1986
DOI: 10.1016/0022-5096(86)90033-5
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On material representation and constitutive branching in finite compressible elasticity

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Cited by 150 publications
(76 citation statements)
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“…We also make use of the hyperfoam strain energy function (Hill 1978, Lei andSzeri, 2007b). (Hill, 1978;Storakers, 1986) is (12) where λ 1 , λ 2 , λ 3 are the principal stretches, J = detF is the ratio of deformed to original volume at a point, while the constants μ, α and β relate to the initial aggregate modulus and Poisson's ratio through (13) The constants α and β define the nonlinearity of the material.…”
Section: Constitutive Equationsmentioning
confidence: 99%
“…We also make use of the hyperfoam strain energy function (Hill 1978, Lei andSzeri, 2007b). (Hill, 1978;Storakers, 1986) is (12) where λ 1 , λ 2 , λ 3 are the principal stretches, J = detF is the ratio of deformed to original volume at a point, while the constants μ, α and β relate to the initial aggregate modulus and Poisson's ratio through (13) The constants α and β define the nonlinearity of the material.…”
Section: Constitutive Equationsmentioning
confidence: 99%
“…MooneyRivlin model and Van der Waals model). The Ogden model [24,25] is a more general energetic model which is supposed to be composed of multiple Green Lagrange generalized models. These energetic models confirm the nonlinear elastic behaviour of foam undergoing large deformation.…”
Section: Symbolsmentioning
confidence: 99%
“…Truly, rubber-like materials are also almost incompressible, having a very high bulk modulus or, equivalently, a value for Poisson's ratio of approximately 0)5 but hyperelastic theory has been extended to admit compressibility, giving what is known as a hyperfoam. Storakers (1986) thus developed the strain-energy functional ; as…”
Section: Hyperelasticitymentioning
confidence: 99%