Additive Schwarz Methods for Elliptic Finite Element Problems in Three Dimension

Cover Additive Schwarz Methods for Elliptic Finite Element Problems in Three Dimension
Additive Schwarz Methods for Elliptic Finite Element Problems in Three Dimension
Maksymilian Dryja
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1. For all u G V'''(r), with To and T, j defined by (4. 9), we have jj (4. 10) 7o(l + \og—)-K^{u, u) < s{Tu, u) < j, s{u, u) Here 70 and 71 are constants independent of H and h and the jumps of the coefficients. To prove this theorem, we use Theorem 3. 1 of Section 3; cf. Dryja, Smith and Widlund [4]. For an alternative proof, see Smith [9], [10]. We now briefly discuss how the method can be implemented. Problem (2. 14) has been replaced by (4. 11) Tu = g where g = go + ES'ij. 9o = TqW/i, and gij = T. /u/i- To solve (4. 11) we can use the conjugate gradient method since T is symmetric, positive definite and well conditioned. For simplicity we only consider the first Richardson method. Thus ^ ^, "+1 = i, n _ ^rp^^n _ y) ^ ^ ^ 2/(70(1 + log -r)-' + 7l) n Let r" = r(u" - tz) = rS + Eij rf^, where r^ = ro(u" - u) and rf^ = r. J(u" - u). To find Tq and r^j, we solve (4. 12a) boir^, v) = ^(u", u) -{g, v) = F{v), v e Vo and (4. 126) b, j{r^^, v) = Fiv), vGV„ To compute s{u"-, v) we solve the Dirichlet problems (4.

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