2000
DOI: 10.1002/(sici)1099-1476(20000325)23:5<441::aid-mma123>3.0.co;2-u
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Boundary integral method for thermoelastic screen scattering problem in ?3

Abstract: We investigate a three‐dimensional mathematical thermoelastic scattering problem from an open surface which will be referred to as a screen. Under the assumption of the local finite energy of the unified thermoelastic scattered field, we give a weak model on the appropriate Sobolev spaces and derive equivalent integral equations of the first kind for the jump of some trace operators on the open surface. Uniqueness and existence theorems are proved, the regularity and the singular behaviour of the solution near… Show more

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Cited by 9 publications
(7 citation statements)
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“…The direct TESP to be considered in this paper is to determine the displacement field u and the temperature variation field p satisfying (2.6), the boundary condition (2.7) and the Kupradze radiation conditions. For given F ∈ (H −1/2 (Γ)) 4 , we refer to [7,22] for the uniqueness of the direct problem.…”
Section: Thermoelastic Scattering Problem (Tesp)mentioning
confidence: 99%
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“…The direct TESP to be considered in this paper is to determine the displacement field u and the temperature variation field p satisfying (2.6), the boundary condition (2.7) and the Kupradze radiation conditions. For given F ∈ (H −1/2 (Γ)) 4 , we refer to [7,22] for the uniqueness of the direct problem.…”
Section: Thermoelastic Scattering Problem (Tesp)mentioning
confidence: 99%
“…For the TESP, it follows from the potential theory ( [7,22]) that the unknown function U can be represented as…”
Section: Bie For Tespmentioning
confidence: 99%
“…where the upper left 3 3 block of the matrix (2.6) is an elliptic differential operator, and Q I the identity dyadic in R 3 (the from now on in this paper will denote dyadics). Also in (2.5), the differential operator L is given by [3] L D…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…In the sequel, we will use a Betti's theorem arising from thermoelasticity theory [3]. In particular, for every U, We now employ the following Twersky's notation: for every U, V 2 C 2 .D/ Using asymptotic analysis of the fundamental solution of the Navier equation [9] expressions of the far-field patterns are obtained:…”
Section: Integral Representations and Far-field Patternsmentioning
confidence: 99%
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