“…Also, Ω E represents spin of the Eulerian triad which is called the Eulerian spin. The logarithmic spin has a specific property such that its corresponding corotational rate of lnV results in the rate of deformation tensor D. This spin has been introduced seperately by Lehman et al [15], Reinhardt and Dubey [21,22] and Xiao et al [28,29]. Some useful details on this issue are given in [30].…”
Section: Preliminariesmentioning
confidence: 97%
“…of e ( f ) should be determined by use of (63), (21) and (22). With α f 1 ; α f 2 in hand, tensor K is adjusted to the appropriate one.…”
Section: Basis-free Expression In the Case Of Distinct Principal Strementioning
In the present paper, some new basis-free expressions for an arbitrary objective corotational rate of the general Eulerian strain measures are provided which are in compact form. Moreover, a complete discussion on the requirements for the continuity of the objective corotational rates are presented.
“…Also, Ω E represents spin of the Eulerian triad which is called the Eulerian spin. The logarithmic spin has a specific property such that its corresponding corotational rate of lnV results in the rate of deformation tensor D. This spin has been introduced seperately by Lehman et al [15], Reinhardt and Dubey [21,22] and Xiao et al [28,29]. Some useful details on this issue are given in [30].…”
Section: Preliminariesmentioning
confidence: 97%
“…of e ( f ) should be determined by use of (63), (21) and (22). With α f 1 ; α f 2 in hand, tensor K is adjusted to the appropriate one.…”
Section: Basis-free Expression In the Case Of Distinct Principal Strementioning
In the present paper, some new basis-free expressions for an arbitrary objective corotational rate of the general Eulerian strain measures are provided which are in compact form. Moreover, a complete discussion on the requirements for the continuity of the objective corotational rates are presented.
“…Here, e 8 Log is the logarithmic rate of the strain tensor e as specified in Equation (16). From the symmetry requirement of t and e, and the objectivity of t and _ w w, it is concluded that the extended work conjugacy relation (27) holds only for objective corotational rates e 8 * [11].…”
Section: Work Conjugacy and Work Conjugated Stressmentioning
. BruhnsA thermodynamic model describing pseudoelasticity is proposed. The kinematics are based on a self-consistent Eulerian theory of finite deformations using the logarithmic rate. The thermomechanical state of the material is described by means of the mass fraction of martensite as internal state variable. From the Helmholtz free energy of the two-phase solid, a kinetic law for the evolution of martensite is derived, taking into account the heat generated during phase transition. The material model is implemented into a finite element code in an updated Lagrangian scheme. Its parameters are calibrated to experimental data. The characteristics of the model are illustrated by simulations under different loading conditions.
At the beginning of the last century two different types of constitutive relations to describe the complex behavior of elastoplastic material were presented. These were the deformation theory originally developed by Hencky and the Prandtl-Reuss theory. Whereas the former provides a direct solid-like relation of stress as function of strain, the latter has been based on an additive composition of elastic and plastic parts of the increments of strains. These in turn were taken as a solid-and fluid-like combination of the de Saint-Venant/Lévy theory with an incremental form of Hookes law.Even nowadays this Prandtl-Reuss theory is still accepted within the restriction of small elastic deformations, i.e. it is generally stated in most textbooks on plasticity that this theory due to a number of defects can not be applied to large deformations. In the present article it is shown that this restrictive statement may be no longer true. Introducing a specific objective time derivative it could be shown that these defects disappear.
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