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

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

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Example<br />

B. Jaumann stress rate <strong>for</strong>mulation<br />

This <strong>for</strong>mulation uses <strong>the</strong> following constitutive relationship:<br />

t˜τ ij = t C ijrs t D rs (7)<br />

where <strong>the</strong> velocity strain tensor t D is computed using <strong>the</strong> velocity gradient L (see<br />

Lecture 4) :<br />

[ ]<br />

0 2<br />

L = ẊX −1 =<br />

0 0<br />

L can be decomposed to s symmetric part D = D T (<strong>the</strong> velocity strain tensor) <strong>and</strong> a<br />

skew symmetric part W = −W T (<strong>the</strong> spin tensor):<br />

L = D + W<br />

[<br />

0 1<br />

D =<br />

1 0<br />

which in this case yields<br />

] [ ]<br />

0 1<br />

, W =<br />

−1 0<br />

Now we use <strong>the</strong> same constitutive matrix C <strong>and</strong> Eqn (7) to obtain <strong>the</strong> Jaumann stress at<br />

time t:<br />

⎡ ⎤ ⎡ ⎤<br />

˜τ 11 0<br />

⎢ ⎥ ⎢ ⎥<br />

⎣ ˜τ 22 ⎦ = ⎣ 0 ⎦<br />

˜τ 12<br />

3846<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 16

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