1973
DOI: 10.1137/1015093
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Solution of Boundary Value Problems by Integral Equations of the First Kind

Abstract: SummaryThis paper is concerned with the recent developments in the solution of boundary value problems by integral equations of the first kind. Basic results for weakly singular and hypersingular boundary integral operators will be discussed. Emphases will be given to the mathematical foundation of the method' as well as to the physical interpretations of various side conditions derived for the unique solvability of the integral equations of the first kind.

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Cited by 167 publications
(94 citation statements)
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“…We also estimate the conditioning of the discrete equations. Next we generalize the estimates to the case of certain systems of equations of a form which arises frequently in applications, e.g., in Fichera's method with Fredholm integral equations of the first kind [37], [50], [51], [52], [53]. We then verify that strongly elliptic pseudodifferential operators satisfy all the assumptions made in the analysis.…”
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confidence: 85%
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“…We also estimate the conditioning of the discrete equations. Next we generalize the estimates to the case of certain systems of equations of a form which arises frequently in applications, e.g., in Fichera's method with Fredholm integral equations of the first kind [37], [50], [51], [52], [53]. We then verify that strongly elliptic pseudodifferential operators satisfy all the assumptions made in the analysis.…”
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confidence: 85%
“…The scalar case with p = q = 1, B = 1, X0 = 1, L = 0 is Symm's integral equation of conformai mapping [40], [45], [48], [51], [95], [100]. In [31] it is shown that the numerical conditioning is superior with B = 1, X0 = 1 rather than B = 0, X0 = 0 and scaling of T. As a system, (2.3.12) is used in viscous flow problems, particularly in connection with Stokes flows [50]- [53], electrostatics [73], [85], [86], acoustics [38], plane elasticity [20], [32], [51], [56], [73], plate bending [51], [52], and torsion problems [56] [50], [51], [53], [54], [55], [73], [85], [86], [100]. However, only preliminary convergence results have appeared for the collocation method [1], [2], [5, p. 271 ff.…”
Section: Iax -A2\mentioning
confidence: 99%
“…This is different than the proof available in [4]. The following two lemmas may also be found in [3].…”
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confidence: 79%
“…This is a standard argument. (b) The uniqueness of problems I and II are also standard, as is the existence of 4> and (i//, C) (see for example [3,4]). Our low-frequency theory is based on the existence proofs presented in [3], To present our main result we need several lemmas.…”
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confidence: 99%
“…In order to avoid difficulties of nonuniqueness when the interior domain has conformai radius one, we follow [6], [11], [14] in seeking to express « as a normalized single layer potential plus a constant. That is, we seek a function xp on L" of mean value zero and a real number co such that (1.2) u(z) = -^-flog\z-y\xp(y)dsv + oo, zER2.…”
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confidence: 99%