Preview A Level Further Mathematics for AQA: Mechanics by Cambridge International Education

9781316644539 A LEVEL FURTHR MATHEMATICS FOR AQA MECHANIC SB BARKER, BARKET, CONWAY, SUCH C M Y K

This Student Book has been written for the AQA AS/A Level Further Mathematics specifications, for first teaching from 2017. Developed by a highly experienced author team with a wealth of maths teaching expertise, teachers and students can be confident that the content matches the course requirements.

For this linear course in 2017, AS/A Level Further Mathematics learning needs to go beyond rote techniques; students should develop a coherent understanding of mathematics as a whole subject. This is why our resources focus on promoting a deeper understanding throughout.

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Overarching themes of problem-solving, proof and modelling are built into every chapter, with additional Focus on pages to further develop students’ proficiency in these key mathematical skills. A synoptic approach underpins all the resources. This includes cross-topic review exercises and fast forward/rewind signposts to reinforce concepts and connect Pure and Applied topics. An extensive question bank includes discussion, synoptic, past paper and a wealth of practice questions, which are colour-coded for different skill levels.

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Continual assessment is embedded at chapter, strand and course level to help build student and teacher confidence with the new linear assessment.

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Further requirements for the specifications are fulfilled through opportunities to practise incorporating technology throughout.

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The unique Work it out feature challenges common misconceptions.

Visit cambridge.org/education for details of all AS/A Level Mathematics resources.

A LEVEL FURTHER MATHEMATICS FOR AQA MECHANICS STUDENT BOOK (AS/A LEVEL)

A Level Further Mathematics for AQA Mechanics Student Book (AS/ A Level)

Brighter Thinking

A Level Fur ther Mathematics for AQA

Mechanics Student Book (AS/A Level) Jess Barker, Nathan Barker, Michele Conway and Janet Such

Contents

Contents Introduction.............................................................. iv How to use this book................................................ v 1 Work, energy and power 1

1: The work done by a force.....................................2 2: Kinetic energy and the work–energy principle....5 3: Potential energy, mechanical energy and conservation of mechanical energy....................9 4: Power ��14

145

1: Variable force and vector notation.................. 145 2: Oblique impacts and the impulse– momentum triangle..........................................148 7 Circular motion 2 160 1: Conservation of mechanical energy................ 161 2: Problem solving situations............................... 172 8 Centres of mass 185 1: Centre of mass of a system of point masses....186 2: Centres of mass of standard shapes..............190 3: Centres of mass of composite bodies............ 196 4: Centres of mass by integration........................205 5: Equilibrium of a rigid body............................... 215

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23 2 Dimensional analysis 1: Defining and calculating dimensions................24 2: Units and dimensions of sums, differences and angles............................................................29 3: Finding dimensions from units and derivatives, conversion of units and predicting formulae............................................35 4: Summary of dimensions and units....................42

6 Momentum and collisions 2

3 Momentum and collisions 1 47 1: Momentum and impulse....................................48

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2: Collisions and the principle of conservation of momentum......................................................57

235 9 Moments and couples 1: Moments............................................................236 2: An introduction to couples..............................242 3: Vector methods.................................................246 4: Problem solving using moments and couples............................................................... 251

3: Restitution and kinetic energy...........................67

4 Circular motion 1 84 1: Linear speed versus angular speed...................85 2: Acceleration in horizontal circular motion........89 3: Horizontal circular motion in 3D........................95 5 Work, energy and power 2

107

1: Work done by a variable force f(x)...................108 2: Hooke’s law, work done against elasticity and elastic potential energy............................. 110 3: Work done by a force at an angle to the direction of motion........................................... 119 4: Problem solving involving work, energy and power .................................................................122

Focus on … Proof 2............................................ 262 Focus on … Problem solving 2.......................... 264

Focus on … Modelling 2.................................... 267 Cross-topic review exercise 2............................ 269

AS Level practice paper.......................................273 A Level practice paper..........................................275 Formulae................................................................277 Answers ..................................................................278 Glossary..................................................................295 Index...................................................................... 296 Acknowledgements..............................................298

Focus on … Proof 1..............................................135 Focus on … Problem solving 1.......................... 138 Focus on … Modelling 1.....................................141 Cross-topic review exercise 1............................ 143

iii

1 Work, energy and power 1 In this chapter you will learn how to: calculate the work done by a force calculate kinetic energy use the work–energy principle equate gravitational potential energy to work done against gravity understand and use the power of a driving force.

Before you start…

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•• •• •• •• ••

You should know how to convert units of distance, speed and time.

1 Convert 15 000 metres to kilometres.

A Level Mathematics Student Book 1, Chapter 18

You should know how to calculate the weight of an object from its mass, and know the unit of weight.

2 Calculate the weight of a car of mass 1150 kg, stating the unit with your answer.

A Level Mathematics Student Book 1, Chapter 18

You should be able to use Newton’s second law of motion: F = ma.

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GCSE

3 A resultant force of 50 N acts on an object of mass 2.5 kg. Calculate the acceleration of the object.

The relationship between work and energy In this chapter, you will learn the definition of the work done by a force, which is a quantity that is measured in joules, the same units that are used for energy. You will learn about propulsive and resistive forces. You will learn that work done by a propulsive force is equivalent to kinetic energy gained. Work done against a resistive force is equivalent to kinetic energy lost. The driving force of a car engine can cause a car to accelerate; work done by the car engine increases the kinetic energy of the car. Resistances to motion can cause a car to decelerate; work done against these forces decreases the kinetic energy of the car. You will also learn about power, which is the rate of doing work. Principles of work, energy and power are crucial in engineering, enabling engineers to design machines to do useful work. Hydroelectric power stations work by converting the work done by falling water first into kinetic energy, as the hydroelectric turbines rotate, and then into electricity. © Cambridge University Press

Rewind You have already studied the effect of a force or system of forces in A Level Mathematics Student Book 1, Chapter 18.

Fast forward In Chapter 5, you will learn about elastic potential energy and its conversion to kinetic energy.

A Level Further Mathematics for AQA Mechanics Student Book

Section 1: The work done by a force Work is done by a force when the object it is applied to moves. Some forces promote movement while others resist it. For example, when you cycle into a breeze, your pedalling promotes movement but the breeze acts against your movement. Forces that promote movement are propulsive forces and those that resist movement are resistive forces. Other propulsive forces include the tension in a rope being used to drag an object across the ground and the driving force of a vehicle engine. The driving force of an engine is often described as its tractive force. Other resistive forces include vehicle braking and resistance from still air.

Key point 1.1 For a force acting in the direction of motion:

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Weight is a special case because it can either resist or promote movement. When you cycle uphill your weight acts as a resistive force – you do work against your own weight. But when you cycle downhill your weight acts as a propulsive force – your weight does work on you. Work done by weight is usually described as ‘work done by gravity’. Work done against weight is usually described as ‘work done against gravity’.

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work done = force × distance

Work done is measured in joules (J):

1 joule = 1 newton × 1 metre 1J = 1N m

For example, a force of 5 newtons acting on an object that moves 15 metres in the direction of the force does 5 × 15 = 75 joules of work. Doubling the force to 10 newtons over the same distance would double the amount of work done to 150 joules. Likewise, doubling the distance moved to 30 metres with an unchanged force of 5 newtons would double the amount of work done to 150 joules.

WORKED EXAMPLE 1.1 A box is pushed 5 m across a horizontal floor by a horizontal force of 25 N. Calculate the work done by the force. Work done = force × distance = 25 × 5 J = 125 J

Use the definition of work done. State the units of work done (J) with your answer.

1 Work, energy and power 1 WORKED EXAMPLE 1.2 A lorry driver driving along a horizontal road applies a braking force of 75 kN for 25 m. Calculate the work done by the brakes, giving your answer in kilojoules (kJ). 75 kN = 75 000 N

Convert 75 kN to 75 000 N as you need to work in standard units.

Work done by brakes = braking force × distance

Use the definition of work done.

= 75 000 × 25 J = 187 5000 J = 1880 kJ (3 s.f)

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Change J to kJ.

Tip

Work done by the brakes against movement is equivalent to work done by the lorry against the brakes.

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WORKED EXAMPLE 1.3

A 50 kg crate is lifted 12 m by means of a rope and pulley system. Calculate the work done against gravity. Work done = force × distance

∴ Work done against gravity = weight × height gained Weight of crate = 50 × 9.8 = 490 N

Apply the definition of work done to the gravitational force. Force becomes weight and distance becomes height gained. Calculate the weight of the crate, using the approximation for the acceleration due to gravity of 9.8 m s −2 .

Work done against gravity = weight × height gained = 490 × 12 J = 5880 J

= 5900 J (2 s.f.)

You have used a value of g to 2 s.f. so this is an appropriate degree of accuracy for your final answer.

Fast forward

Key point 1.2 When a mass, m, is raised or lowered through a height h: work done by or against gravity = weight × height work done = mg × h

In Section 3 you will learn the equivalence of work done by or against gravity and gravitational potential energy.

A Level Further Mathematics for AQA Mechanics Student Book WORKED EXAMPLE 1.4 A competitor of mass 75 kg dives from a diving board that is 10 metres high into a pool. Air resistance averages 12 newtons as he descends 10 metres through the air. Resistance from the water then averages 3000 newtons as he descends 2.0 metres further. Calculate: a the total work done by gravity as he descends 12 metres b the total work done against air and water resistance during this descent. a Work done by gravity = mgh = 75 g × 12 ≈ 8800 joules (2 s.f.) b

You have used a value of g (9.8 m s-2) to 2 s.f. so this is an appropriate degree of accuracy for your final answer.

Work done against air resistance = 12 × 10 = 120 joules Use force × distance to calculate the work done by each of the resistances.

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Work done against water resistance = 3000 × 2 = 6000 joules Total work done against resistances = 6120 joules

WORKED EXAMPLE 1.5

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A van of mass 1250 kg travels along a straight road. The driving force of the vehicle engine is 500 newtons and resistance to motion is 220 newtons, on average. The van travels 1.5 km from one delivery to the next, descending 8 metres in height. Find: a the work done by the vehicle engine b the work done by gravity c the work done against resistance. a 15 . km = 1500 metres

Work done by vehicle engine = 500 × 1500

= 750 000 joules

Convert distance to SI units. Use force × distance to calculate the work done by the vehicle engine.

b Work done by gravity = mgh

= 1250 g × 8

= 98 000 joules

c Work done against resistance = 220 × 1500

= 330 000 joules

Use force × distance to calculate the work done against resistance.

EXERCISE 1A In this exercise, unless otherwise instructed, use g = 9.8 m s −2 , giving your final answers to an appropriate degree of accuracy. 1

A parcel is dragged 5 metres across a horizontal floor by means of a horizontal rope. The tension in the rope is 12 N. Calculate the work done by the tension in the rope.

Susan climbs a vertical rock 32 m high. Susan’s mass is 65 kg. Calculate the work done by Susan against gravity.

1 Work, energy and power 1 3

Sunil descends a vertical ladder. His mass is 82 kg and the work done by gravity is 2150 J. Find the height Sunil descends.

In this question use g = 10 m s −2, giving your final answer to an appropriate degree of accuracy. A ball of mass 100 g is dropped from a window. Calculate the work done by gravity as it falls vertically to the ground 6.0 m below.

A puck slides 50 metres across an ice rink, against a resistive force of 2.5 N. Calculate the work done against resistance.

A cyclist travelling on horizontal ground applies a driving force of 25 N against a headwind of 10 N and a resistance from friction of 5.0 N. The cyclist travels 1.2 km. Find: a the work done by the cyclist

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b the total work done against wind and friction. A fish basket is raised from the sea floor to a fishing boat at sea level, 18 metres above. The mass of the basket is 15 kg. The resistance to motion from the seawater is 50 N. Calculate the total work done, against gravity and water resistance, in raising the fish basket.

A driving force of 400 N does 50 kJ of work moving a van along a horizontal road from A to B. Resistance to motion averages 185 N. Calculate the work done against resistance as the van moves from A to B.

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Section 2: Kinetic energy and the work–energy principle Kinetic energy is the energy an object has because it is moving.

Tip

Key point 1.3

An object of mass m moving with speed v has kinetic energy 1 mv 2 . 2

If mass is measured in kilograms (kg) and speed is measured in metres per second (m s −1 ), kinetic energy is measured in joules (J).

If speed is not given in m s −1, you should convert to m s −1 before you start the rest of your calculations.

WORKED EXAMPLE 1.6

A particle of mass 1.5 kg is moving with kinetic energy 48 joules. Calculate the speed of the particle. 1 mv 2 2 Substituting and rearranging to find speed: Kinetic energy =

1 × 1.5 × v 2 2 ∴ v 2 = 64 ⇒ v = ± 8 m s −1 48 =

Since speed is a positive quantity,

Use the formula for kinetic energy.

As mass was given in kg and kinetic energy in joules, speed is in m s −1.

v = 8 m s −1 © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book WORKED EXAMPLE 1.7 A cyclist slows down from 25 km h −1 to 10 km h −1 . The combined mass of the cyclist and her bicycle is 95 kg. Calculate the loss of kinetic energy. Let u be the starting speed and v be the final speed. 25 10 u= = 6.944 m s −1 and v = = 2.778 m s −1 3.6 3.6

To convert km h −1 to m s −1 you must multiply by the conversion factor 1000 , 3600 which simplifies to division by 3.6.

WORKED EXAMPLE 1.8

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Loss of kinetic energy = initial kinetic energy - final kinetic energy 1 1 Loss of kinetic energy = mu2 − mv 2 2 2 1 1 Loss of kinetic energy = × 95 × 6.9442 − × 95 × 2.7782 2 2 = 1920 J (3 s.f.)

Calculate the increase in kinetic energy when a boat of mass 2.0 tonnes changes velocity from (3.0i + 4.0j) m s −1 to (4.5i + 4.5j) m s −1. Give your answer in kJ. (Starting speed)2 = 32 + 42 = 25 (Final speed) = 4.5 + 4.5 = 40.5 2

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Gain in kinetic energy = final kinetic energy – initial kinetic energy Gain in kinetic energy =

Use Pythagoras’ theorem to convert the velocity vectors to speeds. You need the square of the speed, not the velocity vector, for the kinetic energy formula.

1 m(v 2 − u2 ) 2

2 tonnes = 2000 kg

1 Gain in kinetic energy = × 2000 × (40.5 − 25) 2 ≈ 15.5 kJ

You can write 1 mv 2 − 1 mu 2 in 2 2 factorised form. Convert 2 tonnes to 2000 kg. Divide by 1000 to convert joules to kJ.

The work–energy principle is an essential idea in mechanics that enables you to calculate and compare the work necessary to cause a change in kinetic energy.

Tip

Key point 1.4 The work done by a force on an object causes an equal increase in its kinetic energy. Work done = 1 mv 2 − 1 mu 2 2 2

Work done by propulsive forces causes an increase in kinetic energy. Work done against resistive forces causes a loss of kinetic energy. To use the work– energy principle you must calculate the total work done on the moving object. Total work done = work done by propulsive forces − work done against resistive forces 6

Remember that gravity acts as: • a propulsive force when the object is moving downwards • a resistive force when the object is moving upwards.

1 Work, energy and power 1 WORKED EXAMPLE 1.9 A particle of mass 1.6 kg is at rest on a smooth horizontal plane. It is acted on by a constant horizontal force of 8.0 N. Find the speed of the particle after it has travelled 5.0 metres. Work done = force × distance

Work done = force × distance

= 8×5 = 40 joules Work–energy principle: work done = 1 mv 2 2

Applying the work–energy principle: 40 = 1 × 1.6 × v 2 2 v 2 = 50

WORKED EXAMPLE 1.10

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⇒ v = 7.1m s −1 (2 s.f.)

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Stephen is driving his car along a horizontal road at 55 km h −1 when he notices a broken-down vehicle, just off the road, 150 m ahead. Stephen and his car together have a mass of 1025 kg and the total resistance to motion is assumed constant at 500 N. Stephen believes he should slow down and that he can slow down sufficiently without applying the brakes. Calculate Stephen’s speed, in km h −1, as he reaches the broken-down vehicle, taking account of the resistance to motion.

Work done against resistance = resistive force × distance = 500 × 150 = 75 000 J

55 3.6 ≈ 15.28 m s −1

Assume that Stephen allows the resistance to motion to slow his car down over 150 m. There is no driving or braking force. Calculate the work done against resistance.

55 km h−1 =

Convert 55 km h −1 to m s −1 .

Loss of kinetic energy = initial kinetic energy - final kinetic energy Loss of kinetic energy = 1 × m × (u 2 − v 2 ) 2 Using the work–energy principle:

Write down the expression for loss of kinetic energy.

1 × 1025(u2 − v 2 ) 2 Rearranging and solving for v :

75 000 =

2 × 75 000 u2 − v 2 = 1025 ≈ 146.3 v 2 ≈ 15.282 − 146.3 v = 9.337 m s −1 v ≈ 9.337 × 3.6 km h−1

Work–energy principle: work done against resistance = loss of KE

Substitute in the value for u. Convert back to km h −1

v = 33.6 km h−1 (3 s.f.) © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book EXERCISE 1B In this exercise, unless otherwise instructed, use g = 9.8 m s −2, giving your final answers to an appropriate degree of accuracy. 1

Calculate the kinetic energy of a cyclist and her bicycle, having a combined mass of 70 kg, travelling at 12 m s−1 . Give your answer in kJ.

Calculate the mass of an athlete who is running at 8.5 m s−1 , with kinetic energy 3500 J.

Calculate the speed of a bus of mass 20 tonnes with kinetic energy 1100 kJ. Give your answer in km h −1.

A box of mass 5.0 kg is pulled from A to B across a smooth horizontal floor by a horizontal force of magnitude 10 N. At point A, the box has speed 1.5 m s−1 and at point B the box has speed 2.8 m s−1 . Ignoring all other resistive forces, find:

b the work done by the force c the distance AB. 5

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a the increase in kinetic energy of the box

A car driver brakes on a horizontal road and slows down from 20 m s−1 to 12 m s−1 . The mass of the car and its occupants is 1150 kg. a Find the loss in kinetic energy.

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b Given that the work done against resistance to motion is 50 kJ, find the work done by the brakes.

A child of mass 35 kg descends a smooth slide, after propelling herself onto the top at 1.6 m s −1. Ignoring air resistance, calculate her speed at the bottom of the slide, which is 2.1 metres lower than the top.

A bullet of mass 10 grams passes horizontally through a target of thickness 5.0 cm. The speed of the bullet is reduced from 240 m s−1 to 90 m s−1. Calculate the magnitude of the average resistive force exerted on the bullet.

A train of mass 100 tonnes is travelling at 108 km h −1 on horizontal tracks, when the driver sees a speed reduction sign. The train’s speed must be reduced to 75 km h −1 over 500 m. Resistance to motion is approximately 8 kN. Calculate the braking force required, in kN.

A package of mass 500 grams slides down a parcel chute of length 3.5 metres, starting from rest. The bottom of the chute is 2.2 metres below the top. The speed of the package at the bottom of the chute is 4.5 m s−1. Find the resistance to motion on the chute.

10 Eddy cycles up a hill. His mass, together with that of his bicycle, is 92 kg. His driving force is 125 N and resistance from friction is 45 N. Eddy travels 350 metres along the road, which rises through a vertical height of 32 metres. His starting speed is 8.2 m s−1. Find his final speed.

1 Work, energy and power 1

Section 3: Potential energy, mechanical energy and conservation of mechanical energy Consider an object of mass m falling freely under gravity from height h1 to height h2 , with starting speed u and final speed v. Since the only external force acting on the object is gravity, the work–energy principle becomes: work done by gravity = increase in kinetic energy

u h1 – h2 h1

v h2

2 2 ⇒ mg (h1 − h2 ) = mv − mu 2 2

ground level

Rearranging this gives:

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2 2 mgh1 − mgh2 = mv − mu 2 2 2 2 mu mv ⇒ mgh1 + = mgh2 + 2 2

Each side of this equation is made up of the sum of two terms, one of which is kinetic energy. The other term is gravitational potential energy. Gravitational potential energy is equal to the work done by gravity causing an object of weight mg to fall through height h if no external forces act on the object.

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Key point 1.5

Gravitational potential energy (GPE) = mgh , where h is the height above ground (zero) level.

If no external force acts on the object, the sum of kinetic energy and gravitational potential energy is conserved. The sum is usually called mechanical energy.

Tip

Whilst you can choose any height as your ground (zero) level it is usually best to choose the lowest height reached by the moving object.

Key point 1.6

If the only force acting on an object is its weight then mechanical energy is conserved. GPE + KE = mgh + 1 mv 2 = constant 2

where h is the vertical height above the zero level.

A Level Further Mathematics for AQA Mechanics Student Book

1 mu2 2

mgh1

ob j as ect sp it d esc eeds u en po ds p ten con tia l kin verte ener gy eti c e d to ne rgy

1 mv 2 2

mgh2

o as bjec it t s ki as lo ce w co net nd s d po nv ic e s ow e te rt ne n nt ed rg ia y l e to ne rg y

mechanical energy is conserved

This diagram may help you to understand the formula for conservation of mechanical energy more easily. As an object descends vertically in height it speeds up, so gravitational potential energy is converted into kinetic energy. As an object ascends vertically in height it slows down, so kinetic energy is converted into gravitational potential energy. An object will stop its vertical ascent when all of its kinetic energy has been converted to gravitational potential energy.

mghmax

WORKED EXAMPLE 1.11

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ground level

Faisal throws a ball of mass 125 grams upwards from ground level, with a speed of 12.5 m s−1. Assuming no external forces apply, calculate:

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a the speed of the ball after it has risen 5.0 metres b the maximum height gained by the ball. a Starting KE = 1 × 0.125 × 12.52 2 = 9.766 J Starting KE = mgh + final KE

9.766 = 0.125 g × 5 + final KE

Final KE = 3.635 J

Convert 125 g to 0.125 kg .

Use conservation of mechanical energy over the first 5 metres of the ascent.

Take the gravitational potential energy at ground level to be zero. Calculate the final kinetic energy of the ball.

1 2 mv = 3.635 2 3.635 Final speed = 0.5 × 0.125 = 7.6 m s −1 (2 s.f.)

b Starting KE = mghmax

= 0.125 g × hmax

Calculate the final speed of the ball.

Use conservation of mechanical energy over the whole ascent (final kinetic energy is zero). All the kinetic energy will have been converted into gravitational potential energy. Calculate the maximum height gained.

⇒ hmax = 8.0 metres (2 s.f.)

1 Work, energy and power 1

Using energy to solve problems The principle of conservation of mechanical energy applies to the situation where the only force acting on an object is its weight. You have already used the work–energy principle to solve problems involving other propulsive and resistive forces. You are now ready to combine the work–energy principle and the principle of conservation of energy: (GPE1 + KE1 ) + work done by driving forces − work done against resistive forces = (GPE 2 + KE 2 ) When using this formula you must remember that you do not need to include work done by gravity or work done against gravity as these are already accounted for.

WORKED EXAMPLE 1.12

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When an object moves vertically upwards or downwards you can work out the change of gravitational potential energy. When an object moves diagonally upwards or downwards it is only the vertical component of the movement that causes a change in gravitational potential energy – you need not consider the horizontal component of movement. This simplification often makes the energy approach to problems very useful.

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A 1.5 kg package is attached to one end of an inextensible string. The string and package are being raised by the action of a pulley. The tension in the string is 18 N. Find the height gained by the package as it increases in speed from 1.2 m s−1 to 3.2 m s−1. 1 Increase in KE = × 1.5 × (3.22 − 1.22 ) Calculate the increase in kinetic energy 2 = 6.6 joules work–energy principle: Propulsive work done − resistive work done = 6.6 joules

18 × h − 15 . g × h = 6.6

total work done = increase in KE work done = tension × h − mg × h

6.6 h = = 2.0 metres 18 − 1.5 g

WORKED EXAMPLE 1.13

Helen cycles from rest at the top of a sloping track, 35 m above the valley floor. She pedals downhill, then continues along a horizontal track, before ascending 10 m on an uphill track and stopping. The total distance she travels is 500 m. The average resistance to motion is 55 N. The combined mass of Helen and her bicycle is 62 kg. Calculate the total work done by Helen and the average driving force she applies.

35 m 10 m valley floor

Continues on next page © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book

mgh1 + KE1 + work done by Helen − work done against resistance = mgh2 + KE2 KE1 = KE2 = 0

Use the work–energy principle and the principle of conservation of energy. Helen has no kinetic energy at the start of her ride and none at the end. You do not need to consider her motion throughout her ride – just at the start and at the end.

Work done against resistance = resistive force × distance = 55 × 500 = 27 500 J

Calculate the work Helen does against resistance.

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The distance used is the total distance along the road.

62g × (35 − 10) + work done by Helen = 27 500

Let both kinetic initial and final energy be zero and rearrange:

mgh1 − mgh2 + work done by Helen − work done against resistance = 0 mgh1 − mgh2 is the loss of potential energy of Helen and her bicycle.

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Work done by Helen ≈ 27 500 − 15 200 ≈ 12 000 J

Helen’s average driving force work done by Helen distance 12 000 = 500 = 25 N (2 s.f.) =

Use Helen’s work done, together with her distance travelled, 500 m, to calculate her average driving force.

Did you know?

Conservation of energy is an important principle throughout Physics. Work done by a moving object against resistance, which is lost mechanical energy, is converted to other forms of energy such as heat and noise. This means that total energy is still conserved. The mechanical equivalent of heat was first proposed by James Joule and explains the relationship between mechanical energy and heat energy.

1 Work, energy and power 1 EXERCISE 1C In this exercise, unless otherwise instructed, use g = 9.8 m s −2 , giving your final answers to an appropriate degree of accuracy. 1

Calculate the increase in potential energy when a mass of 5.0 kg is raised by 25 m.

In this question, use g = 10 m s−2, giving your final answers to an appropriate degree of accuracy. Calculate the loss of potential energy when a mass of 2 tonnes is lowered through 10 m. A boy of mass 68 kg gains 3600 J of potential energy by climbing a vertical rope. Calculate the height he gains.

A toy train loses 1.5 J of potential energy when it descends a spiral track, losing 50 cm in height. Find the mass of the toy train.

Felipe strikes a golf ball off an elevated tee. The golf ball has mass 45 grams and Felipe imparts an initial speed of 35 m s−1 to the ball.

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a Find the initial kinetic energy of the golf ball.

The ball lands on the green 25 metres below the tee. b Calculate the loss of potential energy of the ball.

c Calculate the kinetic energy of the ball as it lands on the green. d Calculate the speed of the golf ball as it lands on the green.

Anita dives off a highboard into a diving pool. When Anita leaves the highboard she has a speed of 7.5 m s −1 and she is 8.0 metres above the water surface. Anita’s mass is 60 kg.

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a Find Anita’s kinetic energy as she leaves the highboard.

b Calculate Anita’s kinetic energy as she enters the water. c Calculate Anita’s speed as she enters the water.

d What modelling assumptions have you made to simplify your calculations?

Wing serves a 58 gram tennis ball with a speed of 9.5 m s −1 from a height 3.0 metres above the level of the tennis court. Assuming there are no resistive forces acting on the ball, calculate: a the kinetic energy of the ball as Wing serves it

b the potential energy lost by the ball as it descends to the level of the court c the kinetic energy of the ball as it strikes the court d the speed of the tennis ball as it strikes the court.

Preeti descends a smooth slide starting from rest. Her mass is 58 kg. Overall, her change in vertical height above the ground is 5.8 m and her speed at the bottom of the slide is 6.5 m s −1. Calculate the work done against resistance during her descent.

A package of mass 0.80 kg is projected down a smooth sloping parcel chute with a speed of 2.2 m s −1. The height of the bottom of the chute is 7.5 m vertically below the top. Assuming there are no external resistive forces, calculate: a the loss of potential energy of the package b the speed of the package at the bottom of the chute. © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book 10 Karol slides on his sledge down a straight track of length 210 m, descending 32 m . The combined mass of Karol and his sledge is 72 kg . Karol’s starting speed is 2.8 m s −1 and his speed at the end of his descent is 10.5 m s −1 . Calculate the average resistance to motion, R N, during Karol’s descent. 11 Loretta and her bicycle have a combined mass of 75 kg. Loretta cycles up a straight hill AB, accelerating from rest at A to 4.0 m s −1 at B. The level of point A is 5.5 m below the level of B. Find: a the increase in kinetic energy of Loretta and her bicycle as she cycles from A to B b the increase in potential energy of Loretta and her bicycle. During her ride, the resistance to motion is constant at 60 N parallel to the road surface and Loretta does 8500 J of work.

Section 4: Power

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c Calculate the distance from A to B.

Power is the rate of doing work. Average power is defined as the total work done by a force divided by the time taken.

Key point 1.7 When the force applied is constant:

work done time taken

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average power =

Often, you consider power in relation to a driving force but it applies equally to any constant force acting on an object. Power is measured in watts (W). 1 joule per second is equal to 1 watt.

Did you know?

James Watt (1736–1819) was a Scottish engineer and scientist. The unit of power is named after him.

WORKED EXAMPLE 1.14 A crane lifts a 2.5 tonne concrete block 35 m in 25 seconds. Calculate the average power rating of the crane during the lift, giving your answer in kW. Work done against gravity = weight × height gained = 2500 g × 35

Calculate the work done by the crane lifting the block against gravity.

= 87 500 g J 87 500 g 25 = 34 000 W or 34 kW (2 s.f.)

Power =

Use the definition of power =

work done time taken

1 Work, energy and power 1 WORKED EXAMPLE 1.15 The engine brakes on a truck have a power rating of 25 kW. Calculate the total work done in 5.0 seconds by the braking force at this average power rating, giving your answer in kJ. Work done by brakes = 250 000 × 5

Rearrange the definition of power to make work done the subject. work done = power × time

= 1250 000 J or 1250 kJ

Convert your answer to kJ.

WORKED EXAMPLE 1.16

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A pump is used to raise water from a well. In one minute, 1500 litres of water are raised 8 metres before being ejected into a tank at a speed of 7.5 m s−1. The density of water is 1000 kg m−3. a Calculate the gain of potential energy of the water per second. b Calculate the gain of kinetic energy of the water ejected per second. c Calculate the power of the pump, in watts. There are 1000 litres in 1m3 , with a mass of 1000 kg.

Work out the mass of 1500 litres of water.

The mass of 1500 litres of water is 1500 kg.

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1500 g × 8 60 = 1960 J 1 × 1500 × 7.52 2 b Gain of KE of water per second = 60 = 703.125 J a Gain of PE of water per second =

c Total gain of mechanical energy per second = 2700 W

Use mgh to calculate the gain in potential energy of the water per second. Use 1 mv 2 to calculate the gain of kinetic 2 energy of the water per second. Use conservation of mechanical energy: work done by the pump = gain in GPE + gain in KE The gain of total mechanical energy per second is the power of the pump.

You can use an alternative formula for power when solving problems. From the definitions of power and work done: Power = work done = force × distance = force × distance = force × speed time taken time taken time

This definition allows you to work out power at a specific point in time if you know the force and the speed. This is often referred to as ‘instantaneous power’ and can be used to work out power when either the force or the velocity varies over time.

Key point 1.8 Power = tractive force × speed © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book WORKED EXAMPLE 1.17 Chris is cycling on a horizontal road. He is moving at a constant speed of 8.0 m s −1 with a power output of 200 W . Calculate the total resistance to Chris and his bicycle, in newtons. 200 = tractive force × 8

Power = tractive force × speed

⇒ tractive force = 25 N Tractive force − total resistive force = 0 ∴ tractive force = total resistive force

As Chris is travelling at constant speed the resultant force is zero.

∴ total resistive force = 25 N

WORKED EXAMPLE 1.18

90 km h−1 = 25 m s −1

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Julia is riding her motorbike along a horizontal road. She is travelling with constant speed 90 km h −1, at an engine power of 15 kW . Julia decides to overtake and increases to full power, 20 kW. Assuming the resistance to motion is unchanged, calculate Julia’s acceleration. Julia and her motorbike have a combined mass of 465 kg . Convert Julia’s speed to m s−1.

Power = tractive force × speed power speed

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⇒ tractive force =

Use the definition of power, but rearrange to make tractive force the subject.

For the motorbike: 15 000 Tractive force = = 600 N 25

Calculate the tractive force of Julia and her motorbike when she is travelling at constant speed.

tractive force − resistance to motion = 0 ∴ tractive force = resistance to motion ∴ resistance to motion = 600 N

As Julia is cruising at constant speed the resultant force is zero. Hence calculate the resistive force.

When Julia increases to full power:

When Julia increases the power, the tractive force increases so that it is greater than the resistive force, and she accelerates. Calculate the resultant force.

Tractive force =

power speed

20 000 25 = 800 N =

Resultant force = tractive force − resistance to motion = 800 N − 600 N = 200 N Using F = ma : 200 = 465 × acceleration

Use F = ma to calculate Julia’s initial acceleration.

= 0.430 m s −2 (3 s.f.)

1 Work, energy and power 1 WORKED EXAMPLE 1.19 1

A car of mass 1250 kg is travelling along a straight horizontal road against a resistance to motion of kv 2 N , where v is the speed of the car and k is a constant. When the engine is producing a power of 13.5 kW , the car has speed 12.5 m s−1 and is accelerating at 0.45 m s−2. a Find the value of k. The maximum constant speed of the car on this road is 28 m s−1. b Find the engine’s maximum power, giving your answer in kW. 0.45 m s–2 R

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12.5 m s–1

kv 2

Let T be the tractive force of the car engine. 1

1250g N 1

Resultant force = T − resistance.

a Resultant force = T − kv 2 power speed

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Resistance varies with v 2 .

13 500 12.5 = 1080 N

⇒T =

Resultant force = mass × acceleration

Rearrange the formula: power = force × speed. Calculate T . Use F = ma.

1 2

1080 − k × 12.5 = 1250 × 0.45 1080 − 1250 × 0.45 12 = 146 units (3 s.f.)

b T ′ − kv 2 = 0

Rearrange to find the value of k.

Let the new driving force be T ′. As the car is now moving with constant speed the resultant force is now zero.

T′ = ⇒

maximum power speed

1 maximum power − 146.4 × 28 2 = 0 28 1

Maximum power = 146.4 × 28 2 × 28

Rearrange to find the maximum power rating of the car engine.

= 22 kW (2 s.f.)

A Level Further Mathematics for AQA Mechanics Student Book EXERCISE 1D In this exercise, unless otherwise instructed, use g = 9.8 m s −2, giving your final answers to an appropriate degree of accuracy. A 38 tonne truck is able to brake from 65 km h −1 to rest in 20 seconds. Find the average power rating of the brakes.

A crane lifts a 2 tonne concrete block 25 m in 12 seconds. Find the average power of the crane.

A lift of mass 800 kg can accommodate up to 12 people, who are assumed to have combined mass no more than 1500 kg. Calculate the average power required by the lift motor to raise the maximum load through 60 m in 45 s.

A car engine has a maximum driving force of 750 N when travelling at 80 km h −1. Calculate the average power of the engine.

A train engine has a power rating of 2.5 MW . Calculate the tractive force when the train is travelling at 216 km h −1 .

Find the average power exerted by a climber of mass 78 kg when climbing a vertical distance of 35 m in 3 minutes.

A boat is travelling at a constant speed of 16 km h −1. The boat has mass 10.5 tonnes and the engine is working at its maximum power output of 8 kW. Calculate the work done when the boat is displaced (5.0i + 6.0j) km.

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Find the average power of an engine that lifts 500 bags of flour 5 m in 1 hour. Each bag of flour has mass 50 kg.

A pump is used to raise water from a well that is 12 metres deep. Water is raised at a rate of 50 kg per second. It is ejected into a pipe at a speed of 5.5 m s−1 .

a Calculate the gain of potential energy of the water per second. b Calculate the gain of kinetic energy of the water ejected per second. c Calculate the average power of the pump, in watts.

10 Victoria is cycling on level ground. Victoria and her bicycle have a combined mass of 61.5 kg and she is working at a rate of 380 W. Given that Victoria is accelerating at 0.65 m s−2, find the sum of the resistive forces acting on Victoria and her bicycle at the instant when her speed is 7.5 m s−1 . 11 Stan is driving his 35 tonne truck on a horizontal road. Stan accelerates from 50 km h −1 to 65 km h −1, which is his maximum speed at 500 kW power output. Find the maximum acceleration of the truck, assuming that total resistance is constant. 12 Vince is driving his van against a constant resistance to motion of 5500 N . The van has mass 2.8 tonnes and engine power 125 kW . Vince’s acceleration at the instant when his speed is u m s−1 is 0.90 m s −2. Calculate u. 3

13 The resistance to motion of a car is kv 2 newtons, where v m s−1 is the speed of the car and k is a constant. The power of the car’s engine is 12 kW and the car has a constant speed of 27.5 m s−1 along a horizontal road. Show that k ≈ 3.0. 18

1 Work, energy and power 1 14 A rocket, Athena, of mass 500 kg is moving in a straight line in space, without any resistance to motion. Athena’s rocket motor is working at a constant rate of 500 kW and its mass is assumed to be constant. Athena’s speed increases from 90 m s−1 to 140 m s−1 in time t seconds. a Calculate the value of t . b Calculate Athena’s acceleration when its speed is 120 m s−1 .

Checklist of learning and understanding In this chapter you have learned the relationship between mechanical work and mechanical energy. You have learned the work–energy principle and the principle of conservation of energy. You have used the definition of power to solve problems.

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• Work done = force × distance • Work done against gravity = weight × height gained • Gravitational potential energy: GPE = mgh

1 mv 2 2 • Work–energy principle: work done = change in energy work done • Average power = time taken • Power = tractive force × speed

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• Kinetic energy =

A Level Further Mathematics for AQA Mechanics Student Book

Mixed practice 1 In this exercise, unless otherwise instructed, use g = 9.8 m s −2 , giving your final answers to an appropriate degree of accuracy. 1

An osprey, flying at 5 m s−1, is carrying a 2.5 kg salmon towards the chicks in its nest, when it drops the fish 15 metres into the loch. Assume there is no air resistance and calculate: a the kinetic energy of the salmon when it is dropped by the osprey b the potential energy lost by the salmon as it falls to the water surface c the kinetic energy, and hence the speed, of the salmon as it enters the water.

Inge, who has mass 62 kg, takes part in a ski-jumping contest. She achieves a speed of 20 m s−1 at the point of take-off and lands at a point in the landing zone 18 metres vertically below. Assuming there is no air resistance, calculate:

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a Inge’s kinetic energy at take-off

b Inge’s loss of gravitational potential energy as she descends through 18 metres c Inge’s kinetic energy and hence her speed, as she lands. 3

Leo throws a stone of mass 500 grams into the sea from the top of a cliff 50 metres above sea level. He throws the stone with speed 8 m s−1. a Calculate the kinetic energy of the stone as it leaves Leo’s hand.

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b Calculate the potential energy lost by the stone as it enters the sea.

c Calculate the kinetic energy of the stone as it enters the sea and, hence, its speed at this time.

Carol, a circus performer, is on a swing. She jumps off the swing and lands in a safety net. When Carol leaves the swing, she has a speed of 7 m s−1 and she is at a height of 8 metres above the safety net. Carol is to be modelled as a particle of mass 52 kg being acted upon only by gravity.

a Find the kinetic energy of Carol when she leaves the swing.

b Show that the kinetic energy of Carol when she hits the net is 5350 J, correct to 3 significant figures. c Find the speed of Carol as she hits the net.

A car travels along a straight horizontal road. The resistance to motion is kv N, where v is the speed of the car, measured in m s−1 . The car travels at a constant speed of 25 m s−1 and the engine of the car works at a constant rate of 21 kW. Show that k = 33.6.

Find the average power produced by a climber of mass 82 kg in climbing a vertical distance of 65 metres in 3 minutes.

1 Work, energy and power 1 7

A pump is being used to empty a flooded basement. In one minute, 400 litres of water are pumped out of the basement. The water is raised 8 metres and is ejected through a pipe at a speed of 2 m s−1. The mass of 400 litres of water is 400 kg. a Calculate the gain in potential energy of the 400 litres of water. b Calculate the gain in kinetic energy of the 400 litres of water. c Hence calculate the power of the pump, giving your answer in watts. [© AQA 2011] A cyclist rides from rest up an inclined rough track with an average pedalling force of 38 N. She travels a distance of 850 metres along the track, whilst gaining 25 metres in height. Resistance to motion from the track averages 18 N. The cyclist and her bicycle have a mass of 68 kg . Calculate her speed at the end of her ride.

A child of mass 28 kg descends a slide of length 25 metres, losing 4.5 metres in height. She starts from rest and reaches the bottom of the slide at 6.5 m s−1 . Find the average resistive force from the slide during her descent.

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10 A car travels along a straight horizontal road. When its speed is v m s −1 , the car experiences a resistance force of magnitude 25v newtons.

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a The car has a maximum constant speed of 42 m s−1 on this road.

Show that the power being used to propel the car at this speed is 44 100 watts.

b The car has mass 1500 kg.

Find the acceleration of the car when it is travelling at 15 m s−1 on this road under a power of 44 100 watts. [© AQA 2012]

11 A train consists of an engine and five carriages. A constant resistance force of 3000 N acts on the engine and a constant resistance force of 400 N acts on each of the five carriages. The maximum constant speed of the train on a horizontal track is 90 km h −1.

a Show that this speed is 25 m s−1.

b Hence find the maximum power output of the engine. Give your answer in kilowatts. [© AQA 2011]

12 A train, of mass 22 tonnes, moves along a straight horizontal track. A constant resistance force of 5000 N acts on the train. The power output of the engine of the train is 240 kW. Find the acceleration of the train when its speed is 20 m s−1. [© AQA 2013]

A Level Further Mathematics for AQA Mechanics Student Book 13 Alan is driving a train of mass 65 tonnes at its maximum speed of 42.5 m s−1 on a straight horizontal track. Its engine is working at 850 kW . a Find the magnitude of the resistance acting on the train. When the train is travelling at 42.5 m s−1, Alan disengages the engine and the train slows down. Assume that the total resistance is unchanged. b Use a work–energy calculation to find how far the train travels as it reduces its speed from 42.5 m s−1 to 32.5 m s−1 . 14 Calculate the loss of kinetic energy when a boat of mass 3.5 tonnes reduces in velocity from (3.0i + 4.0j) m s −1 to (2.5i + 3.0j) m s −1. 15 Use the equation of motion, F = ma, together with the formula v 2 = u 2 + 2 as , to derive the relation Fs = 1 m(v 2 − u 2 ). 2

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16 A particle of mass 500 grams moves along the x-axis under the action of a propulsive force F . The particle’s displacement, s metres, depends on time, t seconds, as shown: s = 3t 2 + 2t Find the power of force F when t = 5 seconds.

17 A van of mass 1500 kg travels along a horizontal road against a constant resistive force of 225 N. The van travels with constant acceleration from rest, at time t = 0 seconds, to 15 m s −1 at time t = 30 seconds. It then travels at constant speed for 120 seconds before decelerating to rest over 25 seconds. The speed–time graph illustrates the motion.

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speed (m s–1) 15

150

175

time (seconds)

Calculate the power of the vehicle engine when: a t = 20 seconds

b t = 120 seconds.

Calculate the power of the van’s brakes when: c t = 160 seconds.

2 Dimensional analysis In this chapter you will learn how to: understand the concept of dimensions use the language and symbols of dimensional analysis understand the connections between units and dimensions check the validity of a formula by using dimensional considerations predict formulae by using dimensional analysis.

Before you start…

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• • • • •

A Level Mathematics Student Book 1, Chapter 2

You should be able to work with indices and surds.

GCSE

You should be able to rearrange formulae.

2 Make x the subject of the formula. 2 3 y = x zt t +1

GCSE

You should be able to solve simultaneous equations.

3 Solve these simultaneous equations. 2x + 3y = 2 3 x − 2 y = 16

GCSE

You should be able to express direct and indirect proportion in mathematical terms.

4 P is inversely proportional to r 2 . If P = 2 when r = 2, what is the value of P when r = 6?

GCSE

You should know common area and volume formulae.

5 What, in terms of π, is: a the volume b the surface area of a sphere of radius 3 cm?

A Level Mathematics Student Book 1, Chapter 16

You should be familiar with the SI units of mass (kg), length (m) and time (s).

6 What are the SI units of velocity?

1 Simplify each expression. a

r 5r 8 r9 −4 3

(r 4 )3

3 6 27

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c 8

Continues on next page

A Level Further Mathematics for AQA Mechanics Student Book 7 What is the angle, in radians, of a sector of a circle of radius 4 cm and arc length 5 cm?

A Level You should know the Mathematics definitions and units of Student Book 1, velocity and acceleration. Chapter 16

8 A particle moving in a straight line with constant velocity travels 10 m in 2 seconds. What is its velocity? State the units. 9 A particle moving in a straight line with constant acceleration increases its velocity from 8 m s −1 to 15 m s −1 in 10 seconds. What is the acceleration? State the units.

A Level You should know the Mathematics definition and units of Student Book 1, force. Chapter 18

10 A mass of 3 kg is acted on by a constant force of 12 N. What is its acceleration? State the units.

Chapter 1

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A Level You should know the Mathematics definition of a radian. Student Book 2, Chapter 7

You should know the definitions of kinetic energy 1 mv 2 and 2 potential energy (mgh ).

(

)

11 A mass of 3 kg is held at a height of 2 metres vertically above the ground. The particle is released from rest. By equating its loss in potential energy to its gain in kinetic energy, find its speed at the instant when it hits the ground. Use g = 9.8 m s−2, giving your final answer to an appropriate degree of accuracy.

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What is dimensional analysis?

In dimensional analysis you look at the type of quantity you are dealing with rather than the specific units. You use it as a mathematical way of checking that equations and formulae are consistent, and that you are combining like quantities, and also to predict and establish formulae.

Section 1: Defining and calculating dimensions The dimension of a given quantity describes what sort of quantity you are measuring; for example, any distance or length, whatever its units, has the dimension of length and has the symbol L. You can use square brackets to represent ‘the dimension of’ so, for example, [metres] = L . The dimension of distance is L. The diameter of a pin, the radius of a circle, the length of a running track and the distance from London to Hong Kong would all be measured in different units but they are all measurements of length or distance and have the dimension L. The other common dimensions that you use in Mechanics are M for mass and T for time.

2 Dimensional analysis The mass of a spider, the mass of an elephant, the mass of a sphere might all be measured in different units but they are all measurements of mass with the dimension M. Similarly time, whether measured in seconds, days or centuries, has the dimension T. If t is a time in seconds, then it has dimension T. 2t and 60t will also be times with dimension T. The 2 and the 60 do not affect the units as they are numbers and numbers are dimensionless.

Did you know? In the USA, there is a unit of mass called a slug!

Some branches of science use other dimensions, for example, the dimensions of temperature, electric current, amount of light and amount of matter.

Did you know?

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There is a connection between dimensional analysis and the greenhouse effect. The concept of dimensional analysis is often attributed to Joseph Fourier, a famous French mathematician and physicist. He is best known for the Fourier series, which is widely used in Mathematics and Physics, and for his work on heat flow.

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Fourier is widely recognised as being the first scientist to suggest that the Earth’s atmosphere would act as an insulation layer – the idea now known as the greenhouse effect.

Key point 2.1

The dimensions of quantities in Mechanics can be expressed in terms of M for mass, L for length and T for time.

Square brackets are used to abbreviate the phrase 'the dimension of', so for example, [time] = T.

Fast forward Dimensionless constants are explored in greater detail later in this chapter.

Finding dimensions

To find the dimensions of quantities that are multiplied or divided, you combine their dimensions in the same way as the quantities are combined. WORKED EXAMPLE 2.1 Find the dimensions of: a velocity

b acceleration

c force = mass × acceleration.

a If an object is moving with constant velocity v in a straight line and it moves a distance s in time t, then you have the relationship: State an equation for velocity. v=s t Continues on next page © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book

[v ] =

[s] [t ]

Write down the dimensions of the right-hand side of the equation and simplify. The dimension of distance is L and of time is T. Use negative indices when you divide by dimensions.

=L T = LT −1

In more general terms: v = ds dt

Find the dimensions – ds has the same dimensions as s and dt has the same dimensions as t.

[ ds ] [ dt ] [s] [t ]

L = T = LT −1

ds has the same dimensions as s . dt t

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[v ] =

State the general case.

b If a particle starts from rest and moves with constant acceleration a in a straight line gaining speed v in time t, then: dv dt [dv ] [a ] = [dt ]

State a definition of acceleration.

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[v ] [t ]

Find the dimensions. dv has the dt same dimensions as v . t

LT −1 T = LT −2 =

F = ma

[ force ] = [m ][a ] = MLT −2

WORKED EXAMPLE 2.2

Work out the dimensions of: a area

b kinetic energy.

a [area] = [length][length] = L2

Area formulae always involve multiplying two lengths together or squaring a length. Continues on next page

State an equation for force… …and take dimensions of both sides of the equation.

Tip Vector quantities such as velocity and displacement have the same dimensions as their scalar equivalents (speed and distance). Remember that vectors have magnitude and direction, but scalar quantites have only magnitude, not direction.

2 Dimensional analysis

1 Kinetic energy = mv 2 2 [kinetic energy] =

( 21 ) [m][v ]

= [m ][v ]2

State the formula for kinetic energy. To find the dimensions, you need to multiply the dimension of m by the square of the dimensions of v. 1 2 is a constant so has no dimensions and does not affect the calculation of dimensions.

= ML2T −2

Dimensionless quantities

Remove the brackets and simplify the result.

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[m ][v ]2 = M(LT −1)2

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If all the dimensions cancel out, then the quantity is dimensionless. This is true of many quantities in Mechanics that are described as coefficients. Examples are the coefficient of restitution (which you will meet in Chapter 3) and the coefficient of friction. The coefficient of friction, µ , between two surfaces is defined as the ratio of the limiting frictional force, F, to the normal reaction force, R. Both FLIM and R have the dimensions of force that you worked out in Worked example 2.1.

µ=

[µ ] =

Rewind

You met the coefficient of friction in A Level Mathematics Student Book 2, Chapter 18. In this chapter, you will be given the definition when it is required, as a reminder.

FLIM R

[ FLIM ] [R]

−2 = MLT −2 MLT = M0L0 T 0 =1

So µ is dimensionless.

You can leave out dimensionless quantities when you are working out the dimensions of a formula or expression, or you can put in the number 1 to represent the dimensionless quantity.

Key point 2.2 Numerical constants, such as the real numbers, π and e, are dimensionless. For example, in the formula C = 2 πr, 2 and π are dimensionless.

A Level Further Mathematics for AQA Mechanics Student Book

Tip

EXERCISE 2A 1

Find the dimensions of each quantity, or state if it is dimensionless. a linear acceleration (a) b acceleration due to gravity ( g ) c force (ma) d weight e momentum (mv ) f π in the formula C = 2 πr g volume h density (mass per unit volume) i moment of a force F (force × distance) j pressure (force per unit area)

State the dimensions of tan 2 θ .

a Find the dimensions of potential energy (mgh ).

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State the dimensions of sin θ .

b Are these the same as the dimensions of kinetic energy? a Work out the dimensions of work done (work done = force × distance).

b How does this compare to the dimensions of kinetic or potential energy? The coefficient of restitution e is defined as relative velocity of separation e= . Find [e ]. relative velocity of approach The refractive index n of a material is defined as n = c where c is the v speed of light in a vacuum and v is the speed of light through the material. Find [n ].

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State the dimensions of dF where F is a force and t is time. dt

a G iven that all forms of mechanical energy have the same dimensions, find the dimensions of mechanical energy. b The mechanical energy stored in an elastic string of initial length 2 l extended by a distance x is λ x , where λ is the modulus of 2l elasticity of the string. Find [ λ ].

10 Newton’s law of gravitational attraction states that the force of attraction between two masses m1 and m2 that are a distance r apart Gm1m2 is , where G is the gravitational constant. Find [G ]. r2 11 The energy–frequency relationship for slow moving particles is given by the formula λ = h , where λ is the wavelength, m is the mv mass of the particle, v is the velocity of the particle and h is Planck’s constant. Find the dimensions of h. 28

Kinetic energy and potential energy have different formulae but they are both expressions of mechanical energy and so have identical dimensions. Forces such as friction, tension, thrust and reaction force all have the same dimensions however they are described.

Once you have established the dimensions of a quantity, then the dimensions will be the same however you calculate it.

2 Dimensional analysis

Section 2: Units and dimensions of sums, differences and angles Key point 2.3 You can only add and subtract terms that have the same dimensions. When you add or subtract two or more quantities with the same dimensions, then the resulting sum or difference will also have the same dimensions.

If you add two or more lengths, then the answer is also a length with dimension L. If you add and subtract several forces the answer is also a force.

Common error

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You can add 10 minutes to 3 hours or you can add 6 kilometres to 5 miles but you cannot add 10 seconds to 6 metres to give any form of meaningful result.

You can only add or subtract terms with the same dimensions to give a consistent formula. You can use this principle to check whether or not a formula is dimensionally consistent; this is called an error check.

Remember that you can only add or subtract quantities if they have the same dimensions. They do not however have to have the same units.

The sum u + v where u and v are speeds is also a speed and has the dimension of speed.

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In dimensional terms:

[u + v ] = [u ] + [v ]

= LT −1 + LT −1 = LT −1

The sum

∑ m v has the same dimensions as mv which is: i i

i =1

[m ][v ] = (M)(LT −1 ) = MLT −1

The integral which is:

∫ v dt is a sum and has the same dimension as v dt t

[v ][dt ] = (LT −1 )T =L For sums and differences, you should check that the dimensions of the terms that you are adding or subtracting are the same. Then the dimensions of the answers will also be the same. For products and quotients you must multiply or divide the dimensions.

Tip Many dimensional analysis questions look very complicated as they involve formulae, often with indices. Do not let the look of the question put you off, it’s just about applying rules!

A Level Further Mathematics for AQA Mechanics Student Book WORKED EXAMPLE 2.3 Given that a , r , r1 , r2 and h are lengths and m1 and m2 are masses, check that the terms being added or subtracted have the same dimensions and find the dimensions of the result.  m r + m2r2  b  1 1  m1 + m2 

a ar 2 + arh

a [ar 2 + arh ] = [ar 2 ] + [arh ]

The dimensions of both terms are L3 , so the dimension of their sum is also L3 .

= L3 + L3 = L3  m r + m2r2  [m1r1 ] + [m2r2 ] b  1 1 = [m1 + m2 ]  m1 + m2 

3 3 c  r1 + r2  r1 + r2

  r13 + r23   =  r + r  1 2  3 [r1 ] + [r23 ] = [r1 ] + [r2 ]

The dimensions of both terms of the numerator are L3, so the dimension of their sum is also L3.

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3 = L L =L

The dimensions of both terms in the numerator are ML so the dimension of their sum is also ML. The dimensions of both terms in the denominator are M, so the dimension of their sum is also M. The dimension of the quotient is L.

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= ML M =L

r13 + r2 3 r1 + r2

The dimensions of both terms of the denominator are L, so the dimension of their sum is also L.

Divide L3 by L giving L2 and take the square root.

WORKED EXAMPLE 2.4

Is the equation v 2 = u 2 + 2 gt , where u and v are velocities, g is the acceleration due to gravity and t is time, dimensionally consistent? Checking the dimensions of each term:

To check an equation for consistency you need to find the dimensions of each term and show that they all have the same dimensions.

Velocity involves dividing distance by time so has dimensions LT −1.

Find the dimensions of v 2 by squaring the dimensions of v.

[v 2 ] = [v ]2 = (LT −1)2 = L2T −2 Continues on next page

2 Dimensional analysis

Similarly [u2 ] = L2T −2

The dimensions of u 2 will be the same as those of v 2 as they are both velocities.

[2gt ] = [2][g ][t ]

Find the dimension of 2 gt by multiplying the dimensions of 2 and g (acceleration) and t .

= [g ][t ] [g ][t ] = (LT −2 )T = LT −1 As the dimensions of the three terms are not the same the equation is not dimensionally consistent so cannot be correct.

Dimensions of angles and trigonometric functions

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Rewind

The definition of an angle in radians is the ratio:

You learned about radians in A Level Mathematics Student Book 2, Chapter 7.

arc length angle in radians = radius

As both arc length and radius are lengths then the dimensions of angle are L = L0 (= 1) which is dimensionless. L

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All trigonometric functions are dimensionless for the same reason – each is the ratio of two quantities with the same dimensions.

Key point 2.4

An angle has units but is dimensionless.

WORKED EXAMPLE 2.5

What are the dimensions of angular velocity, ω = dθ where θ is an angle in radians? dt

Angular velocity ω = dθ radians per second dt where θ is the angle in radians

[ω ] =

[dθ ] [dt ]

Define the quantity involved – angular velocity is rate of change of angle and has the symbol ω . Equate the dimensions of all terms in the equation.

=1 T = T −1

A Level Further Mathematics for AQA Mechanics Student Book

Did you know? The metric system originated during the French Revolution of the 1790s. It was intended to provide a unified system of measures that used the metre and kilogram as standard units of length and mass, respectively. The name of the system, SI, stands for système international d’unités. The units are now commonly used by the scientific communities of most developed nations. The main units are metres for length, kilograms for mass and seconds for time. The wider adoption of this system, sometimes known as MKS after the units, was the result of an initiative, started in the late 1940s, to standardise units. At that time, the UK was using feet, pounds and seconds as standard and most of Europe was using centimetres, grams and seconds (cgs).

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Definitions of some SI units Some common SI units have particular names.

Rewind

The newton is the unit of force. 1 newton (N) is the force required to give a mass of 1 kilogram an acceleration of 1 metre per second per second. The joule is the unit of work and energy. 1 joule (J) is the work done (or energy transferred) to an object when a force of 1 newton acts on that object in the direction of motion for a distance of 1 metre.

Recall the formula for force from A Level Mathematics Student Book 1, Chapter 18: force = mass × acceleration.

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The newton metre is the unit of moment (or torque). It is the effect of a force of 1 newton applied perpendicularly to a moment arm of 1 metre.

The moment of a force about a point is force × perpendicular distance to the line of action of that force.

Rewind

Recall the formula for work done from Chapter 1, work done = force × distance.

The watt is the unit of power. 1 watt (W) is a rate of energy transfer or a rate of working of 1 joule per second. The pascal is the unit of pressure. 1 pascal is the pressure exerted by a force of 1 newton acting on an area of 1 square metre. Pressure is force per unit area. EXERCISE 2B

In this exercise, these letters refer to specific quantities: • u and v represent velocities

• a represents acceleration

• r , s , h , x and y represent distance or displacement

• θ represents an angle

• F represents force

• t represents time.

2 Dimensional analysis 1

Given that r , l and h are measurements of length, state the dimensions of: b h 2 + rl

a r + l + h 2

c r 2l − h 3 .

Given that mi are masses, xi are distances and vi are speeds, state the dimensions of: b 1 mv22 − 1 mv12 a m1v1 + m2v2 2 2 n

∑m x i

2 i

∫ v dt . n

∑m x i

Given that mi are masses and xi are distances, state the dimensions of

∑m

Given that m represents mass, u and v represent speeds, a represents acceleration, t and T represent times and l and h represent distances, find the dimensions of each term in these equations and hence determine which equations are dimensionally consistent. b s = ut + 1 at a v 2 = u 2 + 2 as 2 1 1 2 2 d impulse (force × time) = change in momentum c mv − mu = mgh 2 2 2 e T = 2 π l g

a Write down the dimensions of angular acceleration, commonly written as θ . g b Is the formula θ = − θ dimensionally consistent? Give a dimensional argument for your answer. l

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In simple harmonic motion (SHM) the restoring force measured towards the centre of the motion is proportional to the displacement, x , measured away from the centre of the motion.

a Write this as an equation, in terms of m , x and t, using k as the constant of proportionality. b Find the dimensions of k.

Angular momentum is defined as Iω where I is the moment of inertia a Work out the dimensions of angular momentum.

( ∑ mr ) and ω is angular velocity. 2

b Are these the same as the dimensions of linear momentum, where linear momentum is defined as

∑ mv?

c Explain why angular momentum is sometimes call ‘moment of momentum’. 8

The rotational kinetic energy of a rigid body about an axis is defined as 1 Iω 2 where I is the moment 2 of inertia mr 2 of the body about that axis and ω is the angular velocity.

(∑ )

a Work out the dimensions of rotational kinetic energy. b Is this the same as the dimensions of translational kinetic energy?

A Level Further Mathematics for AQA Mechanics Student Book 9

Young’s modulus, E , for a solid is defined as E = stress . Stress is the pressure in the solid and strain strain is defined as the ratio of extension to the original length. a Write a formula for E in terms of F , A , l , and x , where F is the force exerted on the solid, A is its cross-sectional area, l is the original length and x is the extension. b What are the dimensions of E?

10 A student writes the equation for the path of a projectile as: gx y = x tan θ − 2 sec2 θ 2v a Find the term in this equation that is dimensionally inconsistent.

WORK IT OUT 2.1

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b Suggest an alteration to one variable in this term that would make it dimensionally consistent.

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A particle of mass m is fixed at the midpoint of an elastic string of natural length 2l. The string is then fixed to two points A and B on a smooth horizontal surface, AB = 2a and a > l. When the particle is displaced through a small distance x along the perpendicular bisector of AB it is thought to perform small oscillations. The modulus of elasticity of the string is λ and it has the dimensions of force. Use dimensional analysis to determine which option gives the correct formula for the periodic time of these oscillations. A T = 2 π

ma 2l 2 λ (a − l )

B T = 2 π

mal 2 λ (a − l )

C T = 2 π

mal 2 λ (a − l ) 2

Which is the correct solution? Identify the errors made in the incorrect solutions. Solution 1

Formula A:

T = 2π

ma l is correct 2 λ (a − l ) 2

because the right-hand side has the dimensions of time.

Solution 2

Solution 3

Formula B:

Formula C:

T = 2π

mal is correct 2 λ (a − l )

because the right-hand side has the dimensions of time.

Tip You can derive dimensions of a quantity either from its formula or from its units. Any formula for that quantity will have the same dimensions. The volume of an icosahedron will have the same dimensions as the dimensions of a cube: L3. You only need to know that it is a volume to state its dimensions; you do not need to know the specific formula.

mal is correct 2 λ (a − l ) 2 because the right-hand side has the dimensions of time.

T = 2π

2 Dimensional analysis

Section 3: Finding dimensions from units and derivatives, conversion of units and predicting formulae This process is similar to finding the dimensions of a quantity from its formula. WORKED EXAMPLE 2.6

(

)

A pascal is a unit of pressure. Pressure is force per unit area force . The poiseuille (PI) is the (very rarely area used!) SI unit of dynamic viscosity. It is equivalent to pascal seconds (Pa s). Find the dimensions of a poiseuille.

pressure = force area

A pascal is a unit of pressure so you can find its dimensions from the definition of pressure as force per unit area.

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  [Pa ] =  force   area 

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To find the dimensions of dynamic viscosity you do not need to know its formula, or even what it is, as long as you know its units. You are told that it is measured in pascal seconds.

Simplify the dimensions of a pascal…

[mass][acceleration] [area]

−2 [Pa ] = MLT 2 L = ML–1T –2

[poiseuille] = [Pa ][s ]

= ML–1T –2T = ML–1T –1

…then multiply by the dimension of seconds to give the required dimensions.

You have seen that angles have units but not dimensions. This makes it difficult to predict units from dimensions. For example, angular velocity, ω , has dimension T −1 but units of radians per second. Frequency also has dimension T −1 but has units of hertz (Hz, sometimes called cycles per second).

Key point 2.5 You can predict dimensions from units or formulae but it is not always possible to predict units from dimensions.

A Level Further Mathematics for AQA Mechanics Student Book There are quantities that you might think of as constants that have dimensions even if they are not always written with units. The tension T in an elastic string of initial length l which has been stretched to (l + x ) is given by the formula T = λ x , where λ is the l modulus of elasticity for the string.

λ is a physical constant, so if the string were made of a different material, then it would have a different value. λ has the same units and dimensions as the tension. Other examples of physical constants are surface tension and the gravitational constant.

Common error Do not assume that a quantity represented by a letter is dimensionless unless you are told specifically that it is.

Fast forward You will study the tension in an elastic string in Chapter 5.

WORKED EXAMPLE 2.7

First state a formula involving λ .

Then rearrange it to give a formula for λ .

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a The tension (force) T in an elastic string or spring of initial length l, which has been stretched to (l + x ), is given by: T =λ x l Tl λ= x

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a Derive the dimensions of λ , the modulus of elasticity. b State the units of λ .

[λ ] =

[T ][l ] [x ]

−2 = MLT L L = MLT −2

b The units are newtons as x is dimensionless. l

Find the dimensions of each term and combine them.

As x and l have the same dimensions, their quotient will be dimensionless so it is reasonable to assume that T and λ will have the same units – newtons – which is in keeping with the dimensions.

Finding dimensions of second derivatives You saw in Worked example 2.1 that the dimensions of acceleration are 2 LT −2. You know that acceleration can be written as a = d x2 , but how do dt you find the dimensions of acceleration from this?

Rewind You learned about nonuniform acceleration in A Level Mathematics Student Book 1, Chapter 16.

2 Dimensional analysis You know that:

Common error

[dx ] [v ] = [dt ] =

You should recognise that

( )

d 2 x ≠ dx dt dt 2 so you cannot say that:

[x] [t ]

= LT −1

2 [ a ] =  d x2   dt 

It follows that:

( ) So  d x  =  d ( dx )   dt   dt dt  d2 x = d dx dt 2 dt dt

=  dx   dt 

  =  x2  t  = L2 T = LT −2

[ x ]2 [t ] 2

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= L2 T − 2

Using dimensions to convert units

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If two quantities are equal, then their dimensions must be the same, whatever their units. So to find a conversion factor you first need to find the dimensions of the quantities involved and then put these into the expressions for each quantity in the formula. For example, if you are converting hours to seconds, the conversion factor for the T dimension is 60 × 60 = 3600. So if the dimension of the quantity required involves T 2, then the conversion factor involves 36002. WORKED EXAMPLE 2.8

In the centimetres, grams and seconds (cgs) system, a force measures 30 000 dynes. What is this in newtons?

[force] = MLT −2

For M, 1gram = 0.001kg

For L, 1centimetre = 0.01metres For T, 1second = 1second

You do not need to know the definition of a dyne to solve this problem, since you are told that it is a force. You just need to know the dimensions of force. State the dimensions of force (mass × acceleration). For each dimension, put in its conversion factor from cgs to SI units.

The conversion factor is 0.001 × 0.01 × 1−2 = 0.000 01

Put these conversions into the dimensions MLT −2 to find the conversion factor.

30 000 dynes = 30 000 × 0.000 01newtons

Apply this to the question.

= 0.3 N

A Level Further Mathematics for AQA Mechanics Student Book

Using dimensions to predict formulae Key point 2.6

Rewind

You can use dimensional analysis to predict formulae by equating the dimensions of the terms of the proposed formula.

If you take dimensions of both sides of a proposed formula and then equate the indices of each dimension, you will get a set of simultaneous equations. You will need to know, or be able to derive, the dimensions of common quantities such as density, force, pressure and acceleration.

Recall from Section 1 that numerical constants, and other dimensionless quantities such as trigonometric functions, ratios and angles, can be left out of the calculation or given the dimension 1.

WORKED EXAMPLE 2.9

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Pressure, P , is measured in newtons per square metre. Surface tension, S, is defined as force per unit   length  force  .  length  a Derive the dimensions of pressure. b Find the dimensions of surface tension. c The pressure P inside an ideal soap bubble is given by the formula P = 2 Rα S β , where 2 is a dimensionless constant, R is the radius of the sphere and S is the surface tension. Find the values of α and β and hence find the formula for P. newtons  Use the units of pressure given to write a [pressure (P )] =  2 metres   an expression for the dimensions. [force] Newtons are units of force so have the = [metres]2 units of force or mass × acceleration. [P ] =

[mass × acceleration] [metres]2

M × LT −2 L2 −1 −2 = ML T =

force b [surface tension (S )] =  length    [mass × acceleration] = [length]

Metres are units of length. Simplify the indices to give a single expression for the dimensions.

Use the definitions of force and length to find the dimensions of surface tension in the same way.

MLT −2 L = MT −2

[S ] =

c P = 2Rα S β

Write down the formula given in the question.

[P ] = [R ]α [S ]β

Write the dimensional equation, remembering that 2 is dimensionless so can be left out.

ML−1T −2 = Lα (MT −2 )β

Substitute in the dimensions of each quantity… Continues on next page

2 Dimensional analysis

For M : 1 = β

…and equate the indices of the dimensions on each side of the equation to find the values of α and β .

For L : –1 = α For T : –2 = –2β This gives α = −1and β = 1.

Put these values of α and β back into the given formula and simplify.

∴ P = 2R S = 2S R

−1 1

WORKED EXAMPLE 2.10

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A simple pendulum consists of a particle of mass m suspended at the end of an inextensible string of length l. The pendulum is initially hanging at rest and then it is displaced through a small angle θ and released to make small oscillations. a It is thought that the formula for the periodic time T of the small oscillations is of the form T = Amα l β g γ , where A is a dimensionless constant and g is the acceleration due to gravity. Use dimensional analysis to find the values of α , β and γ and hence find an equation for T . b What deductions can you make from this formula? 2π when l = 2. Using g = 10 m s −2, find the value of A. c In an experiment it is found that T = 5 T = Amα l β g γ

(1)

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The periodic time T has dimension T.

[T ] = T

T = [Amα l β g γ ]

= [A ][m ][l ][g ] α

A is dimensionless.

[m ] = M

The dimensions of both sides of the equation must be the same and are equal to T. State the dimensions of each of the terms…

[l ] = L

[g ] = LT −2

T = Mα (LT −2 )γ Lβ

= Mα Lβ +γ T −2γ Equating indices of T:

…then combine them as the formula states and simplify.

T1 = T −2γ so 1 = −2γ giving γ = − 1 2 Equating indices of M: M0 = Mα so 0 = α Equating indices of L: L0 = Lβ +γ so 0 = β + γ giving β = 1 2

Continues on next page

A Level Further Mathematics for AQA Mechanics Student Book

This gives: α =0 1 β = 2 1 γ =− 2

Solve the equations to find the values of α , β and γ ...

So T = Am 0l 2 g =A

−

...and then substitute these values into equation (1) and state a formula for A.

1 2

l g

T 2g l 2 A2 = 4 π × 10 = 4 π2 5 2 A = 2π

Rearrange the expression for T to make A the subject and substitute the values given to find A.

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c A2 =

You now need to consider your answer as the question asks for a deduction. You see that the formula does not include m or θ , so the periodic time T will be the same whatever the mass of the particle as long as the length of the string is unchanged, for small angle displacements θ .

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b You can deduce that for displacements through a small angle θ the periodic time is independent of θ and is also independent of m. T will be the same whatever the mass m of the particle.

So T = 2π l g

EXERCISE 2C

A watt is a unit of 1 joule per second. Derive the dimensions of watts.

The sievert is a unit of 1 joule per kilogram. Derive the dimensions of sieverts.

2 Work out the dimensions of d ω2 , where ω is an expression for angular velocity. dt

A yank is defined to be the rate of change of force with time. What are the dimensions of yank?

5 Using the standard notation, the area of a triangle can be written as area = 1 ab sin C . By stating the 2 dimensions of each of the components (area, 1 , a , b and sin C) and combining them, show that this formula 2 is dimensionally correct. 6

In a simple harmonic motion the displacement x can be written as x = asin ω t, where x is the displacement and a is the amplitude (greatest distance from the centre of oscillation). a Use a dimensional argument to explain why this formula is dimensionally consistent. b Find the dimensions of ω .

2 Dimensional analysis 7

a State the dimensions of force. b In the centimetres, grams and seconds (cgs) system, a force has magnitude 45 000 dynes. Calculate this in newtons.

a = b = c = 2 Rα , where R is the radius of the circumcircle of the sin A sin B sin C triangle and α is a constant. Use dimensional analysis to find the value of α , showing the steps in your argument clearly.

Decibels are used to describe how loud a noise is. A formula for sound level in decibels is sound intensity (dB) = 10 log10  I  , where I is the sound output, in watts, and I 0 is the threshold level sound output, in watts.  I0 

The sine formula states that

a Write down the dimensions of decibels. b A speaker has a sound output of 100 000 times the threshold level. Express this in decibels.

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10 a State the dimensions of acceleration. b An equation for oscillations of a damped simple harmonic motion when a system is displaced through a 2 small distance x is given by d x2 + A dx = −Bx where A and B are constants. Given that this equation is dt dt dimensionally consistent find: i the dimensions of A

ii the dimensions of B.

11 a What are the dimensions of force?

b The thrust, F, of a propeller blade is a force which is thought to have a formula of the form:

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F = 0.5 ρ α A β (v12 − v02 )γ

where r is the density of the air, A is the surface area and v0 and v1 are velocities. Use dimensional analysis to find the values of α , β and γ and hence find a formula for F in terms of ρ , A , v12 and v02 .

12 a Tension is a force. What are the dimensions of tension? b The periodic time, t, of the vibration of a piano wire, of mass m, length l and tension F is thought to be of the form t = 2 πF α m β l γ

where 2 and π are dimensionless constants. Use dimensional analysis to find the values of α, β and γ and hence find a formula for t in terms of F, m and l.

13 The Froude number, Fr, is a dimensionless constant which can be used in analysing channel and river flows. The formula for Fr is of the form: Fr = v α g β h γ where v is the velocity of the water in the channel, g is the acceleration due to gravity and h is a relative depth. a Use dimensional analysis to find β and γ in terms of α. b Take α = 1 to find a formula for Fr in terms of v, g and h.

14 A light inextensible string of length l is fixed at one end and has a particle of mass m fixed at the other end. The mass m is moving at constant speed v in a horizontal circle of radius r and the string is fully extended. The string makes an angle θ with the downward vertical. Given that tan θ = v α r β g −1, use a dimensional argument to find a formula for tan θ in terms of v , r and g , where g is the acceleration due to gravity. © Cambridge University Press

A Level Further Mathematics for AQA Mechanics Student Book

Section 4: Summary of dimensions and units Exercise 2D is a summary of common units and dimensions. EXERCISE 2D Copy and complete this table. Quantity

Dimension

SI unit

Time Mass Weight (mg )

newton (N)

Length/displacement Volume Velocity

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Area

LT −2

Acceleration

m/s 2 or m s −2

Acceleration due to gravity Force (ma)

newton (N)

(

Kinetic energy 1 mv 2 2

)

joule (J)

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Gravitational potential energy (mgh ) Work done (force × distance moved)

joule (J)

Moment of a force (force × distance)

newton metres (N m)

Power rate of doing work: dW dt

watt (W)

(

)

Momentum (mv )

kg m s−1

Impulse (force × time)

newton seconds (N s)

( ∑ mr ) Angular velocity ( ω = dθ ) dt Density ( mass ) volume Pressure ( force ) area Moment of inertia

pascal (Pa)

Periodic time (time for one complete cycle) Frequency (1 ÷ periodic time)

hertz (Hz)

  Surface tension  force   length 

2 Dimensional analysis

Checklist of learning and understanding • In Mechanics, dimensions describe a quantity in terms of three basic dimensions Mass, Length and Time.

Other dimensions are used in other branches of Mathematics and Science. • Square brackets are used to denote ‘the dimensions of’, for example, [time] = T . • You can only add and subtract terms that have the same dimensions; the resulting sum or difference will

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• • • •

also have the same dimensions. A formula must be dimensionally consistent to be valid. Angles and numerical constants are dimensionless. If two quantities are equal, then they have the same dimensions. You can find the dimensions of a quantity from its definition, from an equation describing it or from its units. Quantities can have units but be dimensionless, for example, radians are dimensionless. You cannot predict units from dimensions as some dimensionless quantities have units. In dimensional calculations, you can give dimensionless quantities the dimensional value 1. You can use dimensional analysis to predict formulae by equating dimensions on both sides of a proposed formula.

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• • • •

A Level Further Mathematics for AQA Mechanics Student Book

Mixed practice 2 1

Given that a , b , h , l and r are lengths and that numerical constants are dimensionless, what could be a formula for volume? Choose from these options. B V = h (a + b) C V = hl (a + b) A V = 2 πrl 2 2

If [ density ] = Mα Lβ Tγ , what is the value of β ? Choose from these options.

A 3

B −3

C −2

State the dimensions of: a 2 π l g

2 b d v2 , where v is an expression for speed. dt

Heron’s (or Hero’s) formula for the area of a triangle with sides of length a, b, and c is A = s ( s − a)( s − b)( s − c ) , where s is half the perimeter. Show, with full explanation, why this formula is dimensionally consistent.

a Tension in a string is a force. What are the dimensions of tension?

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b In each formula, T is the tension in a string, m is a mass, v is a velocity, r is a length and θ is an angle. Which of the formulae is/are dimensionally consistent? If the formula is inconsistent state which term is incorrect. 2 2 ii T − mg cos θ = mv iii T − g cos θ = mv i T − mg cos θ = mv r r r a State the dimensions of potential energy.

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b In the centimetres, grams and seconds (cgs) system a particle has potential energy of 5.2 × 108 ergs. Calculate this in joules.

In a simple harmonic motion of a mass m the restoring force is proportional to the displacement. It can be shown that, at time t , the displacement x and the acceleration a are:   x = A cos  k t   m    a = − k A cos  k t  m  m 

Find the dimensions of: a A

b k.

The radial force on a particle moving in a circle is thought to be of the form F = mα v β r γ . By writing each of the components in term of its dimensions, and equating indices, form three equations to find the values of α , β and γ and hence find the formula for F .

a State the dimensions of force. b Newton’s law of gravitational attraction states that the force of attraction, F , between two bodies of masses m1 and m2 is dependent on the masses, the distance r between them and the constant G and it can be written as F = G α m1β m2γ r δ .

Write down, with reasons, the relationship between β and γ .

c Given that the dimensions of G are M −1L3 T −2, use a dimensional proof to find a formula for F . 44

2 Dimensional analysis 10 a Give the dimensions of angular acceleration. b An equation for oscillations of a damped pendulum of length l displaced by a small angle θ is 2 given by d θ2 + A dθ = −Bθ , where A and B are constants. Given that this equation is dimensionally dt dt consistent, find the dimensions of A. c By expressing B as a product of powers of l and g , find an expression for B in terms of l and g . 11 Surface tension is defined as force per unit length. a State the dimensions of surface tension. b When liquid forms a puddle on a clean horizontal surface, the depth d of the puddle has a maximum value which can be written as d = AS α ρ β g γ , where A is a dimensionless constant, S is surface tension, g is the acceleration due to gravity and ρ is the density of water. Use dimensional analysis to find a formula for d.

12 Tension is a force.

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c Given that d = 5.4 mm when S = 0.073 N m −1, and 1 m 3 of water has a mass of approximately 1000 kg, find the value of A.

a State the dimensions of tension.

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b Frequency, f , has dimension T −1. Mersenne’s law states that the fundamental frequency of a string is of the form f = 1 l α F β µ γ , where 1 is a dimensionless constant, l is the length of the string, F is 2 2 the tension in the string and µ is the mass per unit length of the string. Use dimensional analysis to find the values of α , β and γ and hence find the formula for f .

13 A ball of mass m is travelling vertically downwards with speed u when it hits a horizontal floor. The ball bounces vertically upwards to a height h. It is thought that h depends on m , u , the acceleration due to gravity g , and a dimensionless constant k, such that h = kmα u β g γ , where α , β and γ are constants.

By using dimensional analysis, find the values of α , β and γ . [©AQA 2009]

14 a Pressure is force per unit area. Derive the dimensions of pascals – the units of pressure. b Dynamic viscosity µ is measured in pascal seconds. Derive the dimensions of µ .

c The terminal velocity vT of a small spherical particle, of radius r and density ρ , falling vertically down though a medium of density ρ1 and dynamic viscosity µ , is given by vT = A

r α g β ( ρ − ρ1 ) , µ

where A is a dimensionless constant and g is the acceleration due to gravity. Use dimensional analysis to find the values of α and β . 15 Th e formula for the lifting force F generated on a wing of an aeroplane is of the form F = kρ α v β Aγ , where k is a dimensionless constant, ρ is the air density, v is the air speed and A is the surface area of the wing. Use dimensional analysis to find the values of α , β and γ and hence find the formula for F .

A Level Further Mathematics for AQA Mechanics Student Book 16 The speed, v m s −1, of a wave travelling along the surface of the sea is believed to depend on: the depth of the sea, d m the density of the water, ρ kg m −3 the acceleration due to gravity, g m s −2 and a dimensionless constant, k so that v = kd α ρ β g γ , where α , β and γ are constants. By using dimensional analysis, show that β = 0 and find the values of α and γ . [©AQA 2008] 17 Surface tension, S, is defined as force per unit length. a State the dimensions of S.

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b State the dimensions of density.

c The average height, h, of a liquid in a capillary tube can be written as h = ASρ α r β g γ , where A is a dimensionless constant for the liquid, S is the surface tension, ρ is the density of the liquid, r is the internal radius of the tube and g is the acceleration due to gravity. Use a dimensional argument to find the values of α , β and γ and hence find a formula for h.

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d In this question part use g = 9.8 m s-2, giving your final answer to an appropriate degree of accuracy. 1 m 3 of water has a mass of approximately 1000 kg . Water rises up a vertical capillary tube which has a diameter of 0.3 mm. Given that A = 2 and S = 0.072 N m −1, what is the height of water in the tube, in millimetres?

18 The equation: F =c dαuβ ργ where c is a constant, F is a force, d is a diameter, u is a velocity and ρ is a density is dimensionally consistent. Find the values of α, β and γ and hence find a formula for F.