Power and Thrust for Cruising Flight
[Pages:23]Power and Thrust for Cruising Flight
Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2018
Copyright 2018 by Robert Stengel. All rights reserved. For educational use only.
1
U.S. Standard Atmosphere, 1976
2
1
Dynamic Pressure and Mach Number
= air density, function of height = e-h
sea level
a = speed of sound = linear function of height
Dynamic pressure = q V 2 2 Mach number = V a
3
Definitions of Airspeed
Airspeed is speed of aircraft measured with respect to air mass
Airspeed = Inertial speed if wind speed = 0
? Indicated Airspeed (IAS)
IAS =
( ) 2 p - p stagnation
ambient
SL =
( ) 2 ptotal - pstatic
SL
!
2qc SL
,
with
qc
!
impact
pressure
? Calibrated Airspeed (CAS)*
CAS = IAS corrected for instrument and position errors
=
( ) 2 qc corr #1
SL
* Kayton & Fried, 1969; NASA TN-D-822, 1961
4
2
Definitions of Airspeed
Airspeed is speed of aircraft measured with respect to air mass
Airspeed = Inertial speed if wind speed = 0
Equivalent Airspeed (EAS)*
EAS = CAS corrected for compressibility effects =
( ) 2 qc corr # 2
SL
True Airspeed (TAS)*
Mach number
V TAS = EAS
SL (z)
=
IAScorrected
SL (z)
TAS M=
a
* Kayton & Fried, 1969; NASA TN-D-822, 1961 5
Flight in the Vertical Plane
6
3
Longitudinal Variables
7
Longitudinal Point-Mass Equations of Motion
? Assume thrust is aligned with the velocity vector (small-angle approximation for )
? Mass = constant
V!
=
(CT
cos
-
CD
)
1 2
V
2S
-
mg
sin
(CT
-
CD
)1
2
V 2S
-
mg
sin
m
m
!
=
(CT
sin
+
CL
)
1 2
V
2S
-
mg
cos
CL
1 2
V
2S
-
mg
cos
mV
mV
h! = -z! = -vz = V sin
V = velocity = Earth-relative airspeed
r! = x! = vx = V cos
= True airspeed with zero wind = flight path angle
h = height (altitude)
r = range
8
4
Conditions for Steady, Level Flight
? Flight path angle = 0 ? Altitude = constant ? Airspeed = constant ? Dynamic pressure = constant
0
=
(CT
-
CD
)
1 2
V 2S
? Thrust = Drag
m
0
=
CL
1 2
V
2S
-
mg
mV
h = 0
? Lift = Weight
r = V
9
Power and Thrust
Propeller
Power
=
P
=
T
?V
=
CT
1 2
V 3S
independent
of
airspeed
Turbojet
Thrust
=
T
=
CT
1 2
V 2S
independent
of
airspeed
Throttle Effect
T
=
T T max
=
CTmax qS T ,
0 T 1
10
5
Typical Effects of Altitude and Velocity on Power and Thrust
? Propeller
[Air-breathing engine]
? Turbofan
[In between]
? Turbojet
? Battery
[Independent of altitude
and airspeed]
11
Models for Altitude Effect on Turbofan Thrust
From Flight Dynamics, pp.117-118
Thrust
=
CT
(V
,
T
)
1 2
(h)V
2S
( ) =
ko
+
k1V n
1 2
(h)V 2ST ,
N
ko = Static thrust coefficient at sea level k1 = Velocity sensitivity of thrust coefficient n = Exponent of velocity sensitivity [ = -2 for turbojet]
(h) = SLe-h, SL = 1.225 kg / m3, = (1 / 9, 042) m-1
12
6
Thrust of a Propeller-Driven
Aircraft
With constant rpm, variable-pitch propeller
T
= PI
Pengine V
= net
Pengine V
P = propeller efficiency I = ideal propulsive efficiency
( ) ( ) = TV T V + Vinflow = V V + Vfreestream 2
netmax 0.85 - 0.9
Efficiencies decrease with airspeed Engine power decreases with altitude Proportional to air density, w/o supercharger
13
Reciprocating-Engine Power and
Specific Fuel Consumption (SFC)
P(h)
PSL
=
1.132
(h)
SL
-
0.132
SFC Independent of Altitude
? Engine power decreases with altitude ? Proportional to air density, w/o supercharger ? Supercharger increases inlet manifold pressure, increasing power and extending maximum altitude
Anderson (Torenbeek) 14
7
Propeller Efficiency, P, and Advance Ratio, J
Effect of propeller-blade pitch angle
Advance Ratio
J= V nD
where V = airspeed, m / s n = rotation rate, revolutions / s D = propeller diameter, m
from McCormick
15
Thrust of a Turbojet Engine
T
=
m V
02*# 1,% 32+$
o o-
1
(%
t
'$t -
1
& ( '
(
c
-1) + t
o c
-1/2 / .
42 -15
62
m! = m! air + m! fuel
( ) o = pstag
( -1)/
pambient
;
= ratio of specific heats 1.4
t = (turbine inlet temp. freestream ambient temp.)
c = (compressor outlet temp. compressor inlet temp.)
from Kerrebrock
Little change in thrust with airspeed below Mcrit
Decrease with increasing altitude
16
8
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