2019
DOI: 10.1016/j.jmps.2019.05.011
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Elastic Kelvin-Poisson-Poynting solids described through scalar conjugate stress/strain pairs derived from a QR factorization of

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Cited by 12 publications
(10 citation statements)
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“…(2.6) Greek indices α = 1, 2, 3 correspond to an intermediate configuration whose tangent vectors are pulled back from the spatial configuration by Q −1 or pushed forward from the reference configuration by T . The same global Cartesian basis is used for this configuration, called the "physical configuration" in [40]: Physically descriptive deformation measures are the three positive elongation ratios a, b, c that enter the extension matrix Λ and the three shear magnitudes α, β, γ that enter the simple shear matrix Γ . Volume change is measured by J = det T = det Λ = abc.…”
Section: Kinematics Of Finite Deformationmentioning
confidence: 99%
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“…(2.6) Greek indices α = 1, 2, 3 correspond to an intermediate configuration whose tangent vectors are pulled back from the spatial configuration by Q −1 or pushed forward from the reference configuration by T . The same global Cartesian basis is used for this configuration, called the "physical configuration" in [40]: Physically descriptive deformation measures are the three positive elongation ratios a, b, c that enter the extension matrix Λ and the three shear magnitudes α, β, γ that enter the simple shear matrix Γ . Volume change is measured by J = det T = det Λ = abc.…”
Section: Kinematics Of Finite Deformationmentioning
confidence: 99%
“…Volume change is measured by J = det T = det Λ = abc. Parameters a, b, c, α, β, γ are physical attributes because they can be measured directly by an experimentalist in the physical coordinate system of later (2.12), without post analysis [38,40,41]. Let C = F T F = T T T = C IJ e I ⊗ e J = F i I δ ij F j J e I ⊗ e J = T α I δ αβ T β J e I ⊗ e J (2.9) denote the symmetric right Cauchy-Green deformation tensor.…”
Section: Kinematics Of Finite Deformationmentioning
confidence: 99%
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