2014
DOI: 10.1016/j.ijsolstr.2014.03.036
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The effective elastic moduli of columnar composites made of cylindrically anisotropic phases with rough interfaces

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Cited by 5 publications
(4 citation statements)
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“…The present work aims to solve, in the situation of thermal conduction, the problem of determining the effective conductivity of composite materials in which the interface between any constituent phases oscillates quickly and periodically about an arbitrarily curved surface and along two directions. Thus, the present work can be considered as a continuation and an extension of our previous ones [7][8][9][10].…”
Section: Introductionmentioning
confidence: 63%
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“…The present work aims to solve, in the situation of thermal conduction, the problem of determining the effective conductivity of composite materials in which the interface between any constituent phases oscillates quickly and periodically about an arbitrarily curved surface and along two directions. Thus, the present work can be considered as a continuation and an extension of our previous ones [7][8][9][10].…”
Section: Introductionmentioning
confidence: 63%
“…In the work of Le-Quang et al [7], it was shown that, when the rough interface oscillates quickly and periodically along only one direction, the effective properties of the equivalent interphase obtained by homogenizing an interface zone correspond exactly to the ones of a two-phase layered composite material. In addition, the determination of effective properties of composite materials while accounting for interfacial roughness has been carried out in the contexts of elasticity and thermal conduction [7][8][9][10]. the results obtained in these works are limited to the cases where rough interfaces oscillate either along one direction around a curved surface [7][8][9] or along two directions but around a plane surface [10].…”
Section: Introductionmentioning
confidence: 99%
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“…Following Bensoussan et al [14], Sanchez-Palencia [15], and Bakhvalov and Panasenko [16], we suppose that: boldv ( x 1 , x 3 , ϵ ) = boldU ( x 1 , y , x 3 , ϵ ) . Following Bakhvalov and Panasenko [16], we express boldU as follows (see also, Vinh and Tung [1923], Le et al [28], Le Quang et al [29, 30], and Nguyen et al [31]):…”
Section: Explicit Homogenized Equation In Matrix Formmentioning
confidence: 99%