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MAE155A_Lecture04.pdf

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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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    10MAE 155A

    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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    12MAE 155A

    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)


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