2021-04-23 22:50:07 +05:30
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|
|
|
"""
|
|
|
|
|
Finite-strain continuum mechanics.
|
|
|
|
|
|
2021-04-24 10:43:36 +05:30
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|
|
All routines operate on numpy.ndarrays of shape (...,3,3).
|
2021-04-23 22:50:07 +05:30
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|
|
|
|
|
|
|
|
"""
|
2020-11-16 03:44:46 +05:30
|
|
|
|
|
2020-11-19 18:35:59 +05:30
|
|
|
|
from . import tensor as _tensor
|
2020-11-20 03:06:19 +05:30
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|
|
|
from . import _rotation
|
2020-11-16 03:44:46 +05:30
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|
|
|
|
2020-04-10 16:00:39 +05:30
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|
|
import numpy as _np
|
2019-10-19 00:20:03 +05:30
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|
2020-11-16 03:44:46 +05:30
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|
2020-11-18 03:26:22 +05:30
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|
def deformation_Cauchy_Green_left(F):
|
2019-10-30 22:35:44 +05:30
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|
"""
|
2020-11-16 05:31:32 +05:30
|
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|
|
Calculate left Cauchy-Green deformation tensor (Finger deformation tensor).
|
2020-02-15 18:26:15 +05:30
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|
2019-10-30 22:35:44 +05:30
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Parameters
|
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|
|
|
----------
|
2020-06-10 00:57:08 +05:30
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|
F : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
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|
Deformation gradient.
|
2020-11-16 05:31:32 +05:30
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Returns
|
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|
|
-------
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|
|
B : numpy.ndarray of shape (...,3,3)
|
2020-11-19 19:08:54 +05:30
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|
Left Cauchy-Green deformation tensor.
|
2019-10-30 22:35:44 +05:30
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"""
|
2020-11-19 18:35:59 +05:30
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|
return _np.matmul(F,_tensor.transpose(F))
|
2019-11-27 16:49:37 +05:30
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|
2020-11-18 03:26:22 +05:30
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def deformation_Cauchy_Green_right(F):
|
2019-11-27 16:49:37 +05:30
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|
"""
|
2020-11-16 05:31:32 +05:30
|
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|
|
Calculate right Cauchy-Green deformation tensor.
|
2020-02-15 18:26:15 +05:30
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|
2019-11-27 16:49:37 +05:30
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Parameters
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|
|
----------
|
2020-11-16 05:31:32 +05:30
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|
F : numpy.ndarray of shape (...,3,3)
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|
|
Deformation gradient.
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|
Returns
|
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|
-------
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|
|
C : numpy.ndarray of shape (...,3,3)
|
2020-11-19 19:08:54 +05:30
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|
Right Cauchy-Green deformation tensor.
|
2019-11-27 16:49:37 +05:30
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|
|
"""
|
2020-11-19 18:35:59 +05:30
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|
|
return _np.matmul(_tensor.transpose(F),F)
|
2020-11-16 05:31:32 +05:30
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|
2020-11-18 03:26:22 +05:30
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|
def equivalent_strain_Mises(epsilon):
|
2019-10-30 22:35:44 +05:30
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|
"""
|
2020-11-16 05:31:32 +05:30
|
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|
|
Calculate the Mises equivalent of a strain tensor.
|
2020-02-15 18:26:15 +05:30
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|
2019-10-30 22:35:44 +05:30
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|
Parameters
|
|
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|
|
----------
|
2020-06-10 00:57:08 +05:30
|
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|
|
epsilon : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
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|
Symmetric strain tensor of which the von Mises equivalent is computed.
|
2019-10-19 16:40:46 +05:30
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|
2020-11-16 05:31:32 +05:30
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|
Returns
|
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|
-------
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|
|
epsilon_vM : numpy.ndarray of shape (...)
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|
Von Mises equivalent strain of epsilon.
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|
2019-10-30 22:35:44 +05:30
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|
"""
|
2020-11-18 03:26:22 +05:30
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|
return _equivalent_Mises(epsilon,2.0/3.0)
|
2019-10-19 16:24:16 +05:30
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|
2020-11-18 03:26:22 +05:30
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|
def equivalent_stress_Mises(sigma):
|
2019-10-30 22:35:44 +05:30
|
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|
"""
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Calculate the Mises equivalent of a stress tensor.
|
2020-02-15 18:26:15 +05:30
|
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|
2019-10-30 22:35:44 +05:30
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|
Parameters
|
|
|
|
|
----------
|
2020-06-10 00:57:08 +05:30
|
|
|
|
sigma : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
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|
|
Symmetric stress tensor of which the von Mises equivalent is computed.
|
2019-10-19 16:40:46 +05:30
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|
2020-11-16 05:31:32 +05:30
|
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|
Returns
|
|
|
|
|
-------
|
|
|
|
|
sigma_vM : numpy.ndarray of shape (...)
|
|
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|
|
Von Mises equivalent stress of sigma.
|
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|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-11-18 03:26:22 +05:30
|
|
|
|
return _equivalent_Mises(sigma,3.0/2.0)
|
2019-10-19 16:24:16 +05:30
|
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|
2020-11-19 18:35:59 +05:30
|
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|
|
def maximum_shear(T_sym):
|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-11-19 18:35:59 +05:30
|
|
|
|
Calculate the maximum shear component of a symmetric tensor.
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2019-10-30 22:35:44 +05:30
|
|
|
|
Parameters
|
|
|
|
|
----------
|
2020-11-19 18:35:59 +05:30
|
|
|
|
T_sym : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Symmetric tensor of which the maximum shear is computed.
|
2019-10-19 16:40:46 +05:30
|
|
|
|
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Returns
|
|
|
|
|
-------
|
2020-11-19 18:35:59 +05:30
|
|
|
|
gamma_max : numpy.ndarray of shape (...)
|
|
|
|
|
Maximum shear of T_sym.
|
2020-11-16 05:31:32 +05:30
|
|
|
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|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-11-19 18:35:59 +05:30
|
|
|
|
w = _tensor.eigenvalues(T_sym)
|
|
|
|
|
return (w[...,0] - w[...,2])*0.5
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2020-03-03 03:41:05 +05:30
|
|
|
|
|
2020-11-20 03:16:52 +05:30
|
|
|
|
def rotation(T):
|
2020-02-15 18:26:15 +05:30
|
|
|
|
"""
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Calculate the rotational part of a tensor.
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
2020-06-10 00:57:08 +05:30
|
|
|
|
T : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
|
|
|
|
Tensor of which the rotational part is computed.
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Returns
|
|
|
|
|
-------
|
2020-11-20 03:06:19 +05:30
|
|
|
|
R : damask.Rotation of shape (...)
|
|
|
|
|
Rotational part of the vector.
|
2020-11-16 05:31:32 +05:30
|
|
|
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|
2020-02-15 18:26:15 +05:30
|
|
|
|
"""
|
2020-11-20 03:06:19 +05:30
|
|
|
|
return _rotation.Rotation.from_matrix(_polar_decomposition(T,'R')[0])
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
|
|
|
|
|
2020-11-16 05:42:23 +05:30
|
|
|
|
def strain(F,t,m):
|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-11-16 05:42:23 +05:30
|
|
|
|
Calculate strain tensor (Seth–Hill family).
|
2020-02-15 18:40:16 +05:30
|
|
|
|
|
|
|
|
|
For details refer to https://en.wikipedia.org/wiki/Finite_strain_theory and
|
|
|
|
|
https://de.wikipedia.org/wiki/Verzerrungstensor
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2019-10-30 22:35:44 +05:30
|
|
|
|
Parameters
|
|
|
|
|
----------
|
2020-06-10 00:57:08 +05:30
|
|
|
|
F : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
|
|
|
|
Deformation gradient.
|
2020-02-15 18:40:16 +05:30
|
|
|
|
t : {‘V’, ‘U’}
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Type of the polar decomposition, ‘V’ for left stretch tensor
|
2020-11-19 19:08:54 +05:30
|
|
|
|
and ‘U’ for right stretch tensor.
|
2020-02-15 18:40:16 +05:30
|
|
|
|
m : float
|
2020-03-15 02:23:48 +05:30
|
|
|
|
Order of the strain.
|
2019-10-25 17:00:20 +05:30
|
|
|
|
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
epsilon : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Strain of F.
|
|
|
|
|
|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-02-15 18:40:16 +05:30
|
|
|
|
if t == 'V':
|
2020-11-18 03:26:22 +05:30
|
|
|
|
w,n = _np.linalg.eigh(deformation_Cauchy_Green_left(F))
|
2020-02-15 18:40:16 +05:30
|
|
|
|
elif t == 'U':
|
2020-11-18 03:26:22 +05:30
|
|
|
|
w,n = _np.linalg.eigh(deformation_Cauchy_Green_right(F))
|
2019-10-25 17:00:20 +05:30
|
|
|
|
|
2020-02-15 18:40:16 +05:30
|
|
|
|
if m > 0.0:
|
2020-11-16 11:42:37 +05:30
|
|
|
|
eps = 1.0/(2.0*abs(m)) * (+ _np.einsum('...j,...kj,...lj',w**m,n,n) - _np.eye(3))
|
2020-11-16 03:44:46 +05:30
|
|
|
|
|
2020-02-15 18:40:16 +05:30
|
|
|
|
elif m < 0.0:
|
2020-11-16 11:42:37 +05:30
|
|
|
|
eps = 1.0/(2.0*abs(m)) * (- _np.einsum('...j,...kj,...lj',w**m,n,n) + _np.eye(3))
|
2020-02-15 18:40:16 +05:30
|
|
|
|
else:
|
2020-11-16 11:42:37 +05:30
|
|
|
|
eps = _np.einsum('...j,...kj,...lj',0.5*_np.log(w),n,n)
|
2019-10-25 17:00:20 +05:30
|
|
|
|
|
2020-06-10 00:57:08 +05:30
|
|
|
|
return eps
|
2020-02-15 18:40:16 +05:30
|
|
|
|
|
|
|
|
|
|
2020-11-19 18:35:59 +05:30
|
|
|
|
def stress_Cauchy(P,F):
|
|
|
|
|
"""
|
|
|
|
|
Calculate the Cauchy stress (true stress).
|
|
|
|
|
|
|
|
|
|
Resulting tensor is symmetrized as the Cauchy stress needs to be symmetric.
|
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
P : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
First Piola-Kirchhoff stress.
|
|
|
|
|
F : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Deformation gradient.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
sigma : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Cauchy stress.
|
|
|
|
|
|
|
|
|
|
"""
|
|
|
|
|
return _tensor.symmetric(_np.einsum('...,...ij,...kj',1.0/_np.linalg.det(F),P,F))
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def stress_second_Piola_Kirchhoff(P,F):
|
|
|
|
|
"""
|
|
|
|
|
Calculate the second Piola-Kirchhoff stress.
|
|
|
|
|
|
|
|
|
|
Resulting tensor is symmetrized as the second Piola-Kirchhoff stress
|
|
|
|
|
needs to be symmetric.
|
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
P : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
First Piola-Kirchhoff stress.
|
|
|
|
|
F : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Deformation gradient.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
S : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Second Piola-Kirchhoff stress.
|
|
|
|
|
|
|
|
|
|
"""
|
|
|
|
|
return _tensor.symmetric(_np.einsum('...ij,...jk',_np.linalg.inv(F),P))
|
|
|
|
|
|
|
|
|
|
|
2020-11-16 05:31:32 +05:30
|
|
|
|
def stretch_left(T):
|
|
|
|
|
"""
|
2020-11-19 19:08:54 +05:30
|
|
|
|
Calculate left stretch of a tensor.
|
2020-11-16 05:31:32 +05:30
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
T : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Tensor of which the left stretch is computed.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
V : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Left stretch tensor from Polar decomposition of T.
|
|
|
|
|
|
|
|
|
|
"""
|
|
|
|
|
return _polar_decomposition(T,'V')[0]
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def stretch_right(T):
|
|
|
|
|
"""
|
2020-11-19 19:08:54 +05:30
|
|
|
|
Calculate right stretch of a tensor.
|
2020-11-16 05:31:32 +05:30
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
T : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Tensor of which the right stretch is computed.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
U : numpy.ndarray of shape (...,3,3)
|
|
|
|
|
Left stretch tensor from Polar decomposition of T.
|
|
|
|
|
|
|
|
|
|
"""
|
|
|
|
|
return _polar_decomposition(T,'U')[0]
|
|
|
|
|
|
|
|
|
|
|
2020-03-20 13:19:33 +05:30
|
|
|
|
def _polar_decomposition(T,requested):
|
2019-10-30 22:35:44 +05:30
|
|
|
|
"""
|
2020-11-16 05:31:32 +05:30
|
|
|
|
Perform singular value decomposition.
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2019-10-30 22:35:44 +05:30
|
|
|
|
Parameters
|
|
|
|
|
----------
|
2020-06-10 00:57:08 +05:30
|
|
|
|
T : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
|
|
|
|
Tensor of which the singular values are computed.
|
2019-11-22 00:16:05 +05:30
|
|
|
|
requested : iterable of str
|
2020-03-15 02:23:48 +05:30
|
|
|
|
Requested outputs: ‘R’ for the rotation tensor,
|
|
|
|
|
‘V’ for left stretch tensor and ‘U’ for right stretch tensor.
|
2019-10-30 22:35:44 +05:30
|
|
|
|
|
|
|
|
|
"""
|
2020-11-16 05:31:32 +05:30
|
|
|
|
u, _, vh = _np.linalg.svd(T)
|
2020-11-16 11:42:37 +05:30
|
|
|
|
R = _np.einsum('...ij,...jk',u,vh)
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2019-10-30 22:35:44 +05:30
|
|
|
|
output = []
|
|
|
|
|
if 'R' in requested:
|
|
|
|
|
output.append(R)
|
|
|
|
|
if 'V' in requested:
|
2020-11-16 11:42:37 +05:30
|
|
|
|
output.append(_np.einsum('...ij,...kj',T,R))
|
2019-10-30 22:35:44 +05:30
|
|
|
|
if 'U' in requested:
|
2020-11-16 11:42:37 +05:30
|
|
|
|
output.append(_np.einsum('...ji,...jk',R,T))
|
2020-02-15 18:26:15 +05:30
|
|
|
|
|
2020-11-19 15:09:41 +05:30
|
|
|
|
if len(output) == 0:
|
2020-11-20 03:06:19 +05:30
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raise ValueError('output needs to be out of V, R, U')
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2020-11-19 15:09:41 +05:30
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|
2019-10-30 22:35:44 +05:30
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return tuple(output)
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2020-02-15 18:40:16 +05:30
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|
2020-11-18 03:26:22 +05:30
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def _equivalent_Mises(T_sym,s):
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2020-02-15 18:40:16 +05:30
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"""
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2020-11-16 11:42:37 +05:30
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Base equation for Mises equivalent of a stress or strain tensor.
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2020-02-15 18:40:16 +05:30
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Parameters
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----------
|
2020-06-10 00:57:08 +05:30
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T_sym : numpy.ndarray of shape (...,3,3)
|
2020-03-15 02:23:48 +05:30
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|
|
Symmetric tensor of which the von Mises equivalent is computed.
|
2020-02-15 18:40:16 +05:30
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s : float
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2020-03-15 02:23:48 +05:30
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Scaling factor (2/3 for strain, 3/2 for stress).
|
2020-03-03 03:41:05 +05:30
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|
2020-02-15 18:40:16 +05:30
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"""
|
2020-11-19 19:08:54 +05:30
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|
|
d = _tensor.deviatoric(T_sym)
|
2020-11-16 11:42:37 +05:30
|
|
|
|
return _np.sqrt(s*_np.sum(d**2.0,axis=(-1,-2)))
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