Assumed Modes Methods

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  • 8/10/2019 Assumed Modes Methods

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    G.Le

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    7Assumed

    ModesSumm

    ation

    Whenexactnaturalmod

    esandfrequenciesaremodes

    aredifficu

    lttofind...

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    7.1

    Whatar

    eassumedmodes?

    Asetoflinearlyindependentfunctionsi

    thatsatisfythe

    g

    eometricboundaryconditio

    nsbutnotnec

    essarilythena

    tural

    boundarycond

    itionsofthesystem.

    Notes

    1.

    linearlyind

    ependentie

    2.geometricie

    3.naturalie

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    E

    xample:Assumedmodesforabar

    L

    u(x,t)

    x

    B

    oundarycond

    itions:u|x=0

    =0andu/

    x

    |x=L=0

    Q

    uestion:Can

    yousuggesta

    function(x)

    thatsatisfiesthese

    boundaryconditions?

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    Firstguesstry(x)=x.

    W

    illthiswork?

    W

    hatsthenext

    possibleguess?

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    Q

    uestion:Can

    youfindahig

    herorderassu

    medmode?

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    Qu

    estion:Cany

    ouguesstheg

    eneralformfortheassumedmodes?

    A

    possibleseto

    fassumedmodeswouldbe

    Homework:Provethisandco

    mparewithth

    eexactmodes!

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    Example:A

    ssumedmod

    esforasimplysupported

    beam

    x

    x=L

    x=

    -L

    y

    Geometricboundaryconditions:V(L)=

    0andV(-L)=0

    Whatisapos

    sibleassumed

    mode?

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    C

    anyoufinda

    higherordermode?

    H

    owdothesea

    ssumedmodescomparewiththefirsttwo

    modes

    fromtheexactsolution?

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    7.2

    Approxim

    ationofcontinuoussystem

    sviaassumedmodes

    A

    ssumedmode

    scanbeused

    toformaMDOFapproxima

    tefor

    thecontinuous

    systemeg:

    F

    orabar,theelasticstrainenergyandkin

    eticenergyare

    givenby:

    L

    V

    =

    1/2

    EA(u/

    x

    )2dx

    0L

    T

    =

    1/2

    A(u/

    t)2dx

    0

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    i=N

    U

    singNassum

    edmodes,we

    letu(x,t)=

    i(x)qi(t)

    i=1

    T

    heelasticstrainenergythen

    :

    L

    V

    =

    1/2

    0

    w

    hereqT

    =

    {q1,...,qN}

    L

    Kij

    =

    EAi(x)j(x)dx

    0

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    S

    imilarlythekineticenergyis:

    L

    T

    =

    1/2

    0

    w

    hereqT

    =

    {q1,...,qN}

    L

    Mij

    =

    Ai(x)j(x

    )dx

    0

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    F

    inallyiftheexternalaxialforceperunitlengthisp(x,t),thenthe

    v

    irtualworkdonebythisloa

    dingis:

    L

    W

    =

    0

    UsingNassumedm

    odes,u(x,t)

    =

    SothegeneralizedforceQT

    ={Q1,...,QN}is:

    L

    Qi(t)

    =

    p(x,t)

    (x)dx

    0

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    ThereforebyLagrangesformulation,the

    NDOFapproximation

    forthebaris: M

    q

    +

    Kq

    =

    Q

    Question:Howgoodisthisapproximatio

    n?

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    Example

    :MDOFapproximationfo

    rauniform

    bar

    L

    u(x,t)

    x

    1.Boundaryco

    nditions:u|x=0=0andu/x|x=L=0

    2.Assumedmodes,2DOFa

    pproximation

    1(x)=x/L(x/L2)

    2(x)=(x/L)2(x/L2)2

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    Th

    emassmatrix

    isgivenby:

    L

    Mij

    =

    Ai(x)j(x

    )dx

    0

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    Th

    estiffnessmatrixisgivenby:

    L

    Kij

    =

    EAi(x)j(x)dx

    0

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    H

    encetheapproximatedfirsttwofrequenc

    iesare

    3.7/(2L)(E/)1/2an

    d11.8/(2L)(E/)1/2

    Comparewith

    theexactfirst

    twonaturalfr

    equencies: