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

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Setting up <strong>the</strong> governing equations<br />

From <strong>the</strong> last Lecture we obtained <strong>the</strong> Total Lagrangian (TL)<br />

Formulation <strong>of</strong> <strong>the</strong> principle <strong>of</strong> Virtual Displacements:<br />

∫<br />

t+∆t<br />

0 S ij δt+∆t 0 ɛ ij d 0 V = t+∆t R (1)<br />

0 V<br />

where <strong>the</strong> Green-Lagrange strain component has been defined as:<br />

(<br />

)<br />

t+∆t<br />

0 ɛ ij = 1 3∑<br />

t+∆t<br />

0<br />

2<br />

u i,j + t+∆t<br />

0 u t+∆t<br />

j,i + 0 u k,i t+∆t<br />

0 u k,j<br />

If we denote 0 ɛ ij , 0 u i as increments in <strong>the</strong> strains <strong>and</strong> displacements<br />

respectively we can write:<br />

k=1<br />

δ t+∆t<br />

0 ɛ ij = δ t 0ɛ ij + 0 ɛ ij (2)<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 2

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