2011
DOI: 10.1016/j.euromechsol.2011.02.001
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Eshebly tensors for a finite spherical domain with an axisymmetric inclusion

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Cited by 12 publications
(13 citation statements)
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“…β 0 (δ ik t l t j + δ il t k t j + δ jk t l t i + δ jl t k t i ), (3.8) where I ijkl = 1 2 (δ ik δ jl + δ il δ jk ) is the fourth-order unit tensor. It can be proved that (3.8) coincides with the results in Li et al [8], except for a sign misprint of the second term, as pointed out by Mejak [14].…”
Section: )supporting
confidence: 83%
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“…β 0 (δ ik t l t j + δ il t k t j + δ jk t l t i + δ jl t k t i ), (3.8) where I ijkl = 1 2 (δ ik δ jl + δ il δ jk ) is the fourth-order unit tensor. It can be proved that (3.8) coincides with the results in Li et al [8], except for a sign misprint of the second term, as pointed out by Mejak [14].…”
Section: )supporting
confidence: 83%
“…It is easy to prove that our formula (3.2) is the same as equation (80) of Li et al [8]. Combination being made with the first order part of (2.33), namely 5) the solution (3.3) results in the first-order Eshelby tensor field which can be shown to be identical to that given by Mejak [14]. = α 0 7 − 5ν 10…”
Section: )supporting
confidence: 55%
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“…Subsequently, based on the elasticity theory of a simplified strain gradient, Gao et.al [33] and Ma et.al [34] tested the similar problems and extended the solutions in the framework of high-order elasticity theory. Mejak [35] studied axisymmetrically placed inclusion in a sphere and found the Dirichlet-Eshelby tensor of an eccentric spherical inclusion through the power series expansion. Research on arbitrarily-shaped inclusion problems studied by Zou [36] is quite significant.…”
Section: Introductionmentioning
confidence: 99%