Aircraft Propulsion
Propellers
Piston Engines
Thrust Equation
Turbojet Engines
MAE 155A
Curtis Wright R-2600
2MAE 155A
Propellers
The propeller is made up of a series of rotating wings or “blades”.
Propeller theory is more complex than simple wings.
The blades may have complicated shapes that vary with span.
The aerodynamic flow around each blade may interact.
r
V∞r
V∞
Airflow direction over propeller blade
Velocity from propeller rotation
Propeller blade pitch angle
Freestream velocity
r=blade radial position= propeller angular velocity=r=blade pitch angle
3MAE 155A
Propeller Forces
Engine power is used to overcome drag forces on the propeller blades.
Lift from each propeller blade creates a thrust force to propel the airplane forward.
r
V∞
dTdL
dD
dT=dL cos−dD sin
=−
dL=lift incrementdD=drag incrementdT=thrust force
dQ=torque increment
dT=dL cos−−dD sin −
Recall that lift and drag are defined relative to the local velocity vector
dQ=r [dLsin −dDcos − ]
4MAE 155A
Propeller Efficiency
The propeller efficiency is the ratio of power available from the propeller (to move the airplane) to the power delivered by the engine.
=T AV ∞
P
= propeller efficiencyT A=thrust available move airplane
V∞=airspeedP=engine shaft brake power
Define power and thrust coefficients as follows:
cP=P
n3D5cT=
T A
n2D4
cT=thrust coefficient
cP= power coefficient
=atmospheric densityD= propeller diameter
=2n= propeller angular velocityJ=advance ratio
=T AV ∞
P=n2D4cT V ∞
n3D5cP= cTcP V∞
n D = cTcP J J= V ∞n D
5MAE 155A
Example Propeller Charts
Advance Ratio (1/rev)
Advance Ratio (1/rev)
Effi
cien
cy
Thr
ust C
oeffi
cien
t
McCormick, B.W., Aerodynamics,Aeronautics, and Flight Mechanics, Wiley, 1979.
6MAE 155A
Piston Engines
A reciprocating engine produces power by moving a piston inside a cylinder.
A typical engine has intake, compression, power (ignition), and exhaust strokes.
A normally aspirated engine (no turbo or supercharger) loses power as altitude increases.
A turbo- or super-charged engine maintains constant power up to a critcal altitude of about 20,000 ft.
Below critical altitude:
Above critical altitude:
P=PSL[ SL
− 17.75 1−
SL ]≃PSL SL
P≃PSL
P≃PSL crit
P=engine power at altitudeP SL=engine power at sea level
=density at altitudeSL=density at sea level
=density at altitudeSL=density at critical altitude
7MAE 155A
Thrust Equation
A jet engine produces thrust by taking a small amount of air and giving it a lrage increase in velocity (thereby changing its momentum).
The thrust equation is obtained by considering changes in momentum of the airflow entering and exiting the engine.
V a V e
Ae
pape
T=mairm fuel V e−mairV a pe Ae− pa Aa
T=net thrustmair=airmass flow
m fuel= fuel mass flow
Ve=exit velocity
pe=exit static pressure
Ae=exit area
V a= freestream velocity
pa=ambient static pressure
Diff
use
r
Com
pre
sso
r
Bu
rne
r
Tur
bin
e
Noz
zle
Aa
8MAE 155A
Jet Engine Types
A turbojet has all inlet air passing through the combustion area of the engine.
The thrust of a turbofan engine is a combination of thrust produced by fan blades and jet thrust produced from the exhaust nozzle.
The ratio of the weight of air bypassing the combustion area to total weight of air entering the engine is called the bypass ratio.
A turboprop uses a gas turbine to drive a propeller.
Both the turbofan and turboprop impart momentum to greater volumes of air that a turbojet, but the velocity added to the air is less.
9MAE 155A
Turbojet Example
The mass flow of fuel is usually small compared to the mass flow of air.
JetCat P80-SE Turbojet
Idle Rotational Speed 35,000 rev/minMax Rotational Speed 125,000 rev/minIdle Static Thrust 3 NMax Static Thrust 97 NIdle Fuel Consumption 0.075 kg/minMax Fuel Consumption 0.233 kg/minAir Mass Flow Rate 0.25 kg/sExhaust Gas Temperature 510 – 700 CExhaust Gas Velocity 1397 km/hrPressure Ratio 2.4
T≃mairV e=0.25 kgs 1397 kmhr hr3600 s 1000mkm s2Nkg m =97 N=22 lbstatic thrust:
T=mair V e−V a pe Ae− pa Aa
10MAE 155A
Pratt & Whitney JT4A-3 Turbojet
McC
orm
ick,
B.W
., A
ero
dyn
am
ics,
Ae
ron
aut
ics,
and
Flig
ht
Mec
ha
nics
, Wile
y, 1
979
.
Sea Level 45,000 ft