bar elements & le analysis

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    BarElement&LinearStaticAnalysisLinearStaticAnalysis

    ,thefollowingassumptions:1.Smalldeformations(loadingpatternisnotchangedduetothedeformedshape)2.Elasticmaterials(noplasticityorfailures)3.Staticloads(theloadisappliedtothestructureinasloworsteadyfashion)

    Linearanalysiscanprovidemostoftheinformationaboutthebehaviorofastructure,

    andcanbeagoodapproximationformanyanalyses.Itisalsothebasesofnonlinear

    analysisinmostofthecases.

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    BarElement

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    StiffnessMatrix DirectMethod

    ssum ng a e sp acemen u svary ng near ya ong eax so e ar, .e.

    Forcein ar

    Thebarisactinglikeaspring:

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    DegreeofFreedom(DOF)Number

    of

    components

    of

    the

    displacement

    vector

    at

    a

    node.For1Dbarelement:onedofateachnode.

    StiffnessMatrix AFormalApproach

    Define

    two

    linear

    shape

    functions

    as

    follows

    where

    Thedisplacementcanbewrittenas

    or

    Straincanbeexpressesas

    whereB istheelementstraindisplacementmatrix

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    Stresscanbewrittenas

    Thestrainenergystoredinthebarisgivenby

    Thework

    done

    by

    the

    two

    nodal

    forces

    is

    It is stated that: U = W

    istheelementstiffnessmatrix

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    Theelementstiffnessmatrixofabarelement

    Thestrainenergyintheelementcanbewrittenas

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    Example1

    whichisloadedwithforceP,andconstrainedatthetwoends.Pleaseusetwo1Dbar

    elements.

    Element1: Element2:

    Imagineafrictionlesspinatnode2,whichconnectsthetwoelements.Theglobal

    FEequationcanbeconstructedasfollows,

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    Loadandboundaryconditions(BC)are

    FEequationbecomes:

    Stressinelement1is Stressinelement2is

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    Notes:

    In this case, the calculated stresses in elements 1

    structures.It will not help if we further divide element 1 or 2 into

    smaller finite elements.

    For tapered bars, averaged values of the cross

    sectional areas should be used for the elements.

    We need to find the displacements first in order to

    find the stresses, since we are using the displacement

    .

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    Example2

    Wefirstchecktoseeifornotthecontactofthebarwiththewallontherightwill

    occur. o o s,we mag ne ewa on er g sremove an ca cu a e e

    displacementattherightend

    ,contact

    occurs.

    TheglobalFEequationisfoundtobe

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    Theloadandboundaryconditionsare,

    The2ndequationgives

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    Supportreactions:

    The1stequationgives