h 406 3 orthotropiclamina

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    Principalstresses

    e

    pr nc pa

    rec ons

    are

    so u ons

    o

    ress nvar an s:

    ,

    thestresstensor is diagonal:

    Stressinvariantsinprincipalcoordinates3

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    Generalized Hookes law

    4th order tensor ofelastic constants

    Because ofthesymmetry

    ofthe

    strain tensor

    Because ofthesymmetry

    ofthe

    stress

    tensor

    Equation:

    Because ofthe3symmetry relationships,thenumber

    ofindependent elastic constantsis reduced

    from34=81to21inthemost general anisotropic material

    Theorder of

    partial

    differentiation

    Maybe changed

    4

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    Changeofcoordinates intheelastic constants

    Lettwo coordinate systemsxandxrelated bytherotationmatrixA=aij

    Change of coordinates of thestress tensor:

    (same rule forthestrain tensor)

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    Tensor ofelastic constant:

    6

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    r o rop ccompos e:

    axes

    o

    symme ry

    Theelastic constantsdonotchangeunder coordinate transformationsthat preserve symmetry

    x x laneDirectioncosines:ofsymmetry

    ne n s:

    Mustbe =0

    Similarly,8constantsmustbe equal to0:

    7

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    Directioncosines:(x2,x3)plane

    ofsymmetry

    Thefollowing contants

    Mustalso be equal to0:

    e e s noa ona con oncom ng om e p aneo symme y x1,x3 .

    Overall,there are2112=9independent elastic constantsforanorthotropic material.

    8

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    Orthotropic materials:9independent elastic constants

    oo e s aw may e w en nma r x o m

    Vector ofengineering En ineerin stresscomponents

    strain componentsStiffness matrix

    [theaxes

    1,2,3

    coincide with the

    natural (orthotropy)

    axes

    of

    the

    material]

    9

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    Stiffness matrix

    Compliance matrix

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    Stressstrain relationsandengineeringconstantsfororthotropic lamina

    column bycolumn byconsidering 3load cases:

    1.

    Onegets thefirstcolumn

    ofthecompliance matrix

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    2.

    2nd column ofthe

    Compliance matrix

    3.

    3rd column ofthe

    Comp ance matr x

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    Orthotro ic laminainnatural axes

    1.Compliance matrix

    Foranisotropic lamina,

    EL=ET,G=E/2(1+)

    2.Stiffness matrix

    13

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    Changeofreference frame

    We seek thetransformationmatrix [T]

    Changeofcoordinates

    Fora2nd order tensor:

    [T]is nota

    rotation matrix !!

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    Stressstrain relationship

    InLTaxes:

    Inarbitrary axes:

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    Stiffness matrix inarbitrary axes

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    Compliance matrix inarbitrary axes:

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    Example:find thestrains inthelamina=60

    Elastic constants:Stresses:

    ep :compu e es esses no o opy axes

    18

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    Step 2:compute thestrains innatural axes:

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    Step 3:compute thestrains intheaxes(x,y)

    LT

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    Engineeringconstants

    Thecompliance matrix in

    ar rary axesmay e wr en:

    terms of

    the

    4

    constants:

    EL,

    ET,

    GLT,

    LT.21

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    Graphiteepoxy system Boronepoxy system

    Ex

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    Balancedlamina:ET=EL,LT=TL

    Notisotropic !!

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