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Page 1: 1© Manhattan Press (H.K.) Ltd. Work Energy Energy 3.6 Work, energy and power Power Power

© Manhattan Press (H.K.) Ltd. 1

• WorkWork

• • EnergyEnergy

3.6 Work, energy and 3.6 Work, energy and powerpower

• • PowerPower

Page 2: 1© Manhattan Press (H.K.) Ltd. Work Energy Energy 3.6 Work, energy and power Power Power

© Manhattan Press (H.K.) Ltd. 2

Work

3.6 Work, energy and power (SB p. 125)

Work is done when you lift a load

More work is done

- lift heavier load

- lift load higher

work involves:

- force

- movement caused by force

Go to

More to Know 3More to Know 3

Page 3: 1© Manhattan Press (H.K.) Ltd. Work Energy Energy 3.6 Work, energy and power Power Power

© Manhattan Press (H.K.) Ltd. 3

Work

3.6 Work, energy and power (SB p. 125)

sFW )(Work

W = Fs cos

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© Manhattan Press (H.K.) Ltd. 4

Work

3.6 Work, energy and power (SB p. 125)

1. F and s in same direction ( = 0)

W = Fs

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© Manhattan Press (H.K.) Ltd. 5

Work

3.6 Work, energy and power (SB p. 126)

2. F and s in perpendicular ( = 90o)

W = 0

Unit – joule (J)1 J = 1 N m

scalar

Go to

More to Know 4More to Know 4

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© Manhattan Press (H.K.) Ltd. 6

Work

3.6 Work, energy and power (SB p. 126)

Work done by a variable force

= Area under force-displacement graph

xFdsW 0

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© Manhattan Press (H.K.) Ltd. 7

Work

3.6 Work, energy and power (SB p. 126)

e.g.

= Area of triangle under the graph

=

eFdsW 0

Fe21

W = Fe21

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© Manhattan Press (H.K.) Ltd. 8

Energy

3.6 Work, energy and power (SB p. 127)

Energy

- ability to do work

Mechanical energy

- energy due to motion, position, physical condition

- kinetic energy or potential energy

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© Manhattan Press (H.K.) Ltd. 9

Energy

3.6 Work, energy and power (SB p. 127)

Kinetic energy

The kinetic energy (K or KE) is the energy of a body due to its motion.

W = FsF = ma

v2 = u2 + 2asW = mv2/2

Work done by F is changed to KE of body

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© Manhattan Press (H.K.) Ltd. 10

Energy

3.6 Work, energy and power (SB p. 128)

Kinetic energy

Kinetic energy of the body (K) = mv2/2

W = Fs

= (ma)s

= mv2/2 – mu2/2

= Increase in kinetic energy

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© Manhattan Press (H.K.) Ltd. 11

Energy

3.6 Work, energy and power (SB p. 128)

Potential energy

An object stores energy due to its physical condition or of its position. The energy stored in the object is called potential energy (U or PE).

E.g.- stretched spring or rubber band- lifting object against earth’s gravity

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© Manhattan Press (H.K.) Ltd. 12

Energy

3.6 Work, energy and power (SB p. 128)

Potential energy

Gain in gravitational potential energy= Work done against gravitational force

= Fh

Potential energy (U) = mgh

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© Manhattan Press (H.K.) Ltd. 13

Energy

3.6 Work, energy and power (SB p. 128)

Potential energy

Energy stored in stretched spring

= kx2/2k – force constant of spring, x - extension

Obey Hooke’s Law

Elastic potential energy

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© Manhattan Press (H.K.) Ltd. 14

Energy

3.6 Work, energy and power (SB p. 129)

Principle of Conservation of Energy

Kinetic energy (K) + Potential energy (U)

= Total energy (E)

K = -U

constant

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© Manhattan Press (H.K.) Ltd. 15

Energy

3.6 Work, energy and power (SB p. 129)

Principle of Conservation of Energy

E.g.

K = mv2/2K = mv2/2 - 0 and v2 = u2 +2asK = mgh = Loss in gravitational potential energy

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© Manhattan Press (H.K.) Ltd. 16

Energy

3.6 Work, energy and power (SB p. 129)

Principle of Conservation of Energy

E.g.

Gravitational force acting on man (F) = mgWork done by F (W) = Fh = mgh = K

Work done by gravitational force is converted into gain in kinetic energy

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© Manhattan Press (H.K.) Ltd. 17

Energy

3.6 Work, energy and power (SB p. 130)

Relationship between force and potential energy E = K + U K = -U

W = F(s) = -U

Force (F) = dsdU

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© Manhattan Press (H.K.) Ltd. 18

Energy

3.6 Work, energy and power (SB p. 130)

Relationship between force and potential energy E.g.

U = mgs

mgmgsdsd

dsdUF )(

F is –ve (it is in –ve direction)Go to

Example 6Example 6

Go to

Example 7Example 7

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© Manhattan Press (H.K.) Ltd. 19

Power

3.6 Work, energy and power (SB p. 133)

Power

- rate at which work is done

- rate at which energy is delivered

Average power = interval TimedoneWork

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© Manhattan Press (H.K.) Ltd. 20

Power

3.6 Work, energy and power (SB p. 133)

F and s in same direction

Power

tFs

interval Time

doneWork

Power = Fv

F and s at

Power = Fv cos

Unit – watt (W)

Go to

Example 8Example 8

Go to

Example 9Example 9

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© Manhattan Press (H.K.) Ltd. 21

Power

3.6 Work, energy and power (SB p. 135)

Efficiency

- percentage of useful work done compared to the input energy

%100machine by the usedEnergy

machine by the done work UsefulEfficiency

Efficiency < 100%

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© Manhattan Press (H.K.) Ltd. 22

3.6 Work, energy and power (SB p. 137)

3.1 Newton’s Laws of Motion3.1 Newton’s Laws of Motion

1. Newton’s First Law of Motion states that an object will remain at rest or move along a straight line with constant speed, unless it is acted upon by a force.

2. Momentum = Mass ×Velocity

3. Newton’s Second Law of Motion states that the rate of change of momentum of an object is directly proportional to the net force acted on it, and the motion occurs along the direction of the force.

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3.6 Work, energy and power (SB p. 137)

3.1 Newton’s Laws of Motion3.1 Newton’s Laws of Motion

4. Newton’s Third Law of Motion states that when two bodies interact, they exert equal but opposite forces on each other. They are called action and reaction.

5. Action and reaction are equal in magnitude but opposite in direction. They act on different objects.

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© Manhattan Press (H.K.) Ltd. 24

3.6 Work, energy and power (SB p. 137)

3.2 Principle of Conservation of Linear 3.2 Principle of Conservation of Linear MomentumMomentum6. The total linear momentum of a system is

constant, if there is no external forces acting on the system.

7. The Principle of Conservation of Linear Momentum and Newton’s Third Law of Motion are consistent with each other.

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© Manhattan Press (H.K.) Ltd. 25

3.6 Work, energy and power (SB p. 137)

3.3 Elastic and inelastic collisions3.3 Elastic and inelastic collisions

8. The most fundamental law in Physics is the Principle of Conservation of Energy, which states that the total energy of a closed system is conserved.

9. For elastic collisions, the total kinetic energy after collision is equal to that before collision. Therefore, kinetic energy, linear momentum and total energy are conserved.

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© Manhattan Press (H.K.) Ltd. 26

3.6 Work, energy and power (SB p. 137)

3.3 Elastic and inelastic collisions3.3 Elastic and inelastic collisions

10. For inelastic collisions without external force, kinetic energy is not conserved, but total energy and linear momentum are conserved.

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© Manhattan Press (H.K.) Ltd. 27

3.6 Work, energy and power (SB p. 137)

3.4 Inertial mass and gravitational mass3.4 Inertial mass and gravitational mass

11. Inertial mass of a body is a measure of the reluctance to change its state.

12. Gravitational mass of a body is a measure of the gravitational attractive force acted on it (weight of the body).

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© Manhattan Press (H.K.) Ltd. 28

3.6 Work, energy and power (SB p. 137)

3.5 Conservation of momentum in two-3.5 Conservation of momentum in two-dimensiondimension13. If two equal masses collide obliquely, the

angle between the two masses after collision would be 90o.

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© Manhattan Press (H.K.) Ltd. 29

3.6 Work, energy and power (SB p. 137)

3.6 Work, energy and power3.6 Work, energy and power

14. Work (W) = Fs cosθ

where F and s are the magnitude of F and s respectively and θ is the angle between F and s.

15. Work is done by a force F to stretch a spring to produce an extension of e.

FeW21

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© Manhattan Press (H.K.) Ltd. 30

3.6 Work, energy and power (SB p. 137)

3.6 Work, energy and power3.6 Work, energy and power

16. The kinetic energy (K or KE) is the energy of a body due to its motion.

17. An object stores energy due to its physical condition or because of its position. The energy stored in the object is called potential energy (U or PE).

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© Manhattan Press (H.K.) Ltd. 31

3.6 Work, energy and power (SB p. 137)

3.6 Work, energy and power3.6 Work, energy and power

%100machine by the usedEnergy

machine by the done work Useful

machine a of Efficiency 19.

VelocityForceinterval Time

doneWork power Average 18.

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© Manhattan Press (H.K.) Ltd. 32

3.6 Work, energy and power (SB p. 138)

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© Manhattan Press (H.K.) Ltd. 33

End

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© Manhattan Press (H.K.) Ltd. 34

A force does no work if:

1. There is no displacement. e.g. No work is done by static friction.

2. The displacement is perpendicular to the applied force. e.g. No work is done by gravitational force if one walks on a horizontal road.

Return to

TextText

3.6 Work, energy and power (SB p. 125)

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© Manhattan Press (H.K.) Ltd. 35

The sign of work

The sign of work depends on the directions of force and displacement.

1. If their directions are the same, then positive work is done.

2. If their directions are opposite, then negative work is done.

Take an example of lifting a box upwards. The lifting force does positive work since it is acted in the same direction as the displacement. However, the weight of the box does negative work since its direction is opposite to that of displacement.

Return to

TextText

3.6 Work, energy and power (SB p. 126)

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© Manhattan Press (H.K.) Ltd. 36

Q:Q: A sphere of mass m at the end of a string of length is released when the string is horizontal. The sphere then collides with a block of mass 4m at rests on a smooth table. If the collision is perfectly elastic, find in terms of m, and g,(a) the velocity of the sphere, and(b) the velocity of the block after collision.

Solution

3.6 Work, energy and power (SB p. 131)

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© Manhattan Press (H.K.) Ltd. 37

Solution:Solution:The velocity u of the sphere just before collision is given by:

If v1 = velocity of sphere and v2 = velocity of block after collision, then using the Principle of Conservation of Momentum,

mu = mv1 + (4m)v2

u = v1 + 4v2 ..........................(1)By conservation of kinetic energy:

u2 = v12 + 4v2

2 .....................(2)Substituting (1) into (2),

(v1 + 4v2)2 = v12 + 4v2

2

v12 + 8v1v2 + 16v2

2 = v12 + 4v2

2

4v2 (3v2 + 2v1) = 0

3.6 Work, energy and power (SB p. 131)

gu,mgmu 2 21 2

22

21

2 )4(21

21

21 vmmvmu

(3)32

12 ..................vv

Substituting (3) into (1):

g

gvv

guv

vvvu

252

)253(

32

32

253

53

35)

32(4

12

1

111

Return to

TextText

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© Manhattan Press (H.K.) Ltd. 38

Q:Q: (a) A ball bearing is released from a height of 1 m from a metal plate. Describe how you would determine the fractional decrease in the kinetic energy of the ball bearing after it hits the plate. What happens to the difference in kinetic energy?(b) A neutron of mass m collides head-on with a carbon nucleus of mass 12m which was initially at rest. If the collision is elastic, find the ratio of the kinetic energy of the neutron after collision to its kinetic energy before collision. Solution

3.6 Work, energy and power (SB p. 132)

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© Manhattan Press (H.K.) Ltd. 39

Solution:Solution:(a) Suppose that the ball bearing is released from a height ho, and vo is the velocity of the ball bearing just before it hits the metal plate.Using the Principle of Conservation of Energy,

Let v1 = velocity of ball bearing immediately after collision, h1 = height reached by it after collision.Using the Principle of Conservation of Energy,

Therefore, the fractional decrease in kinetic energy:

That is, the fractional decrease in kinetic energy is determined by measuring the heights ho and h1 and substituting them into equation (3).The loss in kinetic energy is converted into heat and sound during collision.

3.6 Work, energy and power (SB p. 132)

(1)21

o2

o ..................mghmv

(2)21

12

1 ..................mghmv

(3)

21

21

21

o

1o

o

1o2o

21

2o

..................h

hhmgh

mghmgh

mv

mvmv

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© Manhattan Press (H.K.) Ltd. 40

Solution (cont’d):Solution (cont’d):(b)

Using the Principle of Conservation of Linear Momentum,mu1 + 12m (0) = mv1 + 12mv2

u1 = v1 + 12v2 ......................................... (1)Since the collision is elastic, kinetic energy of the system is conserved.

substituting (1) into (2), (v1 + 12v2)2 = v12 + 12v2

2

v2(132v2 + 24v1) = 0

3.6 Work, energy and power (SB p. 132)

(2)12 )12(21

21

21 2

221

21

22

21

21 ..................vvu,vmmvmu

(3)112

12 ..................vv

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© Manhattan Press (H.K.) Ltd. 41

Solution (cont’d):Solution (cont’d):

Return to

TextText

3.6 Work, energy and power (SB p. 132)

720169121

21

1311

21

collision beforeneutron ofenergy Kineticcollisionafter neutron ofenergy Kinetic

1311

)112)(12( :(1) into (3) ngSubstituti

21

2

1

11

111

.

mu

um

uv

vvu

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© Manhattan Press (H.K.) Ltd. 42

Q:Q: A toy car which is powered by a motor travels with constant velocity v. The figure shows the variation of the energy supplied by the motor with time t. If the constant force generated by the motor is F, find the value of v in terms of a, b, and F. (Neglect resistance to motion due to friction.)

Solution

3.6 Work, energy and power (SB p. 134)

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© Manhattan Press (H.K.) Ltd. 43

Solution:Solution:

Return to

TextText

3.6 Work, energy and power (SB p. 134)

aFb

Fab

v

Fvab

Fv

Fv

Fv

)(Velocity

graph ofGradient

interval TimedoneWork

work doing of Rate Power

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© Manhattan Press (H.K.) Ltd. 44

Q:Q: A manufacturer claims that the maximum power delivered by the engine of a car of mass 1 200 kg is 90 kW.(a) Find the minimum time in which the car could accelerate from rest to 30 m s−1.(b) An independent test quotes that a time of 12 s is needed to accelerate the car from rest to 30 m s–1. Suggest a reason for the difference from the time you have calculated.

Solution

3.6 Work, energy and power (SB p. 135)

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© Manhattan Press (H.K.) Ltd. 45

Solution:Solution:

(b) There is a difference in time because work is done to increase the kinetic energy of the car, and also work against friction.

Return to

TextText

3.6 Work, energy and power (SB p. 135)

s 610902

)30(1200Power

121 )( taken Time

2interval TimedoneWork Power

21 car by theenergy Kinetic car theof engine by the done Work (a)

3

22

2

2

mvt

tmv

mv