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Level Flight Performance
Equations of Motion
Thrust and Power Required
Minimum Drag
MAE 155A
Oblique Wing Research Aircraft (NASA Image)
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2MAE 155A
Geodetic and Local Coordinates
North
East
Up
Z
X (Prime Meridian)
Y
(X, Y, Z) is an Earth-Centered,Earth-Fixed Coodinate System
Latitude
Longitude
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3MAE 155A
Velocity Vector Orientation
The flight path angleis positive when the
airplane is climbing.
The flight path headingis positive clockwisefrom true north.
VelocityVector
Down
North
North
East
Flight PathHeading
Flight PathAngle
VelocityVector
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4MAE 155A
Forces Acting on the Airplane
Lift Up
Gravity
Velocity
Vector
ThrustDrag
Lift Up
Gravity
VelocityVector
Thrust
Drag
The bank angle is positive when the
lift vector is tilted to cause a rightturn (heading rate is positive).
The thrust vector isaligned in the lift-dragplane, but is rotatedabove the velocity vector.
ThrustAngle
BankAngle
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5MAE 155A
Non-Rotating Spherical Earth
dV
dt=g
[
TcosD
W
sin
]ddt=
g
V {[n TW sin ]cos[ V2
g R1]cos}
d
dt=
g
V
{[n
T
W
sin
]sin
cos
V2
g Rcossin tan
}dWdt=CT
d
dt=
1
R VcoscosVWN
d
dt=
1
R cos VcossinVWE
dR
dt=Vsin V
WU
g = gravity
T = thrustD = dragW = weightC = thrust specific fuel consumptionV = airspeedL = liftP = powern = L/W = load factorR = radial distance from Earth center
= flight path
=thrust angle
=bank angle
= flight path heading
= latitude
= longitude
(VWN
, VWE
, VWU
) = wind speed in (North, East, Up) direction
dW
dt=C
P
or
=propulsive efficiency
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6MAE 155A
Low Speed Aircraft
dV
dt=g
[TDW sin
]ddt=
g
V n coscos
d
dt
=g
V
nsin
cos
dW
dt=CT
d
dt=
1
R VcoscosVWN
d
dt=
1
R cos VcossinVWE
dh
dt=VsinV
WU
Assumptions:
h = altitude = R RE
RE
= Earth radius
V2
g Ris small
is small
dW
dt=C
P
or
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7MAE 155A
Steady Level Flight
Steady (unaccelerated) level flight performance equations make the followingassumptions and simplifications:
0=dV
dt=g[ TDW sin ]
0=d
dt = gV n coscos
0=d
dt=
g
V
n sin
cos
0=dh
dt=Vsin
constant airspeed
constant flight path
constant heading
constant altitudeand zero winds
=0
=0
n=cos
cos= LW=1
T=DWsin=D
L=W
T=D
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8MAE 155A
Drag Polar
The drag and lift forces are typically normalized by dynamic pressure and (wing)reference area.
The resulting coefficients are non-dimensional.
CD
=CD ,
0K C
L
2 K1
e AR
CD=
D
q SC
L=
L
q S
The drag polar provides the basic aerodynamic information needed to predict levelflight performance.
q=1
2V2
AR=b2
S
q = dynamic pressureV = airspeedAR = aspect ratiob = wingspanS = reference area
=atmospheric density
e = wing planform efficiency factorCD,0
= zero-lift drag coefficient
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9MAE 155A
Thrust Required
Turbojet engines are usually rated in terms of thrust.
Thrust required refers to the engine thrust needed to maintain steady, level flight.
TR=D=q S C
DC
D=C
D ,0K C
L2
TR=D=q S CD ,0q S K CL2 W=L=q S C
L
TR=q S C
D ,0
K W2
q Sq=
1
2V2
TR=
1
2V2 S C
D ,0
2K W2
V2 S TR
= thrust required
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Thrust Available
Thrust available from a turbojet engine is approximately constant relative to airspeed.
Available thrust generally varies with altitude:
TR
V
Thrust requiredat sea level
Thrust availableat sea level Thrust required
at altitude
Thrust available
at altitude
Max airspeedat sea level
Max airspeedat altitude
TAT
SL
SL T
A= thrust available at altitude
TSL
= thrust available at sea level
=density at altitude
SL=density at sea level
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11MAE 155A
Minimum Thrust Required
What conditions lead to minimum drag (and therefore minimum thrust required)?
W=L=q S CL
T=D=q S CD
TR=
W
CL/C
D
T
W=
D
L=
1
L /D=
1
CL/C
D
Minimum drag occurs when CL/C
Dis maximized.
CL
CD
=C
L
CD ,0
K CL2
C
L CLC
D=CD ,0K CL
2
CD ,0
K CL2=0 C
L=CD ,0K
CL
CD
=1
2CD ,0KV=
2W
S KCD ,0Minimum Drag
Minimum DragMinimum Drag
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Power Required and Available
PR=V TR=V D=1
2 V3
S CD ,02K W
2
V S
PR
VAirspeed forminimum power
Minimumpower required
CL=3CD ,0K
Minimum
power requiredoccurs at:
Power available frompiston engines isapproximately constantwith airspeed butvaries with alttiude
PAP
SL SL
Power available (piston)
Power available (jet)