1965
DOI: 10.1070/rm1965v020n05abeh001190
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Elliptic Singular Integro-Differential Operators

Abstract: Experiments have been carried o u t i n order to investigate a possible dependence of the film transfer in liquid helium I1 on the geometrical conditions of the measuring arrangement or on a temperature gradient along the film. Using transfer vessels of different shape, no variation in the rate of transfer could be detected. Equally no change from the ordinary rate of flow could be found under temperature differences up to 3.5 x deg.

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Cited by 82 publications
(55 citation statements)
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“…Finally let t G À/3(A) be the H3 projection of z into M3(A), so (3)(4)(5)(6)(7)(8) l|/|l3<ll*ll3<C||t)||3, and, using (3.6), (3.9) ||/ -z||3 < CAA||z||4 < CAa||ü||3.…”
Section: Iax -A2\mentioning
confidence: 99%
“…Finally let t G À/3(A) be the H3 projection of z into M3(A), so (3)(4)(5)(6)(7)(8) l|/|l3<ll*ll3<C||t)||3, and, using (3.6), (3.9) ||/ -z||3 < CAA||z||4 < CAa||ü||3.…”
Section: Iax -A2\mentioning
confidence: 99%
“…t~O Here Aj, C i, L and 2o are sufficiently smooth complex-valued functions [1]. In the case m=0 these equations reduce to singular integral equations with Cauchy kernels which have been solved with Fourier series in [11] and [30].…”
Section: D"u ~1 Dju A~ ~ + J~o A_ J(z)-~fl~jmentioning
confidence: 99%
“…For this equation preliminary convergence results can be found in [1], [2], [5], [14] and [33]. Our strongly elliptic systems with convolutional principal part contain, in addition, systems of integro-differential equations [3] (see [7]) with constant coefficients, certain singular integral equations, in particular, those of plane elasticity [7,Appendix], [24], [25], [26], [34], Fredholm integral equations of the second kind [6], [8], [11], [12], [13], [17], [27], [35], and also the integro-differential operator of Prandtl's wing theory [16], [17], [18], [24], [35].…”
mentioning
confidence: 99%
“…where f = zx(t) + iz2(r), A0, C0 are constant p X p matrices, and where s, respectively T, denotes the arclength on T. The principal symbol of this operator is given by the matrix-valued function [3] aU) = nmi[A0 + c0M foriei> i-2.1.1. The Case of Even m. In the case when m is even, a -m/2 is a nonnegative integer and the strong ellipticity condition (2.2) now reads (2.4) (-l)aRer0K±CoK>a-|2, which must hold for both signs and is equivalent to det(A0 + XC0)*0 forallXe [-1,+1].…”
mentioning
confidence: 99%