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The Finite Element Method for the Analysis of Non-Linear and ...

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Elastic Material<br />

For <strong>the</strong> case <strong>of</strong> an elastic material we already saw that <strong>the</strong> TL<br />

Formulation (used <strong>for</strong> large de<strong>for</strong>mation analysis) yields:<br />

t<br />

0S ij = t t<br />

0C ijrs 0ɛ rs<br />

<strong>The</strong> elasticity tensor <strong>for</strong> 3D stress conditions is defined as:<br />

t<br />

C ijrs = λδ ij δrs + µ(δ ir δjs + δ is δjr)<br />

where λ <strong>and</strong> µ are <strong>the</strong> Lamé constants <strong>and</strong> δ ij is <strong>the</strong> Kronecker delta,<br />

Eν<br />

λ =<br />

(ν)(1 − 2ν) , µ = E<br />

2(1 + ν)<br />

{ 0 i ≠ j<br />

δ ij =<br />

1 i = j<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 8

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