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Work, Energy and

Power

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LESSON OBJECTIVES

At the end of the lessons, pupils should be able to :

• Show understanding that kinetic energy, potential energy (chemical, gravitational, elastic), light energy, thermal energy, electrical energy and nuclear energy are examples of different forms of energy.

• State the principle of the conservation of energy and apply the principle to new situations or to solve related problems.

• State that

– kinetic energy Ek = ½ mv2 and

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• Recall and apply the relationship work done = force x

distance moved in the direction of the force to new situations or to solve related problems.

• Recall and apply the relationship power = work done/time taken to new situations or to solve related problems.

• Calculate the efficiency of an energy conversion using the formula efficiency = energy converted to useful output / total energy input

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Lesson Overview

• Energy

• Principle of Conservation of Energy

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Work

In Physics, work is said to be done when a force produces motion.

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RECALL FROM SEC 1’s WORK

Conditions For Work Done (Very Important !)

1. There is a force acting on an object. 2. The object moves.

3. The movement of the object is in the direction of the force.

object

Force applied by Mario The object moves in

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QUESTION

Is there work done??

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QUESTION

Is there work done??

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d

F

W

in

Newton, N

in

metre, m

in

Joule, J

Work

distance moved in the direction of the force

Work done = force x

Note:

The force exerted on the object must be in the same direction as the

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Moment Work

M = F x d W = F x d

d is the perpendicular distance between

applied force and pivot.

d is the distance moved

in the direction of the force.

Measured in

Newton-metre, Nm

Measured in

Joule, J

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Example 1

A box of 10 kg moves 3 m after being pushed by a constant force of 4 N. What is the work done by the push?

W = F x d

= 4 x 3

= 12 J

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Find the work done by gravity when a diver of mass 60 kg falls through a height of 11m.

Work done by gravity on diver

= F x d = Wdiver x d

= mdiverg x height

= (60 x 10) x 11

= 6600 J or 6.6 kJ

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Energy

• Defined as the capacity to do work

• The SI unit of energy is joule (J)

• There are different form of energy namely:

Kinetic energy

Gravitational potential energy

 Elastic potential energy e.g. rubber band

 Chemical potential energy e.g. food, fuel, battery

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When a body is in motion, it possesses kinetic energy. It can be shown that the amount of kinetic energy possessed by a moving body is given by:

K.E. = ½ m v2

Kinetic Energy (K.E.)

where m : mass of the body in kg;

v : velocity of the body in ms-1

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What is the instantaneous kinetic energy of a car of mass 1200 kg

(a) moving at a velocity of 20 ms-1? (b) at rest?

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(a)moving at a velocity of 20 ms-1?

K.E. = ½ mv2

= ½ (1200)(20)2

= 240000 J or 240 kJ

Instantaneous K.E. of the object is 240 kJ.

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(b) at rest  v = 0 ms-1

K.E. = ½ mv2

= ½ (1200)(0)2 = 0 J

Instantaneous K.E. of the object is 0 J.

Note: Object has K.E. only when in motion….

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A body possesses gravitational potential energy because of its relative position to the ground. Again it can be shown the gravitational potential energy possessed by a body is given by:

where m is the mass of the body in kg;

g is gravitational field strength in Nkg-1;

h is the height above the ground in m.

2.2 Gravitational Potential Energy (P.E.)

G.P.E. = m g h

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40 m

5 N 3 kg

5m

Terry pushes a box of 3 kg up a smooth slope with a

force of 5 N. If the box has moved 40 m and the height of the slope is 5 m,

(a) what is the gravitational potential energy gained by the box?

(b) how much work is done by Terry?

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40 m

5 N 3 kg

5m

(a)what is the gravitational potential energy gained by the box?

P.E. = m g h

= (3) (10) (5) = 150 J

Example 4

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40 m

5 N 3 kg

5m

(b) how much work is done by Terry?

W = F × d = 5 × 40 = 200 J

Example 4

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Principle of Conservation of Energy

It states that:

One of the most fundamental laws in Physics

“Energy cannot be created or destroyed,

but only changes from one form to

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Stored Chemical Energy 

Gravitational

Potential Energy

Kinetic Energy 

Work in driving the nail +

Sound + Heat

Gravitational Potential Energy

Kinetic Energy

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Ground

Potential energy

decreases as kinetic

energy increases.

However, at any

moment of time, total energy remains the same.

Just before ball is

dropped, total energy of the ball is made up of P.E. only.

In mid air, total energy of the ball is made up of P.E. and K.E.

Just before hitting the ground, total energy is made up of K.E. only.

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Example 7:

The diagram shows the heights above the ground of some points on the track of a roller coaster.

What is the speed of the roller coaster at P, Q and R? Assume negligible friction and air resistance.

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QUESTION:

Assume negligible friction and air resistance.

Therefore we can assume there is no:

- heat energy

- sound energy

Can you tell me what are the implications of these assumptions?

All the energy is

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Example 7:

A

Key point:

The total amount of energy in a system is always constant. i.e. Total Energy = K.E. + P.E.

P.E. only

K.E. only

K.E + P.E.

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At point A,

The roller coaster is not moving,

** K.E. = 0 J

Total energy = G.P.E.

= m g h1

= m x 1 0 x 16.2

= 1 6 2m J

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At point P,

** P.E. = 0 J

Total energy = K.E.

162m = ½ mvP2

162m = m (½ vP2)

162 = ½ vP2

vP2 = 324

vP = 18 ms-1

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At point Q,

Total energy = K.E. + P.E.

162m = ½ mvQ2 + mgh

2

162m = m (½ vQ2 + 10 x 11.2)

162 = ½ vQ2 +112

vQ2 = (162 - 112) x 2

= 100

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At point R,

Total energy = K.E. + P.E.

162m = ½ mvR2 + mgh

3

162m = m (½ vR2 + 10 x 9.0)

162 = ½ vR2 + 90

vR2 = (162 – 90) x 2

= 144

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Example 8:

A skier of mass 60 kg slides down a smooth slope as shown in the diagram below. The height of the slope is 20 m.

(a) At the instant where the skier reaches the bottom,

(i) what is amount of energy possessed by the skier? (ii) what is the speed of the skier?

(b) State any assumptions you made in (a)(ii)

20 m Analysis:

- Slide  start from rest i.e. v = 0 ms-1

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(a)(i)

20 m

At the top. Total Energy = G.P.E. At the bottom, Total Energy = K.E.

Loss of G.P.E. = Gain in K.E.

Amount of Energy possessed by the skier at the end

= ∆K.E = ∆G.P.E = mgh

= (60)(10)(20)

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(a)(ii)

∆K.E =

12000 =

v = = 20 ms-1

Speed of skier is 20 ms-1

2 2 1 mv 2 ) 60 ( 2 1 v 60 ) 12000 ( 2 (b)

Assume no friction and air resistance.

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20 m

5 N 3 kg

5m

(a) P.E. gained = 150 J

(b) Work done by terry = 200 J

Let’s Look @ Example 4 again…

Think…..

Is there a problem here?

Principle of conservation of energy doesn’t apply?

What happened to 50 J of energy?

 50 J of work done is used to overcome friction i.e. converted to heat and sound.

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3. Power

Power measures the rate of doing work

or the rate at which energy is transformed.

i.e. How fast work is done.

taken

Time

change

Energy

taken

Time

Done

Work

Power

The SI unit of power is Watt (W).

One Watt simply means one Joule per second.

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A crane lifts a 540kg up a vertical distance of 8m in 1 minute. Taking g to be 10 N kg-1.

Calculate

(a) the work done by the crane

(b) the power of the crane

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540 kg

8 m in 1 min

(a) W = F x d

= 540(10) x 8

= 43200 J

(b) P = W / t

= 43200 / t

= 43200 / (1x60)

= 720 W

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A car moves at a constant velocity of 25 ms-1 along a

straight road for 1 km. The resistive force acting on the car is 4000 N throughout the journey.

Example 10:

(a) What is the forward driving force provided by the car engine?

(b) What is the work done by the car engine?

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RECALL that in “Chap 3 DYNAMICS”

Constant Velocity

Newton’s 1st Law

- Balanced Forces

- No Net Force

Newton’s 2nd Law

- a = 0 ms-2

- Fnet = ma = m(0) = 0 N

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(a) Car moving at constant velocity implies that net force acting on car is zero.

Net force = Sum of all forces acting on car

0 = FE – 4000

FE = 4000 N

4000 N

Forward driving force, FE

a = 0 m/s2

Example 10:

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(b) W = F x d = 4000 x 1000 = 4 x 106 J

Work done by the car engine is 4 x 106 J.

Example 10:

(c) P = W / t

= 4000000 / t = 4000000 / 40

= 1 x 105 W

Power of the car engine 1 x 105 W.

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4. Efficiency

In reality, where there is friction, machines waste energy.

This energy is lost or dissipated as heat or

sound energy.

%

100

Input

Energy

Output

Energy

Useful

Efficiency

% 100   Input Power Output Power Useful Efficiency

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Example 11:

A generator is able to provide 5 000J output for an input of 6 000J.

Calculate

(a) the amount of wasted energy (b) the efficiency of the generator.

(a) Wasted energy = 6000 – 5000

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Example 11:

A generator is able to provide 5 000J output for an input of 6 000J.

Calculate

(b) the efficiency of the generator.

(b) Efficiency =

=

= 83.3 % (to 3 s.f.)

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done over a period of time change over a

period of time

is the ability to do conversions obey Conservation of energy principle Kinetic energy

Elastic potential energy

Gravitational potential energy Chemical potential energy Heat energy Light energy Sound energy Electrical energy Magnetic energy Nuclear energy Solar energy e.g. Energy

power = = energy

time

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References

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