1988
DOI: 10.1093/imanum/8.3.321
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Finite-Element Approximation of Elliptic Equations with a Neumann or Robin Condition on a Curved Boundary

Abstract: This paper considers a finite-element approximation of a second-order selfadjoint elliptic equation in a region flcR" (with n = 2 or 3) having a curved boundary dQ on which a Neumann or Robin condition is prescribed. If the finite-element space denned over D h , a union of elements, has approximation power h k in the L 2 norm, and if the region of integration is approximated by Q* with dist (Q, £?*) =£ Ch k , then it is shown that one retains optimal rates of convergence for the error in the H 1 and L 2 norms,… Show more

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Cited by 17 publications
(23 citation statements)
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“…Therefore the result (3.14) is a direct consequence of Lemma 5.10 in Barrett and Elliott [6]. Likewise the results (3.15) are a direct consequence of Lemmas 5.8 and 5.9 in Barrett and Elliott [6] and the trace inequality (1.17b).…”
Section: (W H Z) H = (W H Z)~ah Vw H Zes H (316)mentioning
confidence: 66%
See 2 more Smart Citations
“…Therefore the result (3.14) is a direct consequence of Lemma 5.10 in Barrett and Elliott [6]. Likewise the results (3.15) are a direct consequence of Lemmas 5.8 and 5.9 in Barrett and Elliott [6] and the trace inequality (1.17b).…”
Section: (W H Z) H = (W H Z)~ah Vw H Zes H (316)mentioning
confidence: 66%
“…Likewise the results (3.15) are a direct consequence of Lemmas 5.8 and 5.9 in Barrett and Elliott [6] and the trace inequality (1.17b). [] Remark 3.1.…”
Section: (W H Z) H = (W H Z)~ah Vw H Zes H (316)mentioning
confidence: 70%
See 1 more Smart Citation
“…The second term can be estimated, similarly as above, and with arguments similar to the ones used in [3,Lemma 4.2], as:…”
Section: Numerical Integration Error Estimatementioning
confidence: 99%
“…It is a simple matter to show, see Theorem 2.1 in Barrett and Elliott (1986), that the solutions of (1.4) and (1.20) satisfy in each element ~ ~ T* with _m(r ~ t3 t2)~ 0. The interpolation points being where ~?f2 crosses either the element's sides (n = 2) or edges (n = 3) yielding a polyhedral domain O h. A fuller description is given in Barrett and Elliott (1988). We now have…”
Section: As(us V) = Le(v) Vveh 1 (F2) As(v1 Vz)=-a(vl Vz)+e -1 (Vmentioning
confidence: 99%