1982
DOI: 10.21236/ada120958
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On the Relationship between the Logarithmic Strain Rate and the Stretching Tensor.

Abstract: In this paper we investigate the relationship between the stretching tensor 2 and the logarithmic (Hencky) strain Any, with V the left stretch tensor. We establish the simple formula (AnV)-sym (j3l), which holds for arbitrary three-dimensional motions. Here F is the deformation gradient, (1n)) 0 is the time derivative of Any measured in a coordinate system which rotates with the left principal strain axes, and Nr is the spin of the right principal strain axes. we use this formula to show that 2-(tnV), (or, equ… Show more

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Cited by 7 publications
(9 citation statements)
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“…Für Quaderverformungen ist die Zeitrate des Tensors der logarithmischen Verzerrungen italicdε italicdt = ε ˙ gleich dem Stretchingtensor . Allgemein gilt für kleine Verzerrungen: D ≈ ε̇ .…”
Section: Begriffe Und Notationunclassified
“…Für Quaderverformungen ist die Zeitrate des Tensors der logarithmischen Verzerrungen italicdε italicdt = ε ˙ gleich dem Stretchingtensor . Allgemein gilt für kleine Verzerrungen: D ≈ ε̇ .…”
Section: Begriffe Und Notationunclassified
“…The logarithmic description 1 is arguably the simplest approach to finite plasticity, suitable for the phenomenological description of isotropic polycrystalline metals if the structure of geometrically linear theories is used with respect to the Lagrangian logarithmic strain. In this paper we do not consider hypoelastic-plastic models [72,22,43,96] in which, contrary to hyperelastic models, the potential character of the elastic energy is ignored [42,52]. Otherwise, they are simply the hyperelastic models rewritten in a suitable incremental form.…”
Section: Preliminariesmentioning
confidence: 99%
“…For the large deformation of isotropic elastic bodies, we adopt the following elastic constitutive equations : bold-italicTMathClass-rel=bold-italicCMathClass-punc:bold-italicE2.56804pttmspace(i.e.,1emnbsp1emnbsptruebold-italicT̈MathClass-rel=bold-italicCMathClass-punc:bold-italicD)MathClass-punc, where T is the Cauchy stress tensor, E is the Hencky strain tensor, truebold-italicT̈ is the Jaumann rate of the Cauchy stress, D is the stretching tensor, and C is the fourth order elasticity tensor described as CijklMathClass-rel=λδijδklMathClass-bin+2μδikδjlMathClass-punc, where λ and μ are the Lame's parameters.…”
Section: Constitutive Equationsmentioning
confidence: 99%