l2_static aeroelasticity of 2d wing segment

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  • 8/10/2019 L2_Static Aeroelasticity of 2D Wing Segment

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    Xie Changchuan

    2014 Autumn

    2nd Static Aeroelasticityof 2D Wing Segment

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    2

    Content1The model of 2D wing segment

    2Solution of aeroelastic load and divergency

    3The model of the 2D wing with control surface

    4Control efficiency and reversal

    Main AimsUnderstand the basic phenomena, concepts,

    math principles, corresponding analysis

    methods and the mechanism of staticaeroelasticity of the aircraft from the simplest

    models of 2D wing segment.

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    3

    The static aeroelasticity

    The success of Wright

    brothers and the failure

    of Longley

    Slowly deform, ignore the inertial forces

    The problems:

    Load RedistributionStatic aeroelastic divergence

    Control efficiency

    Control reversal

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    Airfoilsymmetry thin Spanunity(1)

    Chordc Air force center1/4 chord

    Elastic centere behind air force center

    Coefficient of torsion spring

    Slope of lifting curve Initial AOA

    Elastic angle Speed of flowV

    KyC

    0

    The model of 2D wing segment

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    Forces on the wing segment

    The change of the plunging

    would not produce air force

    Direct analysis

    2

    0 0

    1( ) ( )

    2e y yF V C c qcC

    = + = +

    0( )e e yM F ec qecC = = +

    s K=

    Lift

    Moment

    Elastic torque

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    2D segment equilibrium equation

    0( )yK qecC

    = +

    0 01

    y

    y

    qecC qR

    K qecC qR

    = =

    0( )

    y yK qecC qecC

    =

    s aM=Equality of air forceand elastic force

    Obtain the elastic angle

    Aeroelastic load0 0 0

    1

    ( )

    1e

    qRqRK

    q

    qRM K

    qRR = +

    =

    0 0r yM qecC qRK

    = =

    / /y meC K C K

    = =

    01 1e rq

    MKqR qR

    qR

    =

    =Elastic incremental load

    Rigid load

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    Static Aeroelastic Load and Divergence

    Aeroelastic load0

    1e

    qRM K

    qR

    =

    /mC K

    =

    1 0 ?qR =

    01

    qRq

    =elastic angle

    1/divm

    Kq R

    C

    = =

    eM

    0

    /

    1 /

    div

    div

    q q

    q q =

    divq qWhen

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    0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0

    0

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    M1

    M0

    1

    0

    M

    +0

    k K

    =

    2

    a yqec C=

    The force lines

    are parallel

    div yK q ecC

    =

    div Kq ecC=

    Static Aeroelastic Load and Divergence

    Iteration analysis

    Process of iteration

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    0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.00

    2

    4

    6

    8

    10

    12

    14

    16

    18

    20

    /

    0

    q/qdiv

    The relationship of twist angle and dynamic pressure

    Static Aeroelastic Load and Divergence

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    The energy analysis

    Consider the quilibrium

    state of the system *

    The little disturbance of

    twist angle

    Virtual work of air force*

    a yW M qecC

    = =

    *U K =

    aW U >

    The critical case = divy

    aW U K

    q

    ecC

    =

    Work of outer force is larger than the incrementalof elastic potential energy, the system is unstable.

    Static Aeroelastic Divergence

    Virtual work of elastic force

    When

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    Analysis by equation theory

    The equation of

    static aeroelasticity

    Look as a linear

    algebra equation0A

    0( )yK qecC

    = +

    0( )y yK qecC qecC

    =

    x b=

    =0A

    all Eig( ) 0A >

    any Eig( ) 0A =

    0div yK q ecC

    = div

    y

    Kq

    ecC

    =

    Static Aeroelastic Divergence

    When1x A b=

    Unique solution

    Infinite many solutions

    The critical case

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    Summary

    The static aeroelastic

    divergence div

    y m

    K Kq

    ecC C

    = =

    0

    /

    1 /

    div

    div

    q q

    q q =

    0

    /

    1 /

    dive

    div

    q qK

    q q =

    Four solutionmethods

    Force equilibriumof Newton

    Iteration method

    Energy principle Theory of linear

    equation

    How to promote the divergence speed/dynamic pressure?

    Static Aeroelastic Load and Divergence

    The static aeroelastic

    response

    When divq q

    Lifting coefficient = y m yy y yy

    qcC C K C C C CK qecC

    +

    = +

    When the numrator equals to 0 =0y mrev ycC C K C q

    +

    ( / )=ev

    y

    m

    r

    yK C Cq

    cC

    When

    Usually is positiveyC

    is negativemC

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    Control efficiency

    Rigid lifting coefficient r

    y yC C

    =

    revq q< Define the elastic control efficiency

    ( )

    y y m y

    r

    y y y

    C qcC C K C

    C K qecC C

    +

    = =

    1 / 1 /

    1 / 1 ( / )( / )

    rev rev

    div rev div rev

    q q q q

    q q q q q q = =

    0 0 =

    When

    y

    div

    K

    Cq

    ec

    =

    ( / )=ev

    y

    m

    r

    yK C Cq

    cC

    Divergence

    D. P.

    Reversal

    D. P.

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    Control efficiency and reversal of wing segment

    with control surface

    Homework

    1

    Please draw the curve of the control efficiencyvarying with dynamic pressure

    Consider the case of , the horizontal axis using the

    dimensionless number . Further, determine the curve

    shape when and .

    2The control efficiency and reversal of wing

    segment with leading edge control surface

    The model and the parameters are same with the model inclass, but with the leading edge control surface. Please deduct

    the expressions of the control reversal dynamic pressure and

    the control efficiency. Comparing with the case of trailing edge

    control, give out necessary discussion.

    / divq qdivq q