Merge branch 'development' into MiscImprovements
F***ing commits to development!
This commit is contained in:
commit
0b6620bfb7
|
@ -252,7 +252,8 @@ class Rotation:
|
|||
acceptHomomorph = False,
|
||||
P = -1):
|
||||
|
||||
qu = quaternion if isinstance(quaternion, np.ndarray) else np.array(quaternion)
|
||||
qu = quaternion if isinstance(quaternion, np.ndarray) and quaternion.dtype == np.dtype(float) \
|
||||
else np.array(quaternion,dtype=float)
|
||||
if P > 0: qu[1:4] *= -1 # convert from P=1 to P=-1
|
||||
if qu[0] < 0.0:
|
||||
if acceptHomomorph:
|
||||
|
@ -269,7 +270,8 @@ class Rotation:
|
|||
eulers,
|
||||
degrees = False):
|
||||
|
||||
eu = eulers if isinstance(eulers, np.ndarray) else np.array(eulers)
|
||||
eu = eulers if isinstance(eulers, np.ndarray) and eulers.dtype == np.dtype(float) \
|
||||
else np.array(eulers,dtype=float)
|
||||
eu = np.radians(eu) if degrees else eu
|
||||
if np.any(eu < 0.0) or np.any(eu > 2.0*np.pi) or eu[1] > np.pi:
|
||||
raise ValueError('Euler angles outside of [0..2π],[0..π],[0..2π].\n{} {} {}.'.format(*eu))
|
||||
|
@ -283,15 +285,16 @@ class Rotation:
|
|||
normalise = False,
|
||||
P = -1):
|
||||
|
||||
ax = angleAxis if isinstance(angleAxis, np.ndarray) else np.array(angleAxis)
|
||||
if P > 0: ax[0:3] *= -1 # convert from P=1 to P=-1
|
||||
if degrees: ax[3] = np.radians(ax[3])
|
||||
if normalise: ax[0:3] /=np.linalg.norm(ax[0:3])
|
||||
ax = angleAxis if isinstance(angleAxis, np.ndarray) and angleAxis.dtype == np.dtype(float) \
|
||||
else np.array(angleAxis,dtype=float)
|
||||
if P > 0: ax[0:3] *= -1 # convert from P=1 to P=-1
|
||||
if degrees: ax[ 3] = np.radians(ax[3])
|
||||
if normalise: ax[0:3] /= np.linalg.norm(ax[0:3])
|
||||
if ax[3] < 0.0 or ax[3] > np.pi:
|
||||
raise ValueError('Axis angle rotation angle outside of [0..π].\n'.format(ax[3]))
|
||||
if not np.isclose(np.linalg.norm(ax[0:3]), 1.0):
|
||||
raise ValueError('Axis angle rotation axis is not of unit length.\n{} {} {}'.format(*ax[0:3]))
|
||||
|
||||
|
||||
return cls(ax2qu(ax))
|
||||
|
||||
@classmethod
|
||||
|
@ -330,9 +333,10 @@ class Rotation:
|
|||
normalise = False,
|
||||
P = -1):
|
||||
|
||||
ro = rodrigues if isinstance(rodrigues, np.ndarray) else np.array(rodrigues)
|
||||
if P > 0: ro[0:3] *= -1 # convert from P=1 to P=-1
|
||||
if normalise: ro[0:3] /=np.linalg.norm(ro[0:3])
|
||||
ro = rodrigues if isinstance(rodrigues, np.ndarray) and rodrigues.dtype == np.dtype(float) \
|
||||
else np.array(rodrigues,dtype=float)
|
||||
if P > 0: ro[0:3] *= -1 # convert from P=1 to P=-1
|
||||
if normalise: ro[0:3] /= np.linalg.norm(ro[0:3])
|
||||
if not np.isclose(np.linalg.norm(ro[0:3]), 1.0):
|
||||
raise ValueError('Rodrigues rotation axis is not of unit length.\n{} {} {}'.format(*ro[0:3]))
|
||||
if ro[3] < 0.0:
|
||||
|
@ -345,7 +349,8 @@ class Rotation:
|
|||
homochoric,
|
||||
P = -1):
|
||||
|
||||
ho = homochoric if isinstance(homochoric, np.ndarray) else np.array(homochoric)
|
||||
ho = homochoric if isinstance(homochoric, np.ndarray) and homochoric.dtype == np.dtype(float) \
|
||||
else np.array(homochoric,dtype=float)
|
||||
if P > 0: ho *= -1 # convert from P=1 to P=-1
|
||||
|
||||
return cls(ho2qu(ho))
|
||||
|
@ -355,7 +360,8 @@ class Rotation:
|
|||
cubochoric,
|
||||
P = -1):
|
||||
|
||||
cu = cubochoric if isinstance(cubochoric, np.ndarray) else np.array(cubochoric)
|
||||
cu = cubochoric if isinstance(cubochoric, np.ndarray) and cubochoric.dtype == np.dtype(float) \
|
||||
else np.array(cubochoric,dtype=float)
|
||||
ho = cu2ho(cu)
|
||||
if P > 0: ho *= -1 # convert from P=1 to P=-1
|
||||
|
||||
|
|
|
@ -289,7 +289,7 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,instance,of)
|
|||
real(pReal), dimension(3,3), intent(out) :: &
|
||||
Li !< inleastic velocity gradient
|
||||
real(pReal), dimension(3,3,3,3), intent(out) :: &
|
||||
dLi_dMi !< derivative of Li with respect to the Mandel stress
|
||||
dLi_dMi !< derivative of Li with respect to Mandel stress
|
||||
|
||||
real(pReal), dimension(3,3), intent(in) :: &
|
||||
Mi !< Mandel stress
|
||||
|
@ -298,7 +298,7 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,instance,of)
|
|||
of
|
||||
|
||||
real(pReal) :: &
|
||||
tr !< pressure
|
||||
tr !< trace of spherical part of Mandel stress (= 3 x pressure)
|
||||
integer :: &
|
||||
k, l, m, n
|
||||
|
||||
|
@ -306,7 +306,7 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,instance,of)
|
|||
|
||||
tr=math_trace33(math_spherical33(Mi))
|
||||
|
||||
if (prm%dilatation .and. abs(tr) > 0.0_pReal) then ! no stress or J2 plasticity --> Li and its derivative are zero
|
||||
if (prm%dilatation .and. abs(tr) > 0.0_pReal) then ! no stress or J2 plasticity --> Li and its derivative are zero
|
||||
Li = math_I3 &
|
||||
* prm%dot_gamma_0/prm%M * (3.0_pReal*prm%M*stt%xi(of))**(-prm%n) &
|
||||
* tr * abs(tr)**(prm%n-1.0_pReal)
|
||||
|
@ -321,7 +321,7 @@ subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,instance,of)
|
|||
#endif
|
||||
|
||||
forall (k=1:3,l=1:3,m=1:3,n=1:3) &
|
||||
dLi_dMi(k,l,m,n) = real(n,pReal) / tr * Li(k,l) * math_I3(m,n)
|
||||
dLi_dMi(k,l,m,n) = prm%n / tr * Li(k,l) * math_I3(m,n)
|
||||
|
||||
else
|
||||
Li = 0.0_pReal
|
||||
|
|
Loading…
Reference in New Issue