2019
DOI: 10.1177/1081286519888970
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Steady vibration problems in the coupled linear theory of porous elastic solids

Abstract: This paper concerns the coupled linear theory of elasticity for isotropic porous materials. In this theory the coupled phenomena of the concepts of Darcy’s law and the volume fraction is considered. The basic internal and external boundary value problems (BVPs) of steady vibrations are investigated. Indeed, the fundamental solution of the system of steady vibration equations is constructed explicitly by means of elementary functions, and its basic properties are presented. The radiation conditions are establis… Show more

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Cited by 14 publications
(8 citation statements)
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“…If supposing that h and j h are known functions, taking into account the representations (8), to define the displacement vector u from Eq. , ) 1 ( 1 we get the following non-homogeneous equation , ) 1 ( grad…”
Section: A Representation Of Regular Solutionmentioning
confidence: 99%
See 2 more Smart Citations
“…If supposing that h and j h are known functions, taking into account the representations (8), to define the displacement vector u from Eq. , ) 1 ( 1 we get the following non-homogeneous equation , ) 1 ( grad…”
Section: A Representation Of Regular Solutionmentioning
confidence: 99%
“…The generalization of the theory of elasticity and thermoelasticity for materials with double voids belongs to Ieşan and Quintanilla (2014) [7]. In (2020) [8] Svanadze considered the coupled linear model of porous elastic solids by combining the following three variables: the displacement vector field, the volume fraction of pores and the change of fluid pressure in pore network. In this work the basic internal and external BVPs of steady vibrations are investigated, the uniqueness and the existence theorems are proved by means of the potential method and the theory of singular integral equations.…”
Section: Introductionmentioning
confidence: 99%
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“…y, 0) = u 0 (x, y), at t = 0 and in , u t (x, y, 0) = u 1 (x, y), at t = 0 and in , (1) where is an interconnected domian with bounded boundary ∂ , = ∪∂ , J = [0, T ], T is the final moment, f (x, y, t) is the given sufficiently smooth source function, g 1 (x, y, t), g 2 (x, y, t), u 0 (x, y) and u 1 (x, y) are given sufficiently smooth boundary functions and initial functions respectively.…”
Section: Introductionmentioning
confidence: 99%
“…The 2D fourth-order hyperbolic equation is an important partial differential equation describing vibration or wave phenomena, which has important application value in aerospace, petroleum exploration, urban construction, crustal sounding and so on [1], [2], [3]. For practical problems, due to the complexity of the physical problem itself and the solution region, it is often difficult to obtain the exact solution of the problem (1). In the last few years, many scholars have deeply studied the numerical solution of the problem (1) and put forward a variety of numerical calculation methods.…”
Section: Introductionmentioning
confidence: 99%