1948
DOI: 10.1017/s030500410002421x
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On perturbation problems associated with finite boundaries

Abstract: The methods of a previous paper (9) are improved and extended. It is assumed that the eigenfunctions and eigenvalues of an eigenvalue problem given by an elliptic differential equation are known subject to given boundary conditions on a finite boundary. It is shown how the corresponding quantities can be obtained for a similar problem in which the original differential equation, boundary and boundary conditions are simultaneously perturbed. The introduction of a surface displacement vector allows of a Taylor e… Show more

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Cited by 11 publications
(2 citation statements)
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“…We now assume that the outer boundary is displaced by a small amount such that the new surface point nr is a unit vector from the unperturbed surface pointing outwards. Using the method detailed by (Wassermann, 1948) and (Hinch, 1991) we expand the solution to Eqn. (1b) using perturbation theory.…”
Section: Expansion Of Perturbed Surfaces In Transport Theorymentioning
confidence: 99%
“…We now assume that the outer boundary is displaced by a small amount such that the new surface point nr is a unit vector from the unperturbed surface pointing outwards. Using the method detailed by (Wassermann, 1948) and (Hinch, 1991) we expand the solution to Eqn. (1b) using perturbation theory.…”
Section: Expansion Of Perturbed Surfaces In Transport Theorymentioning
confidence: 99%
“…When these effects are caused by an underlying elastic deformation field u (as defined in section 2.2.1), a coupling between the cavity electromagnetic field and the elastodynamic field results, which we compute now. Following the work of Bethe and Schwinger [181] (see also [182]), we consider the two configurations shown in fig. 2.10, depicting a cavity perturbed in shape, i.e.…”
Section: Photon-phonon Coupling In a Cavitymentioning
confidence: 99%