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Chapter 7 Work and Energy

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Page 1: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Chapter 7

Work and Energy

Page 2: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

2

Energy

Momentum

Integration over space

Integration over time

Scalar

Vector

Significance: They are conserved

Valuable when the forces are not detailed

Wide range including Relativity & Quantum M.

Energy is useful in all areas of physics and in other science as well

Alternative description of dynamics

Page 3: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work done by constant force

3

Work done by a constant force

cosW Fd or W F d

Accomplished by action of force over a distance

F

d

When W = 0?

Example1: An object moves as ,

and there is a force acting on it,

what is the work done by this force in 0~2s?

22r ti t j

5 6F i k

4 4r i j

20W F r J

F d

Page 4: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work done by varying force

4

Divide the path into short intervals

Total worki iW F l

Sum → Integral0il

b

aW F dl

During each interval, force ~ constant

i iW F l

Work

General definition of work

F

F

a

b

Page 5: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work in component form

5

b

aL

W F dl F dl

This is called a line integral.

, x y zF F i F j F k dl dxi dyj dzk

Work can be written asb b b

x y za a aW F dx F dy F dz

Or:tan, dl dl F dl F dl

tan

b

aW F dl

F

F

a

b

dl

Page 6: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work depends on path

6

tan

b b

a aW F dl F dl

Work depends on the specific path from a to b

a b

1

2

3

Moves on horizontal ground,

3 different paths from a to b, work by friction is different!

b

aW Ndl N S

Friction is called a nonconservative force

Page 7: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work done by gravity

7

Work done by gravity is path independent.

Determined only by the initial and final position.

Gravity is called a conservative force.

All constant forces are conservative.

ha

hb

La

b

mg

o

y

x

C

G mg

b

yaW F dy

mg h

b

a

h

h mgdy

Gravity of object:

Page 8: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Lose weight by climbing

8

Example2: Bob (80kg) wants to lose weight by climbing mountains. How many calories he loses at least when he goes from A to B? ( 1cal=4.184J )

A

B

h=1500m

Solution: The work done by gravity is

W mgh 680 9.8 1500 1.18 10 J

5or 2.81 10 281cal kcal

So Bob loses energy 61.18 10 J

That is about 31g fat.

Page 9: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Stretching a spring

9

Example3: Someone slowly pulls a spring from unstretched to make the object m leave the ground, calculate the work done by this person.

m

F

k

Solution: force to stretch a spring:

0 0

x xW Fdx kxdx

F = k x

21

2kx

How to make m leave the ground?

F mg /x mg k

Work :2

21 ( )

2 2

mgW kx

k

Page 10: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Kinetic Energy

10

Energy: one of most important concepts in science.

There are many types of energy, it can be usually

regarded as “the ability to do work”.

Moving objects can do work → have energy

The energy of motion is called kinetic energy

21

2kE mv

Object starts from rest under constant net force:

net netW F d mad

Translational kinetic energy

221

2 2

vma mv

a

Page 11: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work-energy principle

11

Work-energy principle

tan

b

aF dl

For varying force, 3 dimensional motion:b

net netaW F dl

tan

dvF m

dt

b

a

dvm dl

dt

b

a

dlm dv

dt

b

amvdv

2 21 1

2 2b a kmv mv E

The net work done on an object is equal to

the change in its kinetic energy.

Page 12: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work in an elliptical motion

12

Example4: A particle m moves under the equation , where a, b, are positive constants. Determine the net work during t=0~/2.

cos sinr a ti b tj

Solution1: The net force is

2

2 22

d rF m m r m xi yj

dt

1 1

0 0

x y

x yx yW F dx F dy

2 2 2 21 1

2 2m a m b

Net work

0 2 2

0

b

am xdx m ydy

Page 13: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

13

Example4: A particle m moves under the equation , where a, b, are positive constants. Determine the net work during t=0~/2.

cos sinr a ti b tj

Solution2: Using work-energy principle

sin cosdr

v a ti b tjdt

t=0: v0= b;

Net work equals to the change of kinetic energy:

2 2 2 2 2 20

1 1 1 1

2 2 2 2W mv mv m a m b

t=/2: v = a

Page 14: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Work done by friction

14

Example5: An object moves along a semi-circular wall on smooth horizontal plane. Known: v0 and µ, determine the work done by friction from A to B.

v

o

v0

.N

R

B

Solution:

2

v dv

R dt

2vN m

RRadial forcedv

N mdt

Tangential force

dv d v dv

d dt R d

dv

dv

0v v e 2 2

0

1 1

2 2W mv mv 2 2

0

1( 1)

2mv e

Page 15: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

Kinetic energy of spring

15

Example6: Considering the mass of spring ms (k, L),

it is attached by a mass M, determine kinetic energy of the spring when M is moving with velocity v.

x dx

M

Solution: take dx of the spring, the mass is ms·dx/L

If the spring deforms uniformly, then vdx = v·x/L2 2

23

1 1

2 2k s s

dx x xdE m v m v dx

L L L

2

0

1

2 3

Ls

k k

mE dE v

Effective mass

Page 16: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

*Forms of energy

There are 5 main forms of energy

Mechanical

Thermal / heat

Electromagnetic

Chemical

Nuclear

(Fission & Fusion)

Chain reaction

Page 17: Chapter 7 Work and Energy. 2 Energy Momentum Integration over space Integration over time Scalar Vector Significance: They are conserved Valuable when

*Nuclear bomb

“Little boy” & “Fat man”

The effects of nuclear bomb:

Heat, shock wave and radiation (γ ray and neutrons)

“If the radiance of a thousand suns were to burst into the sky, that would be like the

splendor of the Mighty One.”