following python convention
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@ -59,7 +59,7 @@ def cube_to_ball(cube):
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ball = np.zeros(3)
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else:
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# get pyramide and scale by grid parameter ratio
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p = get_order(cube)
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p = _get_order(cube)
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XYZ = cube[p] * sc
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# intercept all the points along the z-axis
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@ -109,7 +109,7 @@ def ball_to_cube(ball):
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if np.allclose(ball,0.0,rtol=0.0,atol=1.0e-300):
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cube = np.zeros(3)
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else:
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p = get_order(ball)
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p = _get_order(ball)
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xyz3 = ball[p]
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# inverse M_3
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@ -137,7 +137,7 @@ def ball_to_cube(ball):
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return cube
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def get_order(xyz):
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def _get_order(xyz):
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"""
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Get order of the coordinates.
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@ -85,7 +85,7 @@ def left_stretch(T):
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Tensor of which the left stretch is computed.
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"""
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return __polar_decomposition(T,'V')[0]
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return _polar_decomposition(T,'V')[0]
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def maximum_shear(T_sym):
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@ -113,7 +113,7 @@ def Mises_strain(epsilon):
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Symmetric strain tensor of which the von Mises equivalent is computed.
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"""
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return __Mises(epsilon,2.0/3.0)
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return _Mises(epsilon,2.0/3.0)
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def Mises_stress(sigma):
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@ -126,7 +126,7 @@ def Mises_stress(sigma):
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Symmetric stress tensor of which the von Mises equivalent is computed.
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"""
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return __Mises(sigma,3.0/2.0)
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return _Mises(sigma,3.0/2.0)
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def PK2(P,F):
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@ -158,7 +158,7 @@ def right_stretch(T):
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Tensor of which the right stretch is computed.
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"""
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return __polar_decomposition(T,'U')[0]
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return _polar_decomposition(T,'U')[0]
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def rotational_part(T):
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@ -171,7 +171,7 @@ def rotational_part(T):
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Tensor of which the rotational part is computed.
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"""
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return __polar_decomposition(T,'R')[0]
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return _polar_decomposition(T,'R')[0]
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def spherical_part(T,tensor=False):
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@ -262,7 +262,7 @@ def transpose(T):
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np.transpose(T,(0,2,1))
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def __polar_decomposition(T,requested):
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def _polar_decomposition(T,requested):
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"""
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Singular value decomposition.
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@ -290,7 +290,7 @@ def __polar_decomposition(T,requested):
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return tuple(output)
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def __Mises(T_sym,s):
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def _Mises(T_sym,s):
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"""
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Base equation for Mises equivalent of a stres or strain tensor.
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