1998
DOI: 10.1088/0266-5611/14/2/007
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Hartig's law and linear elasticity with initial stress

Abstract: The two constitutive equations which have hitherto been called upon in mathematical studies on static determination of residual stress by boundary measurements share the same deficiency, namely that they do not adequately describe the elastic response of any currently known real material. Here we substantiate this critical remark and present a physically more acceptable constitutive equation for further work on the subject.

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Cited by 55 publications
(50 citation statements)
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“…Man [Man98] proposes for elastodynamics with residual stress R a more general constituitive law S = R + ∇u · R + CE where the elasticity tensor C also depends linearly on R. In the isotropic case CE consists of the right-hand side in (3) plus the R dependent terms β 1 tr(E) tr(R)I + β 2 tr(R)E + β 3 tr(E)R + tr(ER)I + β 4 ER + RE .…”
Section: Isotropic Elastodynamic Equationsmentioning
confidence: 99%
“…Man [Man98] proposes for elastodynamics with residual stress R a more general constituitive law S = R + ∇u · R + CE where the elasticity tensor C also depends linearly on R. In the isotropic case CE consists of the right-hand side in (3) plus the R dependent terms β 1 tr(E) tr(R)I + β 2 tr(R)E + β 3 tr(E)R + tr(ER)I + β 4 ER + RE .…”
Section: Isotropic Elastodynamic Equationsmentioning
confidence: 99%
“…The characterization of the stress-dependence in N was first given by Turner and Ghoshal 17 and later demonstrated experimentally by Kube et al 18,19 The present theory utilizes a more commonly used elastic constitutive relation, [31][32][33][34][35][36][37] which is valid for both residual and mechanical stresses. This constitutive relation leads to different stress-dependent elastic properties than those given by Turner and Ghoshal.…”
Section: Theorymentioning
confidence: 96%
“…A set of invariants equivalent to the above has been used by [Hoger 1993a;1996]. For related work concerned with the constitutive equations and material symmetry for a residually stressed elastic material we refer to [Coleman and Noll 1964;Hoger 1986;1993b;Man and Lu 1987;Johnson and Hoger 1993;Man 1998;Saravanan 2008;Tanuma and Man 2008]. We have not for the moment defined particular notation for the invariants (25)-(27).…”
Section: Equations Of Motionmentioning
confidence: 99%