zero level,

then the book has negative PE on the table. Only differences (or

changes) in PE have any physical meaning.

Sign of the Energy II

Page 31: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?

a) only B

b) only C

c) A, B, and C

d) only A and C

e) only B and C

Question 8.2 KE and PE

A) skier’s PE B) skier’s change in PE C) skier’s final KE

Page 32: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?

a) only B

b) only C

c) A, B, and C

d) only A and C

e) only B and C

The gravitational PE depends upon the reference level, but

the difference PE does not! The work done by gravity

must be the same in the two solutions, so PE and KE

should be the same.

Question 8.2 KE and PE

A) skier’s PE B) skier’s change in PE C) skier’s final KE

Follow-up: Does anything change physically by the choice of y = 0?

Page 33: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-2 The Work Done by Conservative Forces

Springs: (8-4)

Page 34: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-3 Conservation of Mechanical Energy

Definition of mechanical energy:

(8-6)

Using this definition and considering only conservative forces, we find:

Or equivalently:

Page 35: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-3 Conservation of Mechanical Energy

Energy conservation can make kinematics problems much easier to solve:

Page 36: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Example: A mass m slides down a 2 m long smooth ramp which makes an angle of 30o with the top of a table which is 1 m above the floor. The end of the ramp is at the edge of the table. At what horizontal distance from the edge of the table does the mass hit the floor?

Page 37: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?

a) only B

b) only C

c) A, B, and C

d) only A and C

e) only B and C

KE and PE

A) skier’s PE B) skier’s change in PE C) skier’s final KE

Page 38: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

You and your friend both solve a problem involving a skier going down a slope, starting from rest. The two of you have chosen different levels for y = 0 in this problem. Which of the following quantities will you and your friend agree on?

a) only B

b) only C

c) A, B, and C

d) only A and C

e) only B and C

The gravitational PE depends upon the reference level, but

the difference PE does not! The work done by gravity

must be the same in the two solutions, so PE and KE

should be the same.

KE and PE

A) skier’s PE B) skier’s change in PE C) skier’s final KE

Follow-up: Does anything change physically by the choice of y = 0?

Page 39: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Example: Two water slides are shaped differently, but start at the same height h and are of equal length. Two rides, Paul and Kathy, start from rest at the same time on different slides.a)Which is travelling faster at the bottom?b)Which makes it to the bottom first?

Page 40: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-4 Work Done by Nonconservative Forces

In the presence of nonconservative forces, the total mechanical energy is not conserved:

Solving,

(8-9)

Page 41: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-4 Work Done by Nonconservative Forces

In this example, the nonconservative force is water resistance:

Page 42: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-5 Potential Energy Curves and Equipotentials

The curve of a hill or a roller coaster is itself essentially a plot of the gravitational potential energy:

Page 43: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-5 Potential Energy Curves and Equipotentials

The potential energy curve for a spring:

Page 44: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

8-5 Potential Energy Curves and Equipotentials

Contour maps are also a form of potential energy curve:

Page 45: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Summary of Chapter 8

• Conservative forces conserve mechanical energy

• Nonconservative forces convert mechanical energy into other forms

• Conservative force does zero work on any closed path

• Work done by a conservative force is independent of path

• Conservative forces: gravity, spring

Page 46: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Summary of Chapter 8

• Work done by nonconservative force on closed path is not zero, and depends on the path

• Nonconservative forces: friction, air resistance, tension

• Energy in the form of potential energy can be converted to kinetic or other forms

• Work done by a conservative force is the negative of the change in the potential energy

• Gravity: U = mgy

• Spring: U = ½ kx2

Page 47: Chapter 7 Work and Kinetic Energy

Copyright © 2010 Pearson Education, Inc.

Summary of Chapter 8

• Mechanical energy is the sum of the kinetic and potential energies; it is conserved only in systems with purely conservative forces

• Nonconservative forces change a system’s mechanical energy

• Work done by nonconservative forces equals change in a system’s mechanical energy

• Potential energy curve: U vs. position