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Explicit representations

The theoretical design of a class of time discretized operators emanating from the generalized family of time discretized operators given earlier in Algorithm 1 leading to explicit representations of the form tex2html_wrap_inline33868 (in a nonlinear sense) follow next.

Type 2-GInO-Explicit: Nth-order accurate representations

A family of Nth-order accurate explicit representations can be directly obtained from Algorithm 1 described in equations (3.110-3.114 ) by taking tex2html_wrap_inline28161 , tex2html_wrap_inline33876 , and tex2html_wrap_inline33878 ( tex2html_wrap_inline33790 ).

      Alr8476

It is to be noted that this explicit time discretized operator is only conditionally stable when tex2html_wrap_inline33888 as in typical traditional explicit time integration operators (and considering Rayleigh damping with tex2html_wrap_inline32879 and tex2html_wrap_inline27935 diagonalized).

Type 2-GInO-Explicit: Nth-order accurate representations with artificial damping

On the other hand, setting tex2html_wrap_inline33896 , tex2html_wrap_inline33898 , tex2html_wrap_inline33900 , and tex2html_wrap_inline33902 in Algorithm 1 represented by equations (3.110-3.114), and tex2html_wrap_inline33728 is taken as

displaymath33906

we then have the theoretical design leading to the representation described next. The resulting Nth-order accurate integration operators are explicit and L-stable for nonlinear structural dynamics [E-LNInO].

      Alr8587

where we introduced tex2html_wrap_inline33916 which is termed as an artificial damping matrix and is taken as

eqnarray8678

and tex2html_wrap_inline33918 and tex2html_wrap_inline33920 may be determined by the following set of inequalities

eqnarray8683

and tex2html_wrap_inline33922 is termed an artificial damping ratio (alternative efforts are currently underway and we hope to disseminate these results in the near future).

Cor8685

Rem8688



Xiangmin Zhou
Wed Sep 6 20:47:30 CDT 2000

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