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/dports/science/tfel/tfel-3.4.0/docs/tutorial/mfront/
H A DEllipticCreep-1b.mfront15 // equivalent deviatoric viscoplastic strain
99 // deviatoric part
H A DEllipticCreep-1.mfront15 // equivalent deviatoric viscoplastic strain
99 // deviatoric part
H A DEllipticCreep-2.mfront16 // equivalent deviatoric viscoplastic strain
100 // deviatoric part
H A DEllipticCreep-final.mfront15 // equivalent deviatoric viscoplastic strain
94 // deviatoric part
/dports/science/tfel/tfel-3.4.0/mfront/tests/behaviours/
H A DEllipticCreep.mfront15 /*! equivalent deviatoric viscoplastic strain */
79 // deviatoric part
H A DGeneralizedMaxwell.mfront40 Stensor devsej = deviator(sej[i]); // deviatoric part
/dports/science/tfel-edf/tfel-3.2.1/mfront/tests/behaviours/
H A DEllipticCreep.mfront15 /*! equivalent deviatoric viscoplastic strain */
79 // deviatoric part
H A DGeneralizedMaxwell.mfront40 Stensor devsej = deviator(sej[i]); // deviatoric part
/dports/science/tfel-edf/tfel-3.2.1/docs/tutorial/mfront/
H A DEllipticCreep-1b.mfront15 // equivalent deviatoric viscoplastic strain
99 // deviatoric part
H A DEllipticCreep-2.mfront16 // equivalent deviatoric viscoplastic strain
100 // deviatoric part
H A DEllipticCreep-1.mfront15 // equivalent deviatoric viscoplastic strain
99 // deviatoric part
H A DEllipticCreep-final.mfront15 // equivalent deviatoric viscoplastic strain
94 // deviatoric part
/dports/science/tfel/tfel-3.4.0/docs/web/
H A Drelease-notes-3.2.md124 …he invariants of the stress deviator tensor with respect to the stress {#sec:deviatoric:invariants}
126 Let \(\tsigma\) be a stress tensor. Its deviatoric part
149 *deviatoric stress invariants*, respectively. Their values are the same
151 chosen. These deviatoric stress invariants can be expressed as a
230 invariants of the deviatoric part \(\tenseur{s}\) of the stress tensor
231 \(\tsigma\) (see also Section @sec:deviatoric:invariants):
244 Section @sec:deviatoric:invariants).
252 Section @sec:deviatoric:invariants for details).
255 `tfel::math` namespace (see Section @sec:deviatoric:invariants
261 to anisotropic conditions of the invariants of the deviatoric stress
[all …]
H A DIsotropicLinearHardeningPlasticity.md79 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
132 and projected on the deviatoric space as follows:
138 The isotropy of the elastic behaviour projected on the deviatoric space leads to:
156 The right hand side is the value of the deviatoric part of the stress
H A DRambergOsgoodNonLinearElasticity.md58 the deviatoric part of the stress tensor.
77 Taking the deviatoric part of Equation @eq:sigeto yields:
279 //! normal associated with the deviatoric part of the strain
345 deviatoric part, the equivalent strain and the normal.
H A Dtensors.md191 is tensor is indeed the projector on the deviatoric space.
218 is tensor is indeed the projector on the deviatoric space.
650 ## Invariants of the stress deviator tensor @wikipedia_invariants_2017 {#sec:deviatoric:invariants}
652 Let \(\tsigma\) be a stress tensor. Its deviatoric part
674 *deviatoric stress invariants*, respectively. Their values are the same
676 chosen. These deviatoric stress invariants can be expressed as a
700 The invariants \(J_{2}\) and \(J_{3}\) of deviatoric part of the
809 ## Orthotropic generalization of the invariants of the stress deviator tensor {#sec:deviatoric:orth…
812 to orthotropic conditions of the invariants of the deviatoric stress
1022 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
[all …]
H A Dsovs.md105 - \(\tenseur{s}\) is the deviatoric stress tensor.
130 By projecting Equation @eq:viscosity on the hydrostatic and deviatoric
140 where \(\tenseur{s}_{\tdepsilonin}\) stands for the deviatoric part of \(\tdepsilonin\).
391 Since the deviatoric part of the inelastic strain is linear with the
615 To express the viscoplastic flow, one need the deviatoric part of the
/dports/science/tfel-edf/tfel-3.2.1/docs/web/
H A Drelease-notes-3.2.md122 …he invariants of the stress deviator tensor with respect to the stress {#sec:deviatoric:invariants}
124 Let \(\tsigma\) be a stress tensor. Its deviatoric part
147 *deviatoric stress invariants*, respectively. Their values are the same
149 chosen. These deviatoric stress invariants can be expressed as a
228 invariants of the deviatoric part \(\tenseur{s}\) of the stress tensor
229 \(\tsigma\) (see also Section @sec:deviatoric:invariants):
242 Section @sec:deviatoric:invariants).
250 Section @sec:deviatoric:invariants for details).
253 `tfel::math` namespace (see Section @sec:deviatoric:invariants
259 to anisotropic conditions of the invariants of the deviatoric stress
[all …]
H A Dtensors.md182 is tensor is indeed the projector on the deviatoric space.
209 is tensor is indeed the projector on the deviatoric space.
599 ## Invariants of the stress deviator tensor @wikipedia_invariants_2017 {#sec:deviatoric:invariants}
601 Let \(\tsigma\) be a stress tensor. Its deviatoric part
623 *deviatoric stress invariants*, respectively. Their values are the same
625 chosen. These deviatoric stress invariants can be expressed as a
649 The invariants \(J_{2}\) and \(J_{3}\) of deviatoric part of the
758 ## Orthotropic generalization of the invariants of the stress deviator tensor {#sec:deviatoric:orth…
761 to orthotropic conditions of the invariants of the deviatoric stress
945 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
[all …]
H A DStandardElastoViscoPlasticityBrick.md222 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
255 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
313 - \(\tenseur{s}\) is the deviatoric stress defined as follows:
372 to orthotropic conditions of the invariants of the deviatoric stress
/dports/graphics/gmt/gmt-6.3.0/doc/rst/source/supplements/seis/
H A Dexplain_meca_-S.rst_78 **-Sz** plots the deviatoric part of the moment tensor (zero trace).
80 Global CMT moment tensors are deviatoric, so **-Sm** and **-Sz** will produce the same result,
140 Use **-St** to plot the deviatoric part of the moment tensor (zero trace).
/dports/science/lammps/lammps-stable_29Sep2021/src/MACHDYN/
H A DREADME11 strength models, i.e. pressure and deviatoric stresses are separated.
/dports/cad/calculix-ccx/CalculiX/ccx_2.18/test/
H A Dlin_stat_twisted_beam.inp9 ** assumed natural deviatoric strain approaches
/dports/science/tfel/tfel-3.4.0/docs/gallery/behaviours/nonlinearelasticity/
H A DRambergOsgoodNonLinearElasticity.mfront46 //! normal associated with the deviatoric part of the strain
/dports/science/quantum-espresso/q-e-qe-6.7.0/Modules/
H A DMakefile157 deviatoric.o

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