1996
DOI: 10.1070/pu1996v039n10abeh000173
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Macroscopic conductivity of random inhomogeneous media. Calculation methods

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Cited by 14 publications
(10 citation statements)
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“…Still, we must stress the large volume of literature produced in a number of disciplines with the aim of finding representative parameters in the theory of conductive media. Such disciplines would include electrical conductivity (see, e.g., Fokin [1996] for a review and Kaganova [2003]), thermal conductivity [e.g., Caldimi and Mahajan , 1999; Boomsma and Poulikakos , 2001], galvanomagnetic conductivity [e.g., Kaganova and Kaganov , 2004; Bergman and Stroud , 2000], and electronic conductivity [e.g., Du et al , 2004].…”
Section: Introductionmentioning
confidence: 99%
“…Still, we must stress the large volume of literature produced in a number of disciplines with the aim of finding representative parameters in the theory of conductive media. Such disciplines would include electrical conductivity (see, e.g., Fokin [1996] for a review and Kaganova [2003]), thermal conductivity [e.g., Caldimi and Mahajan , 1999; Boomsma and Poulikakos , 2001], galvanomagnetic conductivity [e.g., Kaganova and Kaganov , 2004; Bergman and Stroud , 2000], and electronic conductivity [e.g., Du et al , 2004].…”
Section: Introductionmentioning
confidence: 99%
“…While our overarching goal is the treatment of fullfield data pertaining to solid mechanics, the proposed method is discussed here in the context of the scalar conductivity model which has the same mathematical structure as the elasticity model yet avoids resorting to tensorial notations. Note that a Fourier-based forward solution method corresponding to this model is discussed in [24,25]. In [26, ch.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, if we calculate ECT up to the terms independent of the small parameter 1/H only, with respect to laboratory axes LCT is σ ik (H, r) = S( κ, r)δ i3 δ k3 . We can describe such a medium as a set of plane-parallel layers perpendicular to the direction of the magnetic field H. It is known (see, e.g., [1]) that in such a medium the value of the effective conductivity is equal to the inverse the averaged resistivity. This is just our answer for σ ef || .…”
Section: Ikmentioning
confidence: 99%
“…However, in the general case this problem has not been solved yet. In this Introduction we do not pretend to give the full list of references, but refer the readers to the review paper by A.G.Fokin [1], where the long list of references relating to different aspects of the problem is presented. We concentrate mainly on the known exact solutions for the effective conductivity tensor (ECT).…”
Section: Introductionmentioning
confidence: 99%
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