Aircraft - Powerplant Flashcards

1
Q

Boyles Law

A

Pressure and volume inversely proportional.
P x V = constant
Assuming constant temperature

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2
Q

Charles Law

A

Volume and temperature are proportional.
V / T = constant
Assuming constant pressure

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3
Q

Combined Gas Law

A

P x V / T = constant

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4
Q

Bournoulli’s equation

A

Static pressure + dynamic pressure = total pressure (constant)

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5
Q

Newton’s laws

A

1) A body will continue in rest or in uniform motion in straight line, unless acted upon by a force
2) Rate of change of momentum is proportional to (and in direction) of applied force
3) Action and reaction are opposite and equal

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6
Q

Work

A

Force x distance

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7
Q

Power

A

Force x distance / time
[the rate of doing work]

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8
Q

Force

A

Mass x acceleration

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9
Q

Thrust

A

A force based on acceleration and mass of air pushed backwards:
F = M x (V(jet) - V(flight))
Where V(jet) = speed of air existing turbine or propeller
V(flight) = speed of air encountered

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10
Q

Horsepower measurements
- Indicated
- Friction
- Brake
- Thrust

A

Indicated HP - Theoretical reciprocating engine power, based on pressure developed in cylinders, ignoring work done in the engine.
Friction HP - Work done within the engine
Brake HP - Power delivered to the shaft
Thrust HP - Power converted to thrust (brake HP with propeller efficiency)

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11
Q

Piston engine efficiency
- overall
- thermal
- volumetric

A

Overall: 80%
Thermal: 33% (heat lost through exhaust)
Volumetric: 80%

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12
Q

Piston energy type chain

A

Chemical energy ->
Heat energy ->
Pressure energy ->
Mechanical energy

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13
Q

Piston strokes

A

Induction
Compression
Power
Exhaust

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14
Q

Connecting rod

A

Joins piston to crankshaft.
“Small end” at pison
“Big end” at crankshaft

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15
Q

Top dead centre & bottom dead centre

A

Based on piston and combustion chamber at the top and crankshaft & connecting rod at the bottom.
So TDC is small cylinder volume, BDC is max cylinder volume.

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16
Q

Mean Effective Pressure (MEP)

A

The average pressure exerted on the piston during the power stroke.
This determines the theoretical power of the engine.

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17
Q

3 issues with theoretical 4 stroke engine

A

Air has momentum.
At BDC and TDC linear movement of piston is very small despite rotational movement of crankshaft being constant (“area of ineffective crank angle”).
Combustion of fuel and increase in pressure is not instantaneous.

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18
Q

Changes in practical 4 stroke engine based on the issues with theoretical

A

Valve timing
Ignition timing

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19
Q

4 stroke valve timing

A

Both valves lead and lag.
This maximises the amount of mixture that can enter and reduces required valve speeds.
Some loss of power due to exhaust opening before power stroke is complete, but this is minimal due to limited piston movement at BDC.

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20
Q

Valve overlap

A

Lead and lag of the inlet and exhaust valves leads to a period when both are open.
This allows the momentum of exiting exhaust gas to “pull in” new mixture, called scavenging.

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21
Q

Valve timing - fixed or variable?

A

Valve timing is optimised based on the shape of the cam, which is fixed, so valve timing is fixed.
It doesn’t vary with RPM.
[Note: determined in terms of angles, not speed, obviously higher RPM leads to faster physical valve speeds, but same point in the cycle]

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22
Q

4 stroke ignition timing

A

Ignition is “advanced”, so happens before TDC, to ensure that power peaks as piston leaves period of ineffective crank angle.
Timing DOES change based on RPM (unlike valve timing) as combustion delay is fixed, so as the engine gets faster the spark needs to happen earlier to achieve the right timing.

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23
Q

Radial engines

A

Pistons mounted radially around the crank shaft. Need to have an odd number of cylinders to allow timing (e.g. 1, 3, 5, 2, 4).
Creates a big area with a lot of drag, and upside down cylinders have issues with oil pooling.

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24
Q

How is crankshaft supported?

A

On “bearing journals” with shell type bearings

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25
Q

Crank throw

A

This is half of the stroke distance.
It is the range of movement of the connecting rod connection at the crankshaft, between central point (centre of crankshaft) and its TDC or BDC point.
Alternatively could be described as the amplitude of the vertical movement of the crankshaft/connecting rod connection.

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26
Q

Crank throw - considerations around weight

A

Shorter crank throw reduces weight as components can all be smaller.
Thus aircraft engines tend to be “short stroked”.

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27
Q

Camshaft

A

Controls valve timing. Driven via gears by the crankshaft and rotates at half the speed of the crankshaft, so valves each open and close once per cycle.

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28
Q

4 stroke engine materials
- Barrel
- Head
- Pistons
- Crankshaft
- Crankcase
- Valves

A

Barrel - Steel
Head - Alloy
Pistons - Aluminium alloy
Crankshaft - Steel (strong)
Crankcase - Magnesium alloy (light & strong)
Valves - Steel alloy (temp resitant)

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29
Q

Piston engine
- Crankcase

A

Main structural element of engine.
Mounting points to mount to airframe, for accessory gearbox and for cylinders.
Internal passages allow oil to flow and a breather allows air to vent.

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30
Q

Piston engine
- Accessory gearbox

A

Drives oil, ignition, hydraulic, pneumatic systems and sometimes engine starter motor.

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31
Q

Exhaust valve cooling

A

Exhaust valve is hollowed and partly filled with sodium. This melts at high temperature and transfers heat from the valve head to the stem.

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32
Q

Valve bounce

A

Caused when spring closing valve vibrates at its resonant frequency. This prevents the valve from staying gas tight.
Resolved by having two counter wound helical springs (one within the other) holding the valve closed, which have different resonant frequencies.

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33
Q

Valve gear - tappet

A

Fitted between the camshaft and push rod, creates the right clearance to ensure valve movement range is correct.
Has some clearance for thermal expansion so it can fully close when hot, but too much clearance means the valve won’t fully open.

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34
Q

Limitation on normally aspirated engines

A

Engine power limited by the amount of air that enters the cylinders. The greater the mass of air in the cylinder, the more combustive power can be created.
Naturally this is less at higher altitude where outside air pressure is lower.

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35
Q

Manifold Absolute Pressure (MAP)

A

Mixture pressure at inlet manifold just before going into cylinder. Can be measured by a MAP gauge and is a good indicator of MEP and thus engine power.
Controlled by the throttle.

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36
Q

What does MAP gauge show when:
- Engine off
- Engine idle
- Engine full throttle

A

Engine off - shows outside pressure, so 29.92 in Hg at MSL in ISA.
Engine idle - zero
Engine full throttle - Just less than 29.92

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37
Q

Calculating power of piston engine
- MEP method

A

Power = Force x distance / time

Use PLANE
Pressure (MEP) & Area (of piston crown)
Length (Stroke length)
Number of cylinders
Engine (RPM / 2 - only one power stroke per 2 rotations)

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38
Q

Calculating power of piston engine
- Torque method

A

Power = Force x distance / time

Distance x force x rpm
= torque x rpm

Torque measured at the gearbox between engine and propeller

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39
Q

Fixed vs variable pitch propeller engine power monitoring

A

Fixed pitch generally just look at rpm.
Variable pitch power is a function of rpm and manifold pressure, so have a MAP gauge as well as rpm.

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40
Q

Piston engine
- Clearance volume
- Total volume
- Swept volume
- Compression ratio

A

Clearance volume = Volume @ TDC
Total volume = Volume @ BDC
Swept volume = the difference

Compression ratio =
Total volume : Clearance volume

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41
Q

Compression ratio effects

A

High compression ratio improves thermal efficiency, but increases likelihood of detonation.

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42
Q

Squared or square cage engine

A

Piston engine where piston diameter = stroke.

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43
Q

Volumetric efficiency

A

Ratio of mixture induced in cylinder to mass of air (at standard temp/pressure) that would fill the swept volume.
In normally aspirated engine this is affected by the ease of inflow and ease of exhaust flow, along with density of the air.

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44
Q

Effect on volumetric efficiency of:
- Altitude
- RPM

A

Assuming constant MAP (big assumption), volumetric efficiency increases with altitude due to easier exhaust flow.
Also increases with RPM due to increased momentum of gases.

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45
Q

Power at altitude for piston engines

A

Consider variable pitch propeller where MAP and rpm can be controlled
At low altitude throttle is less than full for given MAP, so as you climb volumetric efficiency increases and throttle can be opened to maintain MAP.
When throttle is fully open you are at peak power and above that altitude power will decrease as MAP falls.
Note: MAX power is always decreasing as throttle always full and MAP decreasing with altitude.

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46
Q

Engine oil designations

A

Number indicates viscosity (higher number - higher viscosity).
Letters in front indicate additives.
[New engines run in with zero additive oil to reduce lead in time]

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47
Q

Dry sump oil system

A

Used oil falls into a sump at the bottom of the engine. A scavenge pump (stronger than the main oil pressure pump to prevent pooling in the sump) pumps it through the cooler into the main oil tank (onto a de-aerator plate).

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48
Q

Hot well

A

This is a perforated metal cylinder over the oil tank outlet. When engine started it lets the warmer oil through more easily than the more viscous colder oil. This allows an initial good flow of warm oil before the entire tank is warm.

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49
Q

Oil system filters

A

2 coarse filters fitted before pumps (suction filter before pressure pump, scavenge filter before scavenger pump) to protect the pumps from damage.
A fine pressure filter fitted after pressure pump to protect components, has a bypass valve.

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50
Q

Magnetic plugs

A

AKA chip detectors.
Magnetic parts on oil return lines (from sump pump via scavenger pump to coolers and main oil tank) to extract any bits of metal.

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51
Q

Pressure regulation in oil system

A

Pumps are engine driven and higher pressure than required to ensure they work. Have pressure relief valves fitted in parallel that return oil from outlet to inlet side of pump if pressure is too high.

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52
Q

Oil cooling

A

Might have shutters to allow level of oil cooling to be controlled.
An anti-surge valve allows coolers to be bypassed in case of blockage or excessive cooling causing “oil coring” (congealing in the cooling matrix).

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53
Q

Location of oil cooler in dry and wet sump systems

A

In dry sump cooler is between scavenger pump and the oil tank (in the return line).
In wet pump it is fitted in the supply to the engine.

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54
Q

Impact of oil temperature on oil pressure

A

Cold oil is more viscous and gives higher oil pressure

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55
Q

Impact of low oil quantity on oil pressure

A

Low amount of oil has to do more work so temperature increases. This temperature increase results in reduced oil pressure.

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56
Q

Wet sump system

A

Similar to dry sump but no oil tank, all oil is stored in the sump at bottom of the engine.
Uses “splash lubrication” where crankshaft moving through oil flings it around the engine.

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57
Q

Wet sump disadvantages

A

Sump affected by inverted flight so wet sump can have oil starvation (dry sump has a tank with ready supply).
Splash lubrication at high rpm can cause excessive oiling, plus the splash lubricating oil isn’t filtered or cooled.
Usually need more oil for wet sump.

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58
Q

Checking oil level dry vs wet sump

A

Oil level in dry sump needs to be checked after flight as some will drain back to sump.
Wet sump wait until cooled.

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59
Q

Hydraulicing

A

When oil pools in inverted cylinders (inverted or radial engines) and causes damage when engine starts as it is not compressible.
Need to remove spark plugs to drain and start with a manual cranking to check.

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60
Q

Cylinder Head Temperature (CHT)

A

Hottest part of the engine so useful to measure. Usually measure the hottest cylinder (last one, with worst air cooling).

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61
Q

Functions of engine oil

A

Lubrication
Cooling
Cleaning
Protection
& HYDRAULIC operations

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62
Q

Magneto system description

A

Engine drives a rotating magnet within a U-shaped stator, with primary (few, thick) and secondary (many, thin) windings around it. This generates an AC current.
The primary winding low tension (LT) circuit is regularly broken, which induces a pulse in the secondary winding high tension (HT) circuit.
Large number of secondary windings means high voltage, which is distributed to a spark plug by the distributor.
NOTE: Tension = Voltage

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63
Q

Prevention of arcing in the magneto system

A

Arcing can occur at the breaker points in the low tension circuit when the circuit is broken due to high induced current.
A capacitor is installed parallel with the contact breaker to prevent this (called a condenser) which also assists in breaking of the primary circuit.
Capacitor in magneto circuit PREVENTS ARCING.

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64
Q

Ignition system & magnetos

A

Works opposite to normal system. In normal operation the ignition switches are open, so the LT breaker controls the primary windings. When a magneto ignition switch is grounded, the primary coil is connected to earth so the breaker does nothing and the magneto fails.
As a result of this a break in the ignition wiring will result in permanent ignition firing, not a failure of ignition.
So NOT fail safe on the ground.

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65
Q

Reference to ignition switching system

A

This is what is activated when you turn the key to magneto 1 or magneto 2.
So its action is to connect the primary system to earth.
In this sense in the “dual” setting the ignition switch system is considered disactivated, not activated.

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66
Q

Pressurised magnetos

A

Magnetos use insulating property of air to isolate components. So at high altitudes may need to be pressurised to prevent arcing.

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67
Q

Spark plug augmentation

A

Need sufficient voltage even at low rpm. Gearbox can do this at low rpm (idle) but need extra help at startup:
i) Impulse magneto has a spring-loaded clutch that stores energy and releases it (twice per engine revolution)
ii) HT Booster coil supplies a high voltage directly to the distributor, by powering primary coil with battery and collapsing it with a trembler interrupter.
iii) LT Booster coil uses aircraft battery directly to power the primary coil.

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68
Q

Spark plug retardation

A

The 3 augmentation methods (impulse magneto, HT booster, LT booster) all have methods for retarding ignition during starting to prevent sparking too far ahead of TDC which would damage engine.

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69
Q

Detonation

A

AKA knocking
Rapid spontaneous combustion of mixture after burning has begun (i.e. after ignition). Flame rate about 1000ft per second instead of 60 to 80ft.
Energy produced is given up as heat and shock rather than piston movement.
Occurs AFTER normal ignition.

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70
Q

Pre-ignition

A

When mixture ignites before the spark.
Can cause engine to “run on”, which is continuing to run after ignition is switched off.
Unlike detonation, this gets WORSE with higher rpm.

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71
Q

Octane rating

A

Characteristic of fuel indicated anti-knock value. Above 100 it is a “performance rating”.
Based on the anti-knock qualities of a mix of X% iso-octane and (100-X)% heptane.
It is ok to temporarily run with fuel of a higher rating, but NEVER with a lower rating.

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72
Q

Fuel additives

A

Tetra-ethyl lead the most popular additive, which improves anti-knock capability.
100LL achieves same anti-knock as 100, but with lower amount of lead. 100LL has blue colour (100 is green).

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73
Q

Factors influencing detonation

A

Increased temperature or pressure of mixture increases risk of detonation.
- Carb heat on with higher power;
- High power & low rpm
- Overheated cylinders

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74
Q

Impact of carb heat on mixture

A

Air less dense so rich mixture.

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75
Q

Stoichiometric mixture

A

Chemically correct mixture which achieves complete combustion, 15:1 by mass.

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76
Q

Typical range of mixture

A

8:1 - rich
20:1 - lean

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77
Q

Appropriate mixture settings

A

At 15:1 (stoichiometric) high risk of detonation due to excess latent heat.
10% rich will absorb this heat, but use 15% in practice to ensure all cylinders are ok.
At high power settings use 20% rich.
Take-off use 30% rich.

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78
Q

Effect of lean mixture on temperatures

A

Less fuel means the gas burns cooler, however it also burns slower so more heat is transferred to the engine.
- Low gas burn temp
- High cylinder head temp
- Low exhaust gas temp

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79
Q

Other issues with mixture settings
- Popping back
- Idling

A

Lean mixture can lead to “popping back” when mixture is burning when the inlet valve opens.
At low (idling) rpm exhaust gas momentum is reduced so retention of some exhaust gas dilutes the mixture. So need rich mixture at idle.
However, prolonged idling with rich mixture (e.g. on the ground) causes spark plug fouling.

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80
Q

Fuel volatility

A

This is readiness to vaporise.
We need fuel to vaporise in the mixture to enable combustion, but not in the fuel tanks or lines.

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81
Q

Gravity feed ceiling

A

More likely in jet craft, this is a ceiling for use of gravity feed of fuel.
Climbing without the positive pressure from a fuel pump can lead to “foaming”, the vaporising of fuel in lines due to the decrease in air pressure.

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82
Q

Vane type fuel pump

A

Two double ended vanes split circular housing into 4 segments. They rotate and also slide across each other so segments change in size. Segments large at inlet and small at outlet so pressure changes create the flow.

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83
Q

Basic float carburettor

A

Float in the carburettor operates a needle valve that cuts of fuel supply at a certain level (fuel delivered under pressure from fuel tanks).
Exits via a u-bend through a “jet” narrowing that controls flow, then further through an exit at the choke/throat venturi part of carburettor, before the throttle.
Venturi effect as air flows past fuel outlet causes fuel to be sucked out.

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84
Q

Throttle effect

A

Throttle controls the amount of air (air meaning air & fuel mixture) allowed through by the butterfly valve.
The higher the flow of air, the greater the venturi effect and so the more fuel is extracted to maintain the right ratio.

85
Q

Pressure balance duct

A

At high air speed pressure increases in carb throat due to ram air, thus reducing amount of fuel drawn out. Conversely at high altitude lower density of air would en-richen the mixture.
Therefore a pressure balance duct joins the fuel float chamber to the carb intake to ensure correct mix ratio across AIRSPEEDS and FLIGHT CONDITIONS.

86
Q

Diffuser

A

This is a perforated piece sitting after the jet in the tube from the carb fuel chamber to the nozzle. It has a pressure connection after it to the fuel chamber which adjusts rate of fuel flow to ensure correct mixture ratio across ENGINE SPEEDS.
Required as fuel flow from nozzle isn’t linear with engine power otherwise.
ALSO helps atomise fuel

87
Q

Mixture control - functionality and purpose

A

Can function in a variety of ways.
Purpose is to adjust mixture to take account of air density and also to reduce fuel consumption.

88
Q

Slow running jet

A

This is an outlet positioned by the throttle butterfly valve when almost closed to deliver a rich supply at idle. It has an idle-cut out that closes it to allow the engine to shut down.

89
Q

Power enrichment

A

Provides additional fuel for rich mixture required at high power settings (to provide cooling at high power settings).
Can be provided via a variable size main jet, or a separate power jet controlled via a cam connected to the throttle controls.

90
Q

Accelerator pump

A

Connected to the throttle, provides an injection of fuel into the venturi when throttle is opened, to prevent weak or lean cut.

91
Q

Direct vs indirect fuel injection

A

Direct injection delivers fuel directly to cylinder heads. Highly fuel efficient but requires complex timing.
Indirect delivers fuel on low pressure, continuous flow basis to the air intake of each cylinder.

92
Q

Indirect fuel injection system

A

Have both engine driven pump and electric pump (for redundancy and starting) delivering fuel to “fuel control unit”. Deliver at higher pressure than needed with PRV in parallel and reverse to control pressure.
Fuel control unit first metered by mixture control, then throttle (which is linked to the butterfly valve mechanically).
Then delivered to a manifold which splits it to the multiple injectors. Injectors help vaporise and also enable engine cut off.

93
Q

Exhaust Gas Temperature (EGT)
- How it is used

A

This gauge is used to adjust mixture. 15:1 creates highest temperature, richer than this and extra fuel aids cooling, leaner and there is less fuel to burn.

94
Q

Setting power cruise and economy cruise

A

Power cruise: Find peak EGT then enrichen until it falls a bit, should be at about 12:1.
Economy cruise: Find peak EGT then lean until it falls a bit, should be at about 17:1.

NOTE: Only works in the cruise, doing this at higher power settings can cause detonation.

95
Q

Ground boosted vs altitude boosted superchargers

A

Ground boosted supercharges increase horsepower on the ground. Engine needs to be stronger to withstand extra pressure.
Altitude boosted aim to maintain sea level power as the aircraft climbs.

96
Q

Power vs altitude for ground boosted supercharger

A
97
Q

Power vs altitude for altitude boosted supercharger

A
98
Q

2 unexpected features of power vs altitude relationship for altitude boosted supercharger

A

1) Take off power can be boosted significantly above cruise level for 5 mins
2) Power climbs initially up to the rated altitude (unlike normally aspirated or ground boosted which always reduce with altitude). This is due to exhaust back pressure reducing with altitude, improving scavenging.

99
Q

Full throttle height chart

A
100
Q

Full throttle heights

A

For altitude boosted superchargers.
Rated altitude is the point at which full throttle is reached for maximum cruise MAP, after this power starts to fall.
If MAP is lower (i.e. lower rpm) the entire power curve is lower, but full throttle not reached until a greater height.

101
Q

Components of a centrifugal impeller/compressor

A
102
Q

How centrifugal impellers/compressors work

A

Fast spinning (40,000rpm) impeller gives velocity, pressure and temperature to the air. Centrifugal force pushes it to the outsides to the channels of the diffuser, which trade some of the airs kinetic energy for pressure energy.
Pressurised air then ducted to an inlet or another impeller.
The impeller and diffuser each contribute about half the rise in pressure.

103
Q

Turbocharger

A

Hot exhaust gases used to drive a turbine, which drives the compressor.
The compressor can only be used to compress pure air, unlike supercharger which can compress fuel/air mixture.
This is due to high exhaust gas temperatures, which could ignite the mixture.

104
Q

Turbocharger
- Advantages & disadvantages

A

+ No power taken from the engine
+ Less complex and lighter than supercharger
+ As engine rpm increases, exhaust gases increase and so does the boost

  • Turbo lag
105
Q

Controlling turbocharger output
- Simple system

A

Simple systems just have a PRV and “over-boost” warning light when activated.

106
Q

Controlling turbocharger output
- Single controller, waste gate

A

“Waste gate” (which redirects exhaust gas to waste when open) is operated by a “waste gate actuator” (hydraulic - engine oil).
Engine oil flows past the actuator, but a needle valve downstream can be closed by an aneroid capsule if pressure in the carburettor is too low (open throttle, low turbocharger output).
Hydraulic pressure now builds up in the actuator which closes the waste gate, so all exhaust air now directed to the turbocharger.
Time taken for this process is turbo lag.

107
Q

Critical altitude

A

Attribute of turbocharged engine.
This is the altitude at which throttle is fully open and engine is producing maximum amount of power.
Beyond this point exhaust back pressure will reduce power available (due to all exhaust being directed to the turbine).

108
Q

Turbo & waste gate during phases of flight

A

Startup: Waste gate held open by spring (natural position)
Idle: Low manifold pressure causes waste gate to partially close, but little exhaust gas so less than full turbo power
Takeoff: Partially open
Climb: Waste gate gradually closes, turbine speed increases
Critical altitude: Waste gate fully closed, turbine at max speed.
Beyond critical altitude: Waste gate fully closed, compressor outlet pressure can’t be maintained, MAP falls.

109
Q

Dual Pressure Control Unit System

A

An extra turbocharger control system designed to balance pressure on each side of the throttle butterfly valve. Without this, the standard turbo control system gives excess output at low MAP settings (and “bootstrapping”).
Pressure feeds from each side of the throttle affect a diaphragm, which controls a bleed valve that is linked to the waste gate actuator.

110
Q

Intercooler

A

Heat exchanger at the inlet manifold which exchanges high temperature heat of turbo compressed air with colder ram air.
Reduces risk of detonation due to high temperature compressed air being used in the engine.

111
Q

FADEC

A

Full Authority Digital Engine Control
A computer controls the various power settings (throttle, mixture, cowl flaps, ignition) through a single lever.

112
Q

FADEC components

A
  • Electronic Engine Controller (EEC)
  • Fuel Metering Unit (FMU)
113
Q

FADEC safety

A

Critical system so needs dual electronic control units (redundancy) and its own independent backup power system (permanent magnet alternator or battery with longer endurance than the aircraft).
Described as SINGLE FAULT TOLERANT, one failed data input is acceptable.

114
Q

External vs internal supercharger

A

Internal - supercharger, engine driven
External - turbocharger, exhaust driven

115
Q

Diesel vs petrol engine differences

A

No spark plugs (compression ignition).
So need higher compression ratios (14:1 to 28:1 compared to 9:1 petrol).
This requires a strong (and thus heavy) engine.
Need direct fuel injection, no carburettor.
Hotter, so need liquid cooling usually.

116
Q

Diesel vs petrol fuel

A

Diesel (kerosene) is heavier (SG 0.8 to 0.9) and has more controlled detonation at high compression.
Less volatile and higher flashpoint so safer and more stable.
Poor lubricant however.

117
Q

Diesel vs petrol OTTO cycle differences

A

Induction introduces only air to the system.
Fuel is not introduced at the same time so compression compresses only the air.
Fuel introduced at TDC as the big pressure and temperature increase would cause it to ignite too early otherwise.

118
Q

Diesel engines
- Direct fuel injection

A

Similar to petrol fuel injection.
Engine and electric pumps with PRV deliver pressurised fuel to a control unit.
The control unit knows throttle setting and rpm and delivers pulses of fuel to a manifold, which distributes it to individual injectors (simple mechanical injectors that deliver fuel based on pressure received).
[Older system]

119
Q

Diesel engines
- Common rail injection

A

Supply pump provides pressurised fuel to a common rail. The common rail feeds fuel to individual solenoid injectors, which themselves control when and how much fuel is injected.
An electronic control unit controls both the pressure in the common rail and the individual solenoid injectors.

120
Q

Diesel engine fuel injection high or low pressure?

A

High pressure

121
Q

Glow plugs
- Description
- 2 types

A

Heat injected fuel so that ignition occurs in low temperatures. Will activate a light in cockpit when working.
1) Sheathed: Electrical coil in a magnesium oxide powder sheath which protects from vibration and damage.
2) Ceramic: High melting point element in silicon nitrite case. Quick conductor and heat resistant.

122
Q

Variable pitch propellers
RPM or MAP first when:
- increasing power
- decreasing power

A

RPM then MAP to increase power (to prevent detonation)
MAP then RPM to decrease power

123
Q

Gas turbine cycle

A
  • Compression
  • Combustion
  • Expansion
  • Exhaust
    Called OTTO if steps happen separately, Brayton cycle if they happen continuously.
124
Q

Pressure thrust

A

An additional component of jet thrust based on increase in pressure ONLY when propelling nozzle is CHOKED (i.e. at exit velocity limit).
Pressure thrust = A x (rho - P0)

A: nozzle area
rho: nozzle static pressure
P0: atmospheric pressure

125
Q

Total jet thrust

A

Thrust = M x (V(jet) - V(flight)) +
A x (rho - P0)

or velocity thrust + pressure thrust

126
Q

Thrust vs power

A

Power = force x speed, or rate of doing work
Power at start of take off roll is zero and increases with speed.
Thrust can be considered to remain constant across the whole of the speed range.

127
Q

Flat rated engine

A

Jet engines produce more power when temperatures are low and safety limits might be breached in cold air.
Flat rated engines have fuel flow limitations for temperatures below ISA+15C to stay within safety limits.

128
Q

Jet engine thermal efficiency

A

Conversion of thermal energy to kinetic energy
30%

129
Q

Jet engine propulsive efficiency

A

Work done / (work done + work wasted in the exhaust)
Low for jet engines at low speed, where propeller craft are better. However prop craft peak in efficiency as speed increases, whilst jets have continued increase in efficiency up to 80-90%.

130
Q

Single Spool Axial Flow Turbojet

A

Single spool means single shaft connecting turbine blades to compressor blades (multiple of each).
Axial flow means flow straight through the jet engine.
This is slim, low air mass and high velocity. Low drag (good for fast flight) but not used by airliners as it is noisy and inefficient at cruise speed.

131
Q

Twin Spool Bypass Turbojet

A

Two shafts, connecting LP (low pressure) compressor (at front) to LP turbine (at back), and HP compressor & turbine (in-between). LP compressor feeds some air to a bypass outside the combustion/turbine zone. This is more thermally efficient (no combustion) and better at low speeds. It insulates some of the noise of the core.
Core can be smaller so less weight.
Bypass ratio = Bypass air mass:core air mass.
Produces MORE pressure than single spool.

132
Q

Triple Spool High Bypass Ratio Turbo Fan

A

Have a third intermediate compressor & turbine in the middle on a third shaft, inside the core along with the HP compressor/turbine and LP turbine.
High bypass ratios with most power delivered by the large LP fan at the front.

133
Q

Turbo-prop engines

A

Use high efficiency of continuous combustion of gas turbine engines to drive propeller shaft (propellers more efficient at mid altitudes and <300kt).
Need a gearbox as turbine shaft speeds are faster than desired propeller rpm.
Most exhaust temperature used to rotate turbine, but some jet thrust used.
Equivalent shaft horse power = Shaft HP + Jet thrust

134
Q

Free Turbine Engines

A

Twin-spool turbo prop engines which separate the LP turbine from the HP turbine, allowing propeller shaft speed to be disconnected from HP part of engine.
Reduces pressure on start up and improves power generation.

135
Q

Subsonic turbine engine inlet

A

Called “pitot” intake. Lip to prevent turbulence of air entering compressor, even in crosswinds. Convergent throat then divergent diffuser to increase pressure into compressor.
Smooth profile to minimise turbulence.
In strong crosswinds (startup, takeoff run, sev. turbulence) can get surge or flameout (or hot/hung start).

136
Q

Supersonic turbine engine inlet

A

Pitot intake creates high speed air which can cause issues occasionally with subsonic, but will certainly cause shockwave in supersonic. Engines can’t cope with this.
Use a “multi-shock” inlet with small shockwaves, or variable throat, to slow down airflow without increasing drag.

137
Q

Compressor pressure ratio

A

Absolute output compressor delivery (output) pressure / absolute compressor inlet pressure.
This is the measure of performance of a compressor.

138
Q

Centrifugal vs axial flow compressor

A

Can have double sided centrifugal compressor, but difficult to have multiple stages due to energy loss of passing air to the next stage, so axial more popular.
One disadvantage of axial however is that the rotors are aerofoils and can stall, whilst centrifugal aren’t aerofoils, just directing air outwards to the diffuser.
Compression ratio around 4.5:1 for centrifugal, 35:1 for axial.
Centrifugal can be shorter though, so good for APU, although need big inlet.

139
Q

Axial flow compressor
- functionality

A

Each stage has rotor blades and a set of stator blades. Stator blades convert the kinetic energy to pressure and also fix the aerofoil downwash effect from rotor blades ready for the next stage.
So pressure and temperature increase through the stages whilst velocity stays steady.
Pressure increases around 10-20% each stage.

140
Q

Axial flow compressor
- shape of compressor section

A

Need to oppose the force of high pressure further back pushing towards low pressure at front of engine.
Use a convergent duct shape called “air annulus”. The outer case size tapers whilst the shaft size increases so rotor size squeezed from both directions.

141
Q

Compressor
- stagger angle

A

This is the “twist” in the rotor blades of a compressor to manage the difference in velocity of air at the tip of the blades compared to the root.

142
Q

Axial compressor safety margin

A

Stalling of the axial compressor rotors can lead to a flow breakdown (surge) or reversal of airflow (deep surge).
Chart of pressure ratio to air mass flow shows a “working line” which is separated by a safety margin from a “stability line”, beyond which is the “unstable area”.
“Acceleration line” may sit between the two.
Note that the safety margin is much smaller with low air mass flow.

143
Q

Axial compressor safety margin chart

A
144
Q

Axial compressor
- Variable inlet guide vanes & variable stator vanes

A

Variable inlet guide vanes adjust flow to the first stage to ensure it hits rotors at an appropriate angle of attack - essential during startup.
Variable stator vanes can do the same thing for later stages.

145
Q

Axial compressor
- Inter-stage bleed

A

This lets some air flow past earlier stages through to later stages. They open during start up to reduce angles of attack in early stages and maintain axial flow through all stages.
They INCREASE flow over early stages and REDUCE flow over later stages.

146
Q

Compressor stall symptoms

A
  • High EGT
  • Reduced thrust
  • Rumbling or banging from compressor
  • Fluctuating rpm & fuel flow
147
Q

Compressor surge

A

This is when pressure in combustion chamber exceeds compressor pressure and hot gases move forwards. Oscillating pattern between stalled/unstalled compressor causes a loud “burble”.
In deep surge combustion gases flow all the way into compressor, which can be caused by over-fuelling, but less common now with better engine controls.

148
Q

Centrifugal compressor stall/surge

A

Centrifugal compressor doesn’t experience aerodynamic stall, but severe intake icing, impeller damage or over-fuelling can still cause surge and loss of power.

149
Q

Axial flow blade construction

A

Blades are loosely fitted with a “fir tree root” which allows them to adjust based on balance of forces on them (e.g. centrifugal). Causes a tinkling sound when windmilling on the ground.
Blades can have a “snubber” or “clapper” in the middle to PREVENT AERODYNAMIC INSTABILITY, but wide chord blades don’t need this.

150
Q

Typical combustion chamber efficiency

A

Up to 98%.

151
Q

Turbine Combustor
- Functionality up to primary zone

A

Consists of inner “flame tube” and outer “air casing”.
150m/s air from last compressor stage is straightened by stators then diffuser converts more kinetic to pressure to reach 110m/s.
20% of air is “primary air” directed to flame tube, rest is “secondary air” to the outside.
110m/s still too fast for 3m/s kerosene flame rate so gets swirled in the primary zone of flame tube to slow down.

152
Q

Turbine Combustor
- Combustion in primary zone to exhaust

A

Fuel injector sprays fuel which atomises in turbulent air. Igniter provides initial spark but stops once engine started.
No detonation as pressure is constant so use 15:1 stoichiometric ratio (based on primary air) which produces very hot 2100C.
Secondary air added in the secondary zone and dilution zone to reduce temperatures to 1000 to 1500C which turbines can withstand.

153
Q

Combustor designs

A

Multiple combustion chamber systems have several separate chambers.
Tubo-annular combustion chambers have several flame tubes in a common air casing - lighter, more compact, easier maintenance.
Annular chambers have just one flame tube, which is shorter, stiffer, lighter and more even thermal output. However manufacturing and maintenance can be tricky.

154
Q

Combustion chamber drain valves

A

All have them to remove unburnt fuel

155
Q

Reverse flow annular combustor

A

Air flow from the compressor is directed back around the combustion chamber and enters it from the rear. Some loss of efficiency, but it allows the compressor and combustion chamber to be closer together, so smaller.
Good for helicopters & small turbo-prop.
[Has a VAPORISER facing opposite way to air flow]

156
Q

Turbine Fuel spray nozzle types

A

1) Pressure Jet Injector
Either simplex which delivers single spray of high pressure fuel (not good at low rpm) or duplex with two orifices (to cover high & low rpm).
2) Air spray injector
Compressor air enters inner and outer swirl chambers and fuel injected in-between. Finely atomised spray with improved combustion.

157
Q

Fuel vaporiser

A

Alternative to fuel spray nozzles.
U-shaped tube with holes in it that distributes fuel to combustion chamber. Not used often.

158
Q

Types of jet igniter

A

High energy AC: 25,000V high energy ignition unit (HEIU) delivers 60-100 sparks per minute.
Surface discharge: 2000v, iridium electrode and silicon carbide semi-conducter.
DC: Need a vibrator or tumbler to feed pulsed DC to a step-up transformer.

159
Q

Continuous ignition

A

Can be used on take-off from wet runway or flight through heavy rain.
Ignition continues (at low power setting) even though flame already present, to prevent flame out.

160
Q

Turbine blade operation

A

Nozzle Guide Vanes (NGVs) (stators) direct airflow from combustion chamber on to rotor blades. 2 types of forces used:
1) Impulse - NGVs are convergent, accelerate the gas (-VE pres., +VE vel.) and U shaped rotor blades are driven
2) Reaction - NGVs don’t need to be convergent but direct the gas to reaction blades in a different direction, which creates a reaction force.
In reality a combination of the two is used.
Turbine blades have a twist to equalise velocity along the blade.
NOTE: No aerodynamic force, no stall.

161
Q

Turbine blade lifetime

A

Extreme heat causes them to increase in size over lifetime, which gives them a life limit. Called “blade creep”.

162
Q

Turbine blade cooling methods (3)

A

Convective: Void inside the blades allows heat to pass out via convection through vents.
Impingement: Jets of cool air blown onto internal blade surfaces and exit through holes in the trailing edge.
Film: Cool air blown inside the blades which exits through holes on the surface, creating a cooling “film” over the blade surface.

163
Q

Active Clearance Control

A

This is controlling the turbine blade tip clearance by controlling bleed air onto the turbine casing. The internal circumference can be finely controlled this way.

164
Q

Effect of taking bleed air from compressor (e.g. for anti-icing).

A

Lower mass flow
Reduced thrust
INCREASED turbine temperature

165
Q

Jet exhaust design
- exhaust cone

A

Gas enters from turbine at 370m/s, which would cause a lot of energy loss to friction. So an “exhaust cone” in centre creates a divergent duct, converting velocity to pressure energy and keeping hot air from hanging around last turbine stage.
Rear struts holding the cone straighten the flow.

166
Q

Jet exhaust design
- propelling nozzle

A

Gas held at about 290 m/s (mach 0.5 relative to exhaust system) until the propelling nozzle, which is a convergent duct and accelerates air to mach 1.0.
At mach 1.0 the nozzle is “choked” and thrust is capped, but increase in static pressure at exhaust relative to atmospheric pressure creates an additional pressure thrust.

167
Q

Jet exhaust design
- convergent divergent nozzle

A

Attempts to increase thrust by increasing pressure differential at the exhaust (divergence) rather than just using convergence to reach maximum momentum thrust.

168
Q

Low bypass vs high bypass exhaust

A

Low bypass usually mix the two air streams in the same exhaust.
High bypass will have separation co-axial nozzles.

169
Q

Exhaust noise suppression

A

Medium bypass can have mixer chutes which combine the high and low pressure cases to limit noise.
High bypass allow the outer low pressure air to sheath the noisier high velocity central air.
Turbo jet engines can have lengthened jet pipes called “exhaust hush kits”.

170
Q

Reverse thrust

A

Clamshell doors and bucket systems both redirect the core turbine exhaust air forwards for reverse thrust.
Cold stream reversal systems redirect the bypass air forwards. Less powerful as low pressure air can’t be turned through as great an angle.
Can cause surging and structural damage if used at the wrong time, so MULTIPLE interlocks are essential (e.g. on the ground, idle thrust).

171
Q

Auxiliary gearbox

A

Connects jet engine to powered systems and starter motor.
Starter motor must be connected to HP spool.
Non-essential components connected via “quill shaft” or “shear neck”, weak point that breaks if component seizes to prevent excess load on gearbox & drive system.
Fuel and oil pumps are essential so no quill shaft.

172
Q

Main bearing housing

A

Bearings (i.e. ball bearings) are the major jet moving parts, so important for oil. Temperatures are hot so rubber seals no good, use “labyrinth” seals instead which use high pressure air and a groove & thread system to prevent oil escaping. Pressure controlled with venting.
Results in highly aerated oil which must be separated centrifugally.

173
Q

Gas Turbine Oil pressure relief

A

Older system had a typical pressure relief valve arrangement to limit oil pressure.
Modern engines need higher pressure though, especially for bearings mounted at high level. Thus use “full flow” oil system instead, where higher engine rpm results in higher oil pressure.

174
Q

Gas Turbine Engine Oil types

A

Need low viscosity oil.
Temp ranges are high (-40 to +250C) because rotational speeds are high, but no reciprocating parts. At high altitude temperatures can fall so need low viscosity to maintain flow.

175
Q

Main uses of internal bleed air

A
  • Engine anti-icing
  • Internal engine & accessory cooling
  • Bearing chamber sealing (labyrinth seals)
  • Keeping hot air out of turbine blade cavities
    [Internal means uses for within the engine itself, external is for other parts of the aircraft]
176
Q

Fuel Oil Heat Exchangers (FOHE) or
Fuel Cooled Oil Coolers (FCOC)

A

Exchange oil heat with cool fuel to prevent fuel waxing and help cool oil (before main ram air cooling of oil).
Oil pressure usually higher than fuel pressure as oil in fuel is less of a problem than fuel get into hot parts of the engine where it shouldn’t be!

177
Q

Jet engine starting procedure

A

Starter motor drives HP spool (N2) initially. At 15% rpm fuel HP shut-off valve is opened and fuel enters to start combustion.
Starter continues to help until self-supporting speed (30% rpm), at which point starter and igniter drop out.
Engine accelerates up to idle speed of 60% N2 (25% N1).

178
Q

2 types of jet starter motor

A

Electric (DC!)
Pneumatic (often as a backup, using air from a running engine or APU)

179
Q

Jet engine malfunctions

A

Nil rotation
Dry start - Low EGT, no fuel flow
Hung start - (Caused by weaker starter motor) - Low rpm (20%), low fuel flow, high EGT
Hot start - (Caused by overfuel, maybe previous failed start) - V. high EGT
Wet start - (Failed ignition) - low rpm, low EGT, some fuel flow

180
Q

Dry running engine

A

After a wet start, need to clear fuel from the engine. Close fuel HP shut-off valve, switch off igniters, run engines with starters to blow fuel out.
Without this get flames bursting out of back of engines!

181
Q

Maximum re-light altitude

A

May be an altitude limit for re-lighting engines to ensure sufficient air mass flowing through engines.

182
Q

Exhaust Pressure Ratio

A

Alternative indication to N1 for engine thrust.
= Exhaust pressure / compressor inlet pressure
Can give over-read if inlet is blocked, very dangerous, check N1.

183
Q

APU design

A

Need air flow so either a permanent source or doors that open if it is required.
Run at a constant speed so 3-phase AC can be powered without a CSDU.
Might have altitude restriction for starting (25000ft) but can operate to higher altitude (40000ft).

184
Q

Temperature, Pressure and Velocity in Divergent and Convergent Ducts

A

Divergent: + Pressure, + Temp, - Velocity
Convergent: - Pressure, - Temp, + Velocity

185
Q

Jet fuel flow adjusted in relation to which factors?

A

Compressor inlet pressure (NOT compressor outlet pressure).
So forward speed & ambient air pressure.

186
Q

Engine vibration indications

A

Filtered to remove unwanted frequencies

187
Q

Electric circuit connections of multiple thermocouples

A

Connected in parallel

188
Q

Pusher vs tractor propellers

A

Tractor pull the aircraft (e.g. normal single propeller plane), pusher look backwards and push the aircraft forwards.

189
Q

Propeller reduction gearboxes

A

Necessary for turboprop engines which produce 10,000 to 15,000 rpm. Use “epicyclic” gears to transmit torque whilst reducing rpm.

190
Q

Optimal angle of attack for prop blades

A

4 degrees

191
Q

Forces on propeller

A

Total reaction acts perpendicular to the “thrust face” of the blade.
Broken into 2 components:
- Torque: i.e. prop torque, which opposes engine torque in the plane of rotation
- Thrust: at 90 degrees to the plane of rotation of the blade

192
Q

Blade twist and thickness

A

Need bigger angle of attack at the root, and also thicker blade - for additional aerodynamic assistance and also to account for larger forces at the root.

193
Q

Variable pitch prop positions

A
194
Q

Variable pitch prop alpha and beta ranges

A

Divided by the flight fine pitch stop.
Alpha is the coarse side of this, i.e. flight range and feathered.
Beta is the fine side of this, i.e. taxy and reverse.
Divide at FFP is important as fining beyond this (into beta range) during flight can cause loss of control.

195
Q

Forces acting to turn prop blades

A

Aerodynamic Twisting Moment (ATM) on the blade isn’t in line with the axis, it acts to COARSEN the pitch.
Centrifugal Twisting Moment (CTM) opposes this (FINING the pitch) and is stronger.
Thus it is more difficult to coarsen than fine the blade.

196
Q

Windmilling (ATM & CTM)

A

Reaction force on blades when windmilling becomes drag (reverses direction) so ATM acts with CTM to fine the blades.
This is ok on single prop as it acts to maintain rotation and aid restart, but creates asymmetric drag on multi-engine so need a feathering mechanism.

197
Q

Pitch Control Unit (PCU)

A

Combination of:
- Pitch Control Mechanism (PCM)
- Constant Speed Unit (CSU)

198
Q

Pitch Control Mechanisms (PCM)

A

2 types.
Double acting have a hydraulic (engine oil or hydraulic system) cylinder with controls in both directions.
Single acting use a counterweight and hydraulic control only acts in the direction to oppose the counterweight. Counterweight uses centrifugal force so no effect when prop is stationary.

199
Q

Single acting PCM for single and multi engine

A

Multi engine have spring and counterweight acting to coarsen, so hydraulic failure leads to feathered blade for low drag.
Single engine have weak spring to fine and counterweights to coarsen. If hydraulics fail with engine on, counterweights will coarsen. But if the engine stops (rpm slows down) the counterweight stops working and the spring will fine the blade to allow restart.

200
Q

Centrifugal latch

A

AKA “Low Pitch Stop”
Multi engine PCM would act to fully feather blade at engine stop, which is bad for starting. So a centrifugal latch engages at low speed to lock the pitch in fine position.
Need to take care in engine failure situation to lock coarse pitch (feather) in before rpm degrades and the lock engages.

201
Q

Constant Speed Unit (CSU)

A

Acts to maintain the rpm selected by pilot by coarsening if rpm rises and fining if rpm falls.

202
Q

CSU functionality

A

A hydraulic spool (or “landed”) valve direct engine driven hydraulic force to either a coarsen, fine or neutral position.
It is connected to a spring which is opposed by flyweights that are subject to centrifugal force with rpm.
High rpm (overspeed) leads to the flyweights exerting force over the spring and moving the landed valve to coarsen position, which feeds the PCM.
Pilot rpm selection affects the spring compression.

203
Q

Feathering

A

Unless you have a free power turbine turbo-prop, need to stop the engine before feathering to prevent excess forces.
Pull back rpm lever through coarsen to feather.
In single acting system draining the hydraulics allows the spring/counterweight to coarsen the blade fully - BUT need to do this before rpm decreases to prevent centrifugal latch locking the pitch.
Multi acting system needs a force on spool valve, so have either a mechanical connection to it or solenoid to direct high pressure oil to coarsen.

204
Q

Unfeathering

A

Unfeathering allows engine restart in the air. However oil pressure is lost as engine is off!
Can have an accumulator to store hydraulic power, or a solenoid valve to deliver high pressure oil to fining side of spool valve.

205
Q

Auto feathering

A

Only used during take off and landing, designed to detect low speed high power situations and feather the engine accordingly.

206
Q

Propeller control systems

A

Two lever - Power and rpm levers. For beta range set rpm lever to fully fine, then pulling power back through detents selects ground and reverse ranges.

Single lever - Power lever AND condition lever! Condition lever selects air start, run, ground stop and feather. Power lever then controls power. Governor targets constant rpm.

207
Q

Multi prop synchronising and snychrophasing

A

Synchronising matches rpms by designating one engine master and showing others as rpm differences. Unsynchronised props get “beat” frequency causing noise and vibration.
Synchrophasing achieves specific phase differences (specific settings by aircraft) to reduce noise further.
Need to achieve rpm synchronisation before synchrophasing can be done.

208
Q

Prop torque measurement (2)

A

Helical oil pressure system
AC phase on inner and outer shaft