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Treatment of links in partitioning (4)<br />

• The Lagrange multipliers method (recall Part 1) may<br />

be generalized as follows<br />

• Synchronous case:<br />

A = Cγ<br />

m C<br />

−1 T<br />

Cv<br />

= b<br />

12<br />

z = b−Cv n+ −Cγ<br />

m −1<br />

( f e − f<br />

i )<br />

Aλ = z<br />

n<br />

∆ t +∆t<br />

γ =<br />

2<br />

• Asynchronous case: just replace the scalar γ by the<br />

matrix:<br />

old new<br />

Γ= diag ( γ i<br />

) δti<br />

+ δtL<br />

γ<br />

i<br />

=<br />

2<br />

• The connections matrix remains symmetric and<br />

positive definite like in the synchronous case.<br />

101<br />

n+<br />

1<br />

Example 12a – Taylor bar impact revisited<br />

• A - Solution with spatially uniform time increment<br />

(BAMD01)<br />

• B - Solution with space partitioning (BAMD03) 102<br />

51

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