2015
DOI: 10.1093/qjmam/hbv012
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The shape of Maxwell's equivalent inhomogeneity and ‘strange’ properties of regular polygons and other symmetric domains

Abstract: The Maxwell concept of equivalent inhomogeneity is reexamined in the context of elastic composite, porous or micro-cracked materials of periodic structure. It is demonstrated that accurate estimates for the effective elastic properties can be obtained by the modified Maxwell approach that employs the proper shape of the equivalent inhomogeneity and explicitly accounts for the geometry of the cluster and for the interactions between its constituents. In addition, it is shown that regular polygonal and some othe… Show more

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Cited by 2 publications
(6 citation statements)
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“…The solutions based on conformal mapping were utilized by Zimmerman (1986), Zimmerman (1991), Kachanov et al (1994), Jasiuk et al (1994), Tsukrov and Novak (2002), Ekneligoda and Zimmerman (2006), Ekneligoda and Zimmerman (2008), Zou et al (2010), Mogilevskaya and Nikolskiy (2015) . In 3D, Garboczi and Douglas (2012) presented a procedure to approximate bulk and shear elastic contribution parameters in the case of randomly oriented inhomogeneities shaped as blocks.…”
Section: Introductionmentioning
confidence: 99%
“…The solutions based on conformal mapping were utilized by Zimmerman (1986), Zimmerman (1991), Kachanov et al (1994), Jasiuk et al (1994), Tsukrov and Novak (2002), Ekneligoda and Zimmerman (2006), Ekneligoda and Zimmerman (2008), Zou et al (2010), Mogilevskaya and Nikolskiy (2015) . In 3D, Garboczi and Douglas (2012) presented a procedure to approximate bulk and shear elastic contribution parameters in the case of randomly oriented inhomogeneities shaped as blocks.…”
Section: Introductionmentioning
confidence: 99%
“…The coefficient in the first term of expansion of equation (6.1) represents the resultant force acting on the boundary of the inhomogeneity, while the coefficient in the second term (dipole coefficient) of that expansion is equal to [1] …”
Section: Discussionmentioning
confidence: 99%
“…(ii) A part of L is a straight segment with the beginning at the point a = a 1 + ib 1 and the end at the point b = b 1 + ib 1 .…”
Section: (B) Deviatoric Eigenstrainmentioning
confidence: 99%
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