2021
DOI: 10.1016/j.ijmecsci.2021.106759
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A continuum-molecular model for anisotropic electrically conductive materials

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Cited by 11 publications
(19 citation statements)
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“…where, under the assumed conditions, the pairwise deformations s( ) and ( ) of the generic virtual fiber can be expressed as linear functions of the homogeneous macro strain components ij and quadratic functions of the direction cosines of the orthonormal unit vectors = n i i and = t i i (as previously defined), by which are obtained through the Cauchy-Born rule [87,88], particularized to our case 4 , and according to ε = 𝜺 , where is given by Eq. 44 [72,76]. Hence, one obtains Substituting Eq.…”
Section: Micro-macro Moduli Correspondencementioning
confidence: 98%
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“…where, under the assumed conditions, the pairwise deformations s( ) and ( ) of the generic virtual fiber can be expressed as linear functions of the homogeneous macro strain components ij and quadratic functions of the direction cosines of the orthonormal unit vectors = n i i and = t i i (as previously defined), by which are obtained through the Cauchy-Born rule [87,88], particularized to our case 4 , and according to ε = 𝜺 , where is given by Eq. 44 [72,76]. Hence, one obtains Substituting Eq.…”
Section: Micro-macro Moduli Correspondencementioning
confidence: 98%
“…In non-local models of this kind, the representative cell is the horizon region H over the integral in Eq. 11 is defined, while the micro-macro moduli correspondence principle is based on a micro-macro energy equivalence, which allows macroscopic properties to be directly associated to microscale-defined constitutive laws [72]. Since in-plane Cauchy anisotropic linear elasticity is defined by six independent elastic moduli, it follows that k n ( ) and k t ( ) must be functions of at least six independent microelastic constants.…”
Section: Anisotropic Elastic Pair Potentials and Materials Micromodulimentioning
confidence: 99%
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