Engineering Physics Flashcards

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1
Q

Advantages of flywheels

A

They are very efficient

They last a long time without degrading

The recharge time is short

They can react and discharge quickly

They are environmentally friendly (don’t rely on chemicals to store energy)

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2
Q

Disadvantages of flywheels

A

They are much larger and heavier than other methods

The pose a safety risk as the wheel could break apart at high speeds

Energy can be lost through friction

If used in moving objects they can oppose changes in directions which can cause problems for vehicles

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3
Q

Increasing the energy stored in a flywheel

A

Increase the mass - the moment of inertia and hence the stored kinetic energy is directly proportional to mass

Increase the angular speed

Make it spoked - compared to a solid wheel, a spoked wheel of the same mass stores about twice as much energy

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4
Q

Reducing friction in flywheels

A

Flywheels lose energy to friction and air resistance

Lubrication

Levitate it with superconducting magnets - no contact with bearings

Operate them in vacuums or inside sealed cylinders to reduce drag from air resistance

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5
Q

Uses of flywheels - potters wheels

A

Controlled by a pedal so hard to apply a constant force

A flywheel is used to keep the speed of the wheel constant

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6
Q

Uses of flywheels - regenerative braking

A

In regular vehicles, applying the brakes causes the wheels to slow down, generating lots of heat

However, in some vehicles when the brakes are used a flywheel is engaged - charging it up

When the vehicles is ready to accelerate the flywheel can be used to turn the vehicle’s wheels

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7
Q

Uses of flywheels - wind turbines

A

Flywheels can be used to store excess power on windy days or during off-peak and give power on days without wind

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8
Q

Uses of flywheel - power grids

A

When lots of electricity is used in an area, the electricity grid can’t meet the demand

Flywheels can be used to provide the extra energy needed whilst backup power stations are started up

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9
Q

Uses of flywheels - riveting machines

A

An electric motor charges up a flywheel, which then rapidly transfers a burst of power as the machine presses down on the river

Useful as it stops rapid changes in power going through the motor - which could cause a stall

Also a less powerful motor can be used

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10
Q

Flywheels smoothing torque and angular velocity

A

In systems where the force supplied can vary a flywheel can be used to keep the angular velocity of rotating components constant

They deliver stored energy smoothly to the rest of the system

They can also smooth out force exertion by a system

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11
Q

Conservation of angular momentum

A

The angular momentum of a system remains constant unless external torque acts on the system

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12
Q

Isothermal changes

A

Changes that occur at a constant temperature so the internal energy of the gas doesn’t change

So the work done on or by a system is equal to the heat energy supplied

Q = W

Must take place very slowly in order for no energy to be transferred to dU

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13
Q

Adiabatic processes

A

No heat is lost or gained by the system so Q = 0 and dU = -W

So if work is done by the system W will be positive so internal energy will decrease

A change in temperature occurs as the internal energy only depends on temperature

Must take place fast enough that no energy is able to be transferred to the surroundings

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14
Q

Work done and constant pressure

A

For processes where the pressure doesn’t change W = p dV

For expansion the change in volume and the work done are positive

For compression the change in volume and the work done are negative

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15
Q

Work done and constant volume

A

No work is done W = 0 so Q = dU

So by transferring heat energy to he system you only increase its internal energy

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16
Q

P-V curves - isothermal

A

Smooth curve

area under the curve is work done

Curves are called isotherms

Position of isotherm depends on the temperature

Higher the temperature the further from the origin the isotherm will be

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17
Q

Adiabatic p-V diagrams

A

Similar to isotherms but they have a steeper gradient

More work is done to compress gas adiabatically rather than isothermally

Less work is done to expand has adiabatically rather than isothermally

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18
Q

Four stroke engine stages: induction

A

Piston starts at the top of the cylinder and moves down increasing the volume of gas above it

This sucks in a mixture of fuel and air through the open inlet valve

The pressure of the gas in the cylinder remains constant - just below atmospheric pressure

19
Q

Four-stroke engine stages: compression

A

The inlet valve is closed

The piston moves back up the cylinder and does work on the gas, increasing the pressure

Just before the piston is at the end of this stroke, the spark plug creates a spark which ignites the air-fuel mixture

The temperature and pressure suddenly increase at an almost constant volume

20
Q

Four-stroke engine stages: expansion

A

The hot air-fuel mixture expands and does work on the piston, moving it downwards

The work done by the gas as it expands is more than the work done to compress the gas, as it is now at a higher temperature. There is a net output of work

Just before the piston is at the bottom of the stroke, the exhaust valve opens and the pressure reduces

21
Q

Four-stroke engine stages: exhaust

A

Piston moves up the cylinder and the burnt gas leaves through the exhaust valve

The pressure remains almost constant just above atmospheric pressure

22
Q

Four-stroke Diesel engines

A

Undergo the same four strokes as petrol engines

But during the induction stroke only air is pulled into the cylinder, not an air-fuel mixture

Compression stroke - air is compressed to a high enough temperature that it ignites diesel fuel sprayed into the cylinder

For the indicator diagram there isn’t a sharp peak at the start of the expansion stroke - diesel burns it doesn’t explode

23
Q

Assumptions for theoretical models for engine cycles

A

Same gas is taken continuously around the cycle - pure air with adiabatic constant = 1.4

Pressure and temperature changes can be instantaneous

Heat source is external

The engine is frictionless

24
Q

First law of thermodynamics

A

Q = dU + W

Q is energy transferred by heating either to (+) or from (-) the system

dU is the change in internal energy

W is the work done to (-) or by (+) the system

25
Q

Differences between theoretical and real engine diagrams

A

Rounded corners - inlet and exhaust valves take time to open and close

Heating doesn’t take place at a constant volume - pressure and temperature increase isn’t instantaneous

Theoretical model doesn’t include small amount of negative work it assumes the same air cycles around continuously

Area inside the loop is slightly less due to friction

Fuel is never completely burnt - so you can’t get maximum energy out and pressures are higher in theoretical model

Engines have an internal heat source, not an external one - temperature rise isn’t as large in the theoretical model due to the assumption of an external heat source

Heat is lost - not adiabatic, heat is lost to metal surroundings

26
Q

Engine efficiency - mechanical efficiency

A

= brake power/indicated power

27
Q

Engine efficiency - thermal efficiency

A

Thermal efficiency = indicated power/input power

28
Q

Overall engine efficiency

A

Overall efficiency = brake power/input power

29
Q

Second law of thermodynamics applied to engines

A

Heat engines must operate between a heat source and a heat sink (a region which absorbs heat from the engine)

1) Heat energy transferred from the heat source to the engine is Qh
2) Some of this energy is converted into useful work, W
3) But some of this energy (Qc) must be transferred to a heat sink, which has a lower temperature (Tc) than the heat source
4) This means engines can never be 100% efficient

30
Q

CHP plants

A

Engines are very inefficient - lots of heat is is transferred to the surroundings

Combined heat and power plants (CHP) try to limit energy waste by using it for other purposes - e.g. Heating houses and businesses nearby

Markinch Biomass CHP plant in Scotland - excess heat is used to create steam to dry paper in the paper mill

31
Q

Reversed heat engines

A

Operate between hot and cold reservoirs

Direction of energy transfer - heat energy is taken from the cold reservoir and transferred to the hot reservoir

For reversed heat engines sources and sinks are instead called hot and cold spaces

To transfer heat from a colder space to a hotter space work must be done

32
Q

Refrigerators

A

Aims to extract as much heat energy from the cold space as possible for each joule of work done

The cold space is inside the refrigerator whilst the hot space is the room the refrigerator is in

Refrigerators keep enclosed spaces cool that can then be used to store perishable food to keep it fresh for longer

33
Q

Heat pumps

A

Aims to pump as much heat as possible into the hot space per joule of work done

Cold space is usually outdoors and the and the hot space is the inside of the house

Used to heat rooms and water in homes

34
Q

Coefficient of performance

A

A measure of how well the work done is converted into heat transfer

Similar to efficiency but can be above 1

E.g. Heat pump with coefficient of performance of 4 transfers 4J for every 1J of work done

35
Q

Uses of flywheels

A
Potters wheel 
Regenerative braking 
Power grids 
Wind turbines
Riveting machines
Smoothing torque, energy delivery and angular velocity
36
Q

Friction power

Net Torque

A

Indicated power - output power

Applied torque - frictional torque

37
Q

Function of the crankshaft

A

Converts the up and down motion of the piston into rotational motion

38
Q

What would happen to an engine if it didn’t operate between a heat source and a heat sink?

A

The engine will reach the same temperature as the heat source and so no more heat energy will flow

This is why the second law of thermodynamics and its application to heat engines so important

39
Q

Flywheels in crankshaft

A

Flywheel maintains angular momentum, helping to take the crankshaft over dead centres

There is a variation in engine torque due to changes in engine pressure, the flywheel is used to smooth out these changes

The greater the flywheels moment of inertia, the less fluctuations there are in angular velocity over one cycle

Flywheel stores energy when the gas expands, doing work on the piston and uses this energy to compress the gas

40
Q

How do you know if the overall change of internal energy of a cycle is zero?

A

The cycle will return to the same initial temperature

Change in internal energy is only dependent on temperature

41
Q

Unit for angular momentum

A

kg m^2 s^-1

42
Q

Law of conservation of angular momentum

A

Angular momentum of a system remains constant unless acted on by an external torque

43
Q

Flywheel design features to store maximum kinetic energy

A

Put more mass at a greater radius (e.g. make it spoked) - increases moment of inertia, use a thin axle

Use high density materials - larger mass for a given size

Low friction bearings and smooth outer surface

Rotational speed limited due to the tensile strength of the material - due to the centripetal force acting on the material

Needs to be perfectly balanced to avoid any adverse gyroscopic effects

44
Q

How does a heat pump obey the second law of thermodynamics and the law of conservation of energy?

A

Obeys 2nd law of thermodynamics as it operates between hot and cold spaces and work is done to move energy against the temperature gradient.

Obeys law of conservation of energy as although it delivers more energy than is supplied to it this is because the additional energy is the energy transferred from the hot space.