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An Exact Solution for Moving Finite Elements Applied to the . . .

By J.D.P. Donnelly


4> = 0 which in the limit b !1 becomes (C.6). 9 AppendixC General mesh diffusion We consider the equation u t + f(u; u x ) = fflu xx (C.1) In Appendix A we replace u i\Gamma1 \Gamma m i\Gamma 1 2 ( s i\Gamma1 \Gamma u i\Gamma1 ) in (A.1) by u i\Gamma1 \Gamma m i\Gamma 1 2 s i\Gamma1 + f(u i\Gamma1 ; m i\Gamma 1 2 ) and u i \Gamma m i\Gamma 1 2 ( s i \Gamma u<F8

Year: 1990
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