Construction of boundary operators for the laplacian. 1. Using of simple layer potential

A. D. Polishchuk
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引用次数: 5

Abstract

1. Functional space Hr,A=. Let G be a bounded open C' -set [ I ] in R3 the boundary of which is 1-smooth surface r. We write G'= R3 \ G and introduce [2] Sobolev spaces W2(G), W2,0(G')=(ueD'(G'):u/r,DuEL2(G')}, where r is the distance of the point xE G' to the coordinates origin 0 and W2'2(f) Introduce the space H' = W2(G)x Wl0(G'). We write the elements of H' as u _ (u,iue), U E W (G), Ue E W2 ,0(G') and define [3] the linear continuous operators yru =UIr, yu = Ur, e : W (G) w2 (r), y,o: W2,0(G') -+ yIU = au /aiinr, yfu = au /aI|r , yl : W2 (G) -+ W,"/2(r), ye W21 (G') + W2 "2(r) where ii exterior normal to r, W2(r) be a dual space to W?'2(J).Wewrite y0 =y _sy = yY , E > e= const. Introduce the spaces H,' = {u E H' : yru = 01, (u,V)Hi = JVUVv, IIUIIHI = (U)t, GuG' r H
拉普拉斯算子的边界算子构造。1. 简单层电位的使用
1. 函数空间Hr,A=。设G为R3中的一个有界开C'集[I],其边界为1光滑曲面r。我们将G'= R3 \ G并引入[2]Sobolev空间W2(G), w2,0 (G')=(ueD'(G'):u/r,DuEL2(G')},其中r是点xE G'到坐标原点0和W2'2(f)的距离,引入空间H' = W2(G)x Wl0(G')。我们将H'的元素写成u _ (u, Ue), u E W (G), Ue E w2,0 (G'),并定义[3]线性连续算子yru =UIr, yu = Ur, E: W (G) W2(r), y,o: w2,0 (G') -+ yu = au /aiinr, yfu = au /aI|r, yl: W2(G) -+ W, ' /2(r), ye W21 (G') + W2 '2(r)其中ii外法向于r, W2(r)是W?'2(J)的对偶空间。我们写y0 = y_sy = yY, E > E = const。引入空格H,' = {u E H': yru = 01, (u,V)Hi = JVUVv, IIUIIHI = (u)t, GuG' r H
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