Merge branch 'development' into vectorize_rotation

This commit is contained in:
Martin Diehl 2020-04-21 19:29:30 +02:00
commit 7efe14be35
16 changed files with 492 additions and 446 deletions

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@ -1 +1 @@
v2.0.3-2243-gbb03483b
v2.0.3-2303-g2a6132b7

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@ -6,7 +6,7 @@ name = 'damask'
with open(_os.path.join(_os.path.dirname(__file__),'VERSION')) as _f:
version = _re.sub(r'^v','',_f.readline().strip())
# classes
# make classes directly accessible as damask.Class
from ._environment import Environment # noqa
from ._table import Table # noqa
from ._vtk import VTK # noqa

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@ -291,7 +291,7 @@ class Geom:
comments = []
for i,line in enumerate(content[:header_length]):
items = line.lower().strip().split()
items = line.split('#')[0].lower().strip().split()
key = items[0] if items else ''
if key == 'grid':
grid = np.array([ int(dict(zip(items[1::2],items[2::2]))[i]) for i in ['a','b','c']])
@ -307,7 +307,7 @@ class Geom:
microstructure = np.empty(grid.prod()) # initialize as flat array
i = 0
for line in content[header_length:]:
items = line.split()
items = line.split('#')[0].split()
if len(items) == 3:
if items[1].lower() == 'of':
items = np.ones(int(items[0]))*float(items[2])

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@ -68,12 +68,12 @@ class Result:
self.con_physics = []
for c in self.constituents:
self.con_physics += f['/'.join([self.increments[0],'constituent',c])].keys()
self.con_physics = list(set(self.con_physics)) # make unique
self.con_physics = list(set(self.con_physics)) # make unique
self.mat_physics = []
for m in self.materialpoints:
self.mat_physics += f['/'.join([self.increments[0],'materialpoint',m])].keys()
self.mat_physics = list(set(self.mat_physics)) # make unique
self.mat_physics = list(set(self.mat_physics)) # make unique
self.selection = {'increments': self.increments,
'constituents': self.constituents,'materialpoints': self.materialpoints,
@ -86,13 +86,19 @@ class Result:
def __repr__(self):
"""Show selected data."""
all_selected_increments = self.selection['increments']
self.pick('increments',all_selected_increments[0:1])
first = self.list_data()
self.pick('increments',all_selected_increments[-1:])
last = self.list_data()
last = '' if len(all_selected_increments) < 2 else self.list_data()
self.pick('increments',all_selected_increments)
in_between = ''.join(['\n{}\n ...\n'.format(inc) for inc in all_selected_increments[1:-2]])
return util.srepr(first+ in_between + last)
in_between = '' if len(all_selected_increments) < 3 else \
''.join(['\n{}\n ...\n'.format(inc) for inc in all_selected_increments[1:-2]])
return util.srepr(first + in_between + last)
def _manage_selection(self,action,what,datasets):
@ -1009,7 +1015,7 @@ class Result:
continue
lock.acquire()
with h5py.File(self.fname, 'a') as f:
try:
try: # ToDo: Replace if exists?
dataset = f[result[0]].create_dataset(result[1]['label'],data=result[1]['data'])
for l,v in result[1]['meta'].items():
dataset.attrs[l]=v.encode()

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@ -1,5 +1,5 @@
from scipy import spatial
import numpy as np
from scipy import spatial as _spatial
import numpy as _np
def _ks(size,grid,first_order=False):
"""
@ -11,16 +11,16 @@ def _ks(size,grid,first_order=False):
physical size of the periodic field.
"""
k_sk = np.where(np.arange(grid[0])>grid[0]//2,np.arange(grid[0])-grid[0],np.arange(grid[0]))/size[0]
k_sk = _np.where(_np.arange(grid[0])>grid[0]//2,_np.arange(grid[0])-grid[0],_np.arange(grid[0]))/size[0]
if grid[0]%2 == 0 and first_order: k_sk[grid[0]//2] = 0 # Nyquist freq=0 for even grid (Johnson, MIT, 2011)
k_sj = np.where(np.arange(grid[1])>grid[1]//2,np.arange(grid[1])-grid[1],np.arange(grid[1]))/size[1]
k_sj = _np.where(_np.arange(grid[1])>grid[1]//2,_np.arange(grid[1])-grid[1],_np.arange(grid[1]))/size[1]
if grid[1]%2 == 0 and first_order: k_sj[grid[1]//2] = 0 # Nyquist freq=0 for even grid (Johnson, MIT, 2011)
k_si = np.arange(grid[2]//2+1)/size[2]
k_si = _np.arange(grid[2]//2+1)/size[2]
kk, kj, ki = np.meshgrid(k_sk,k_sj,k_si,indexing = 'ij')
return np.concatenate((ki[:,:,:,None],kj[:,:,:,None],kk[:,:,:,None]),axis = 3)
kk, kj, ki = _np.meshgrid(k_sk,k_sj,k_si,indexing = 'ij')
return _np.concatenate((ki[:,:,:,None],kj[:,:,:,None],kk[:,:,:,None]),axis = 3)
def curl(size,field):
@ -33,18 +33,18 @@ def curl(size,field):
physical size of the periodic field.
"""
n = np.prod(field.shape[3:])
n = _np.prod(field.shape[3:])
k_s = _ks(size,field.shape[:3],True)
e = np.zeros((3, 3, 3))
e = _np.zeros((3, 3, 3))
e[0, 1, 2] = e[1, 2, 0] = e[2, 0, 1] = +1.0 # Levi-Civita symbol
e[0, 2, 1] = e[2, 1, 0] = e[1, 0, 2] = -1.0
field_fourier = np.fft.rfftn(field,axes=(0,1,2))
curl_ = (np.einsum('slm,ijkl,ijkm ->ijks', e,k_s,field_fourier)*2.0j*np.pi if n == 3 else # vector, 3 -> 3
np.einsum('slm,ijkl,ijknm->ijksn',e,k_s,field_fourier)*2.0j*np.pi) # tensor, 3x3 -> 3x3
field_fourier = _np.fft.rfftn(field,axes=(0,1,2))
curl_ = (_np.einsum('slm,ijkl,ijkm ->ijks', e,k_s,field_fourier)*2.0j*_np.pi if n == 3 else # vector, 3 -> 3
_np.einsum('slm,ijkl,ijknm->ijksn',e,k_s,field_fourier)*2.0j*_np.pi) # tensor, 3x3 -> 3x3
return np.fft.irfftn(curl_,axes=(0,1,2),s=field.shape[:3])
return _np.fft.irfftn(curl_,axes=(0,1,2),s=field.shape[:3])
def divergence(size,field):
@ -57,14 +57,14 @@ def divergence(size,field):
physical size of the periodic field.
"""
n = np.prod(field.shape[3:])
n = _np.prod(field.shape[3:])
k_s = _ks(size,field.shape[:3],True)
field_fourier = np.fft.rfftn(field,axes=(0,1,2))
div_ = (np.einsum('ijkl,ijkl ->ijk', k_s,field_fourier)*2.0j*np.pi if n == 3 else # vector, 3 -> 1
np.einsum('ijkm,ijklm->ijkl',k_s,field_fourier)*2.0j*np.pi) # tensor, 3x3 -> 3
field_fourier = _np.fft.rfftn(field,axes=(0,1,2))
div_ = (_np.einsum('ijkl,ijkl ->ijk', k_s,field_fourier)*2.0j*_np.pi if n == 3 else # vector, 3 -> 1
_np.einsum('ijkm,ijklm->ijkl',k_s,field_fourier)*2.0j*_np.pi) # tensor, 3x3 -> 3
return np.fft.irfftn(div_,axes=(0,1,2),s=field.shape[:3])
return _np.fft.irfftn(div_,axes=(0,1,2),s=field.shape[:3])
def gradient(size,field):
@ -77,17 +77,17 @@ def gradient(size,field):
physical size of the periodic field.
"""
n = np.prod(field.shape[3:])
n = _np.prod(field.shape[3:])
k_s = _ks(size,field.shape[:3],True)
field_fourier = np.fft.rfftn(field,axes=(0,1,2))
grad_ = (np.einsum('ijkl,ijkm->ijkm', field_fourier,k_s)*2.0j*np.pi if n == 1 else # scalar, 1 -> 3
np.einsum('ijkl,ijkm->ijklm',field_fourier,k_s)*2.0j*np.pi) # vector, 3 -> 3x3
field_fourier = _np.fft.rfftn(field,axes=(0,1,2))
grad_ = (_np.einsum('ijkl,ijkm->ijkm', field_fourier,k_s)*2.0j*_np.pi if n == 1 else # scalar, 1 -> 3
_np.einsum('ijkl,ijkm->ijklm',field_fourier,k_s)*2.0j*_np.pi) # vector, 3 -> 3x3
return np.fft.irfftn(grad_,axes=(0,1,2),s=field.shape[:3])
return _np.fft.irfftn(grad_,axes=(0,1,2),s=field.shape[:3])
def cell_coord0(grid,size,origin=np.zeros(3)):
def cell_coord0(grid,size,origin=_np.zeros(3)):
"""
Cell center positions (undeformed).
@ -103,7 +103,7 @@ def cell_coord0(grid,size,origin=np.zeros(3)):
"""
start = origin + size/grid*.5
end = origin + size - size/grid*.5
return np.mgrid[start[0]:end[0]:grid[0]*1j,start[1]:end[1]:grid[1]*1j,start[2]:end[2]:grid[2]*1j].T
return _np.mgrid[start[0]:end[0]:grid[0]*1j,start[1]:end[1]:grid[1]*1j,start[2]:end[2]:grid[2]*1j].T
def cell_displacement_fluct(size,F):
@ -118,19 +118,19 @@ def cell_displacement_fluct(size,F):
deformation gradient field.
"""
integrator = 0.5j*size/np.pi
integrator = 0.5j*size/_np.pi
k_s = _ks(size,F.shape[:3],False)
k_s_squared = np.einsum('...l,...l',k_s,k_s)
k_s_squared = _np.einsum('...l,...l',k_s,k_s)
k_s_squared[0,0,0] = 1.0
displacement = -np.einsum('ijkml,ijkl,l->ijkm',
np.fft.rfftn(F,axes=(0,1,2)),
displacement = -_np.einsum('ijkml,ijkl,l->ijkm',
_np.fft.rfftn(F,axes=(0,1,2)),
k_s,
integrator,
) / k_s_squared[...,np.newaxis]
) / k_s_squared[...,_np.newaxis]
return np.fft.irfftn(displacement,axes=(0,1,2),s=F.shape[:3])
return _np.fft.irfftn(displacement,axes=(0,1,2),s=F.shape[:3])
def cell_displacement_avg(size,F):
@ -145,8 +145,8 @@ def cell_displacement_avg(size,F):
deformation gradient field.
"""
F_avg = np.average(F,axis=(0,1,2))
return np.einsum('ml,ijkl->ijkm',F_avg-np.eye(3),cell_coord0(F.shape[:3][::-1],size))
F_avg = _np.average(F,axis=(0,1,2))
return _np.einsum('ml,ijkl->ijkm',F_avg - _np.eye(3),cell_coord0(F.shape[:3][::-1],size))
def cell_displacement(size,F):
@ -164,7 +164,7 @@ def cell_displacement(size,F):
return cell_displacement_avg(size,F) + cell_displacement_fluct(size,F)
def cell_coord(size,F,origin=np.zeros(3)):
def cell_coord(size,F,origin=_np.zeros(3)):
"""
Cell center positions.
@ -193,17 +193,17 @@ def cell_coord0_gridSizeOrigin(coord0,ordered=True):
expect coord0 data to be ordered (x fast, z slow).
"""
coords = [np.unique(coord0[:,i]) for i in range(3)]
mincorner = np.array(list(map(min,coords)))
maxcorner = np.array(list(map(max,coords)))
grid = np.array(list(map(len,coords)),'i')
size = grid/np.maximum(grid-1,1) * (maxcorner-mincorner)
coords = [_np.unique(coord0[:,i]) for i in range(3)]
mincorner = _np.array(list(map(min,coords)))
maxcorner = _np.array(list(map(max,coords)))
grid = _np.array(list(map(len,coords)),'i')
size = grid/_np.maximum(grid-1,1) * (maxcorner-mincorner)
delta = size/grid
origin = mincorner - delta*.5
# 1D/2D: size/origin combination undefined, set origin to 0.0
size [np.where(grid==1)] = origin[np.where(grid==1)]*2.
origin[np.where(grid==1)] = 0.0
size [_np.where(grid==1)] = origin[_np.where(grid==1)]*2.
origin[_np.where(grid==1)] = 0.0
if grid.prod() != len(coord0):
raise ValueError('Data count {} does not match grid {}.'.format(len(coord0),grid))
@ -211,12 +211,12 @@ def cell_coord0_gridSizeOrigin(coord0,ordered=True):
start = origin + delta*.5
end = origin - delta*.5 + size
if not np.allclose(coords[0],np.linspace(start[0],end[0],grid[0])) and \
np.allclose(coords[1],np.linspace(start[1],end[1],grid[1])) and \
np.allclose(coords[2],np.linspace(start[2],end[2],grid[2])):
if not _np.allclose(coords[0],_np.linspace(start[0],end[0],grid[0])) and \
_np.allclose(coords[1],_np.linspace(start[1],end[1],grid[1])) and \
_np.allclose(coords[2],_np.linspace(start[2],end[2],grid[2])):
raise ValueError('Regular grid spacing violated.')
if ordered and not np.allclose(coord0.reshape(tuple(grid[::-1])+(3,)),cell_coord0(grid,size,origin)):
if ordered and not _np.allclose(coord0.reshape(tuple(grid[::-1])+(3,)),cell_coord0(grid,size,origin)):
raise ValueError('Input data is not a regular grid.')
return (grid,size,origin)
@ -235,7 +235,7 @@ def coord0_check(coord0):
cell_coord0_gridSizeOrigin(coord0,ordered=True)
def node_coord0(grid,size,origin=np.zeros(3)):
def node_coord0(grid,size,origin=_np.zeros(3)):
"""
Nodal positions (undeformed).
@ -249,9 +249,9 @@ def node_coord0(grid,size,origin=np.zeros(3)):
physical origin of the periodic field. Defaults to [0.0,0.0,0.0].
"""
return np.mgrid[origin[0]:size[0]+origin[0]:(grid[0]+1)*1j,
origin[1]:size[1]+origin[1]:(grid[1]+1)*1j,
origin[2]:size[2]+origin[2]:(grid[2]+1)*1j].T
return _np.mgrid[origin[0]:size[0]+origin[0]:(grid[0]+1)*1j,
origin[1]:size[1]+origin[1]:(grid[1]+1)*1j,
origin[2]:size[2]+origin[2]:(grid[2]+1)*1j].T
def node_displacement_fluct(size,F):
@ -281,8 +281,8 @@ def node_displacement_avg(size,F):
deformation gradient field.
"""
F_avg = np.average(F,axis=(0,1,2))
return np.einsum('ml,ijkl->ijkm',F_avg-np.eye(3),node_coord0(F.shape[:3][::-1],size))
F_avg = _np.average(F,axis=(0,1,2))
return _np.einsum('ml,ijkl->ijkm',F_avg - _np.eye(3),node_coord0(F.shape[:3][::-1],size))
def node_displacement(size,F):
@ -300,7 +300,7 @@ def node_displacement(size,F):
return node_displacement_avg(size,F) + node_displacement_fluct(size,F)
def node_coord(size,F,origin=np.zeros(3)):
def node_coord(size,F,origin=_np.zeros(3)):
"""
Nodal positions.
@ -319,18 +319,18 @@ def node_coord(size,F,origin=np.zeros(3)):
def cell_2_node(cell_data):
"""Interpolate periodic cell data to nodal data."""
n = ( cell_data + np.roll(cell_data,1,(0,1,2))
+ np.roll(cell_data,1,(0,)) + np.roll(cell_data,1,(1,)) + np.roll(cell_data,1,(2,))
+ np.roll(cell_data,1,(0,1)) + np.roll(cell_data,1,(1,2)) + np.roll(cell_data,1,(2,0)))*0.125
n = ( cell_data + _np.roll(cell_data,1,(0,1,2))
+ _np.roll(cell_data,1,(0,)) + _np.roll(cell_data,1,(1,)) + _np.roll(cell_data,1,(2,))
+ _np.roll(cell_data,1,(0,1)) + _np.roll(cell_data,1,(1,2)) + _np.roll(cell_data,1,(2,0)))*0.125
return np.pad(n,((0,1),(0,1),(0,1))+((0,0),)*len(cell_data.shape[3:]),mode='wrap')
return _np.pad(n,((0,1),(0,1),(0,1))+((0,0),)*len(cell_data.shape[3:]),mode='wrap')
def node_2_cell(node_data):
"""Interpolate periodic nodal data to cell data."""
c = ( node_data + np.roll(node_data,1,(0,1,2))
+ np.roll(node_data,1,(0,)) + np.roll(node_data,1,(1,)) + np.roll(node_data,1,(2,))
+ np.roll(node_data,1,(0,1)) + np.roll(node_data,1,(1,2)) + np.roll(node_data,1,(2,0)))*0.125
c = ( node_data + _np.roll(node_data,1,(0,1,2))
+ _np.roll(node_data,1,(0,)) + _np.roll(node_data,1,(1,)) + _np.roll(node_data,1,(2,))
+ _np.roll(node_data,1,(0,1)) + _np.roll(node_data,1,(1,2)) + _np.roll(node_data,1,(2,0)))*0.125
return c[:-1,:-1,:-1]
@ -347,22 +347,22 @@ def node_coord0_gridSizeOrigin(coord0,ordered=False):
expect coord0 data to be ordered (x fast, z slow).
"""
coords = [np.unique(coord0[:,i]) for i in range(3)]
mincorner = np.array(list(map(min,coords)))
maxcorner = np.array(list(map(max,coords)))
grid = np.array(list(map(len,coords)),'i') - 1
coords = [_np.unique(coord0[:,i]) for i in range(3)]
mincorner = _np.array(list(map(min,coords)))
maxcorner = _np.array(list(map(max,coords)))
grid = _np.array(list(map(len,coords)),'i') - 1
size = maxcorner-mincorner
origin = mincorner
if (grid+1).prod() != len(coord0):
raise ValueError('Data count {} does not match grid {}.'.format(len(coord0),grid))
if not np.allclose(coords[0],np.linspace(mincorner[0],maxcorner[0],grid[0]+1)) and \
np.allclose(coords[1],np.linspace(mincorner[1],maxcorner[1],grid[1]+1)) and \
np.allclose(coords[2],np.linspace(mincorner[2],maxcorner[2],grid[2]+1)):
if not _np.allclose(coords[0],_np.linspace(mincorner[0],maxcorner[0],grid[0]+1)) and \
_np.allclose(coords[1],_np.linspace(mincorner[1],maxcorner[1],grid[1]+1)) and \
_np.allclose(coords[2],_np.linspace(mincorner[2],maxcorner[2],grid[2]+1)):
raise ValueError('Regular grid spacing violated.')
if ordered and not np.allclose(coord0.reshape(tuple((grid+1)[::-1])+(3,)),node_coord0(grid,size,origin)):
if ordered and not _np.allclose(coord0.reshape(tuple((grid+1)[::-1])+(3,)),node_coord0(grid,size,origin)):
raise ValueError('Input data is not a regular grid.')
return (grid,size,origin)
@ -386,10 +386,10 @@ def regrid(size,F,new_grid):
+ cell_displacement_avg(size,F) \
+ cell_displacement_fluct(size,F)
outer = np.dot(np.average(F,axis=(0,1,2)),size)
outer = _np.dot(_np.average(F,axis=(0,1,2)),size)
for d in range(3):
c[np.where(c[:,:,:,d]<0)] += outer[d]
c[np.where(c[:,:,:,d]>outer[d])] -= outer[d]
c[_np.where(c[:,:,:,d]<0)] += outer[d]
c[_np.where(c[:,:,:,d]>outer[d])] -= outer[d]
tree = spatial.cKDTree(c.reshape(-1,3),boxsize=outer)
tree = _spatial.cKDTree(c.reshape(-1,3),boxsize=outer)
return tree.query(cell_coord0(new_grid,outer))[1].flatten()

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@ -1,4 +1,4 @@
import numpy as np
import numpy as _np
def Cauchy(P,F):
"""
@ -14,10 +14,10 @@ def Cauchy(P,F):
First Piola-Kirchhoff stress.
"""
if np.shape(F) == np.shape(P) == (3,3):
sigma = 1.0/np.linalg.det(F) * np.dot(P,F.T)
if _np.shape(F) == _np.shape(P) == (3,3):
sigma = 1.0/_np.linalg.det(F) * _np.dot(P,F.T)
else:
sigma = np.einsum('i,ijk,ilk->ijl',1.0/np.linalg.det(F),P,F)
sigma = _np.einsum('i,ijk,ilk->ijl',1.0/_np.linalg.det(F),P,F)
return symmetric(sigma)
@ -31,8 +31,8 @@ def deviatoric_part(T):
Tensor of which the deviatoric part is computed.
"""
return T - np.eye(3)*spherical_part(T) if np.shape(T) == (3,3) else \
T - np.einsum('ijk,i->ijk',np.broadcast_to(np.eye(3),[T.shape[0],3,3]),spherical_part(T))
return T - _np.eye(3)*spherical_part(T) if _np.shape(T) == (3,3) else \
T - _np.einsum('ijk,i->ijk',_np.broadcast_to(_np.eye(3),[T.shape[0],3,3]),spherical_part(T))
def eigenvalues(T_sym):
@ -48,7 +48,7 @@ def eigenvalues(T_sym):
Symmetric tensor of which the eigenvalues are computed.
"""
return np.linalg.eigvalsh(symmetric(T_sym))
return _np.linalg.eigvalsh(symmetric(T_sym))
def eigenvectors(T_sym,RHS=False):
@ -65,13 +65,13 @@ def eigenvectors(T_sym,RHS=False):
Enforce right-handed coordinate system. Default is False.
"""
(u,v) = np.linalg.eigh(symmetric(T_sym))
(u,v) = _np.linalg.eigh(symmetric(T_sym))
if RHS:
if np.shape(T_sym) == (3,3):
if np.linalg.det(v) < 0.0: v[:,2] *= -1.0
if _np.shape(T_sym) == (3,3):
if _np.linalg.det(v) < 0.0: v[:,2] *= -1.0
else:
v[np.linalg.det(v) < 0.0,:,2] *= -1.0
v[_np.linalg.det(v) < 0.0,:,2] *= -1.0
return v
@ -99,7 +99,7 @@ def maximum_shear(T_sym):
"""
w = eigenvalues(T_sym)
return (w[0] - w[2])*0.5 if np.shape(T_sym) == (3,3) else \
return (w[0] - w[2])*0.5 if _np.shape(T_sym) == (3,3) else \
(w[:,0] - w[:,2])*0.5
@ -141,10 +141,10 @@ def PK2(P,F):
Deformation gradient.
"""
if np.shape(F) == np.shape(P) == (3,3):
S = np.dot(np.linalg.inv(F),P)
if _np.shape(F) == _np.shape(P) == (3,3):
S = _np.dot(_np.linalg.inv(F),P)
else:
S = np.einsum('...jk,...kl->...jl',np.linalg.inv(F),P)
S = _np.einsum('...jk,...kl->...jl',_np.linalg.inv(F),P)
return symmetric(S)
@ -187,14 +187,14 @@ def spherical_part(T,tensor=False):
"""
if T.shape == (3,3):
sph = np.trace(T)/3.0
return sph if not tensor else np.eye(3)*sph
sph = _np.trace(T)/3.0
return sph if not tensor else _np.eye(3)*sph
else:
sph = np.trace(T,axis1=1,axis2=2)/3.0
sph = _np.trace(T,axis1=1,axis2=2)/3.0
if not tensor:
return sph
else:
return np.einsum('ijk,i->ijk',np.broadcast_to(np.eye(3),(T.shape[0],3,3)),sph)
return _np.einsum('ijk,i->ijk',_np.broadcast_to(_np.eye(3),(T.shape[0],3,3)),sph)
def strain_tensor(F,t,m):
@ -216,22 +216,22 @@ def strain_tensor(F,t,m):
"""
F_ = F.reshape(1,3,3) if F.shape == (3,3) else F
if t == 'V':
B = np.matmul(F_,transpose(F_))
w,n = np.linalg.eigh(B)
B = _np.matmul(F_,transpose(F_))
w,n = _np.linalg.eigh(B)
elif t == 'U':
C = np.matmul(transpose(F_),F_)
w,n = np.linalg.eigh(C)
C = _np.matmul(transpose(F_),F_)
w,n = _np.linalg.eigh(C)
if m > 0.0:
eps = 1.0/(2.0*abs(m)) * (+ np.matmul(n,np.einsum('ij,ikj->ijk',w**m,n))
- np.broadcast_to(np.eye(3),[F_.shape[0],3,3]))
eps = 1.0/(2.0*abs(m)) * (+ _np.matmul(n,_np.einsum('ij,ikj->ijk',w**m,n))
- _np.broadcast_to(_np.eye(3),[F_.shape[0],3,3]))
elif m < 0.0:
eps = 1.0/(2.0*abs(m)) * (- np.matmul(n,np.einsum('ij,ikj->ijk',w**m,n))
+ np.broadcast_to(np.eye(3),[F_.shape[0],3,3]))
eps = 1.0/(2.0*abs(m)) * (- _np.matmul(n,_np.einsum('ij,ikj->ijk',w**m,n))
+ _np.broadcast_to(_np.eye(3),[F_.shape[0],3,3]))
else:
eps = np.matmul(n,np.einsum('ij,ikj->ijk',0.5*np.log(w),n))
eps = _np.matmul(n,_np.einsum('ij,ikj->ijk',0.5*_np.log(w),n))
return eps.reshape(3,3) if np.shape(F) == (3,3) else \
return eps.reshape(3,3) if _np.shape(F) == (3,3) else \
eps
@ -258,8 +258,8 @@ def transpose(T):
Tensor of which the transpose is computed.
"""
return T.T if np.shape(T) == (3,3) else \
np.swapaxes(T,axis2=-2,axis1=-1)
return T.T if _np.shape(T) == (3,3) else \
_np.swapaxes(T,axis2=-2,axis1=-1)
def _polar_decomposition(T,requested):
@ -275,17 +275,17 @@ def _polar_decomposition(T,requested):
V for left stretch tensor and U for right stretch tensor.
"""
u, s, vh = np.linalg.svd(T)
R = np.dot(u,vh) if np.shape(T) == (3,3) else \
np.einsum('ijk,ikl->ijl',u,vh)
u, s, vh = _np.linalg.svd(T)
R = _np.dot(u,vh) if _np.shape(T) == (3,3) else \
_np.einsum('ijk,ikl->ijl',u,vh)
output = []
if 'R' in requested:
output.append(R)
if 'V' in requested:
output.append(np.dot(T,R.T) if np.shape(T) == (3,3) else np.einsum('ijk,ilk->ijl',T,R))
output.append(_np.dot(T,R.T) if _np.shape(T) == (3,3) else _np.einsum('ijk,ilk->ijl',T,R))
if 'U' in requested:
output.append(np.dot(R.T,T) if np.shape(T) == (3,3) else np.einsum('ikj,ikl->ijl',R,T))
output.append(_np.dot(R.T,T) if _np.shape(T) == (3,3) else _np.einsum('ikj,ikl->ijl',R,T))
return tuple(output)
@ -303,5 +303,5 @@ def _Mises(T_sym,s):
"""
d = deviatoric_part(T_sym)
return np.sqrt(s*(np.sum(d**2.0))) if np.shape(T_sym) == (3,3) else \
np.sqrt(s*np.einsum('ijk->i',d**2.0))
return _np.sqrt(s*(_np.sum(d**2.0))) if _np.shape(T_sym) == (3,3) else \
_np.sqrt(s*_np.einsum('ijk->i',d**2.0))

View File

@ -9,37 +9,22 @@ from optparse import Option
import numpy as np
class bcolors:
"""
ASCII Colors.
https://svn.blender.org/svnroot/bf-blender/trunk/blender/build_files/scons/tools/bcolors.py
https://stackoverflow.com/questions/287871
"""
HEADER = '\033[95m'
OKBLUE = '\033[94m'
OKGREEN = '\033[92m'
WARNING = '\033[93m'
FAIL = '\033[91m'
ENDC = '\033[0m'
BOLD = '\033[1m'
DIM = '\033[2m'
UNDERLINE = '\033[4m'
CROSSOUT = '\033[9m'
def disable(self):
self.HEADER = ''
self.OKBLUE = ''
self.OKGREEN = ''
self.WARNING = ''
self.FAIL = ''
self.ENDC = ''
self.BOLD = ''
self.UNDERLINE = ''
self.CROSSOUT = ''
# limit visibility
__all__=[
'srepr',
'croak',
'report',
'emph','deemph','delete','strikeout',
'execute',
'show_progress',
'scale_to_coprime',
'return_message',
'extendableOption',
]
####################################################################################################
# Functions
####################################################################################################
def srepr(arg,glue = '\n'):
r"""
Join arguments as individual lines.
@ -144,6 +129,52 @@ def execute(cmd,
return out,error
def show_progress(iterable,N_iter=None,prefix='',bar_length=50):
"""
Decorate a loop with a status bar.
Use similar like enumerate.
Parameters
----------
iterable : iterable/function with yield statement
Iterable (or function with yield statement) to be decorated.
N_iter : int
Total # of iterations. Needed if number of iterations can not be obtained as len(iterable).
prefix : str, optional.
Prefix string.
bar_length : int, optional
Character length of bar. Defaults to 50.
"""
status = _ProgressBar(N_iter if N_iter else len(iterable),prefix,bar_length)
for i,item in enumerate(iterable):
yield item
status.update(i)
def scale_to_coprime(v):
"""Scale vector to co-prime (relatively prime) integers."""
MAX_DENOMINATOR = 1000
def get_square_denominator(x):
"""Denominator of the square of a number."""
return fractions.Fraction(x ** 2).limit_denominator(MAX_DENOMINATOR).denominator
def lcm(a, b):
"""Least common multiple."""
return a * b // np.gcd(a, b)
denominators = [int(get_square_denominator(i)) for i in v]
s = reduce(lcm, denominators) ** 0.5
m = (np.array(v)*s).astype(np.int)
return m//reduce(np.gcd,m)
####################################################################################################
# Classes
####################################################################################################
class extendableOption(Option):
"""
Used for definition of new option parser action 'extend', which enables to take multiple option arguments.
@ -215,47 +246,36 @@ class _ProgressBar:
sys.stderr.write('\n')
sys.stderr.flush()
def show_progress(iterable,N_iter=None,prefix='',bar_length=50):
class bcolors:
"""
Decorate a loop with a status bar.
Use similar like enumerate.
Parameters
----------
iterable : iterable/function with yield statement
Iterable (or function with yield statement) to be decorated.
N_iter : int
Total # of iterations. Needed if number of iterations can not be obtained as len(iterable).
prefix : str, optional.
Prefix string.
bar_length : int, optional
Character length of bar. Defaults to 50.
ASCII Colors.
https://svn.blender.org/svnroot/bf-blender/trunk/blender/build_files/scons/tools/bcolors.py
https://stackoverflow.com/questions/287871
"""
status = _ProgressBar(N_iter if N_iter else len(iterable),prefix,bar_length)
for i,item in enumerate(iterable):
yield item
status.update(i)
HEADER = '\033[95m'
OKBLUE = '\033[94m'
OKGREEN = '\033[92m'
WARNING = '\033[93m'
FAIL = '\033[91m'
ENDC = '\033[0m'
BOLD = '\033[1m'
DIM = '\033[2m'
UNDERLINE = '\033[4m'
CROSSOUT = '\033[9m'
def scale_to_coprime(v):
"""Scale vector to co-prime (relatively prime) integers."""
MAX_DENOMINATOR = 1000
def get_square_denominator(x):
"""Denominator of the square of a number."""
return fractions.Fraction(x ** 2).limit_denominator(MAX_DENOMINATOR).denominator
def lcm(a, b):
"""Least common multiple."""
return a * b // np.gcd(a, b)
denominators = [int(get_square_denominator(i)) for i in v]
s = reduce(lcm, denominators) ** 0.5
m = (np.array(v)*s).astype(np.int)
return m//reduce(np.gcd,m)
def disable(self):
self.HEADER = ''
self.OKBLUE = ''
self.OKGREEN = ''
self.WARNING = ''
self.FAIL = ''
self.ENDC = ''
self.BOLD = ''
self.UNDERLINE = ''
self.CROSSOUT = ''
class return_message:
@ -276,4 +296,3 @@ class return_message:
def __repr__(self):
"""Return message suitable for interactive shells."""
return srepr(self.message)

View File

@ -24,6 +24,10 @@ def reference_dir(reference_dir_base):
class TestResult:
def test_self_report(self,default):
print(default)
def test_time_increments(self,default):
shape = default.read_dataset(default.get_dataset_location('F'),0).shape
default.set_by_time(0.0,20.0)

View File

@ -24,7 +24,7 @@ class TestGridFilters:
n = grid_filters.node_coord0(grid,size) + size/grid*.5
assert np.allclose(c,n)
@pytest.mark.parametrize('mode',[('cell'),('node')])
@pytest.mark.parametrize('mode',['cell','node'])
def test_grid_DNA(self,mode):
"""Ensure that xx_coord0_gridSizeOrigin is the inverse of xx_coord0."""
grid = np.random.randint(8,32,(3))
@ -49,7 +49,7 @@ class TestGridFilters:
assert np.allclose(grid_filters.node_coord(size,F) [1:-1,1:-1,1:-1],grid_filters.cell_2_node(
grid_filters.cell_coord(size,F))[1:-1,1:-1,1:-1])
@pytest.mark.parametrize('mode',[('cell'),('node')])
@pytest.mark.parametrize('mode',['cell','node'])
def test_coord0_origin(self,mode):
origin= np.random.random(3)
size = np.random.random(3) # noqa
@ -61,22 +61,24 @@ class TestGridFilters:
elif mode == 'node':
assert np.allclose(shifted,unshifted+np.broadcast_to(origin,tuple(grid[::-1]+1)+(3,)))
@pytest.mark.parametrize('mode',[('cell'),('node')])
def test_displacement_avg_vanishes(self,mode):
@pytest.mark.parametrize('function',[grid_filters.cell_displacement_avg,
grid_filters.node_displacement_avg])
def test_displacement_avg_vanishes(self,function):
"""Ensure that random fluctuations in F do not result in average displacement."""
size = np.random.random(3) # noqa
size = np.random.random(3)
grid = np.random.randint(8,32,(3))
F = np.random.random(tuple(grid)+(3,3))
F += np.eye(3) - np.average(F,axis=(0,1,2))
assert np.allclose(eval('grid_filters.{}_displacement_avg(size,F)'.format(mode)),0.0)
assert np.allclose(function(size,F),0.0)
@pytest.mark.parametrize('mode',[('cell'),('node')])
def test_displacement_fluct_vanishes(self,mode):
@pytest.mark.parametrize('function',[grid_filters.cell_displacement_fluct,
grid_filters.node_displacement_fluct])
def test_displacement_fluct_vanishes(self,function):
"""Ensure that constant F does not result in fluctuating displacement."""
size = np.random.random(3) # noqa
size = np.random.random(3)
grid = np.random.randint(8,32,(3))
F = np.broadcast_to(np.random.random((3,3)), tuple(grid)+(3,3)) # noqa
assert np.allclose(eval('grid_filters.{}_displacement_fluct(size,F)'.format(mode)),0.0)
F = np.broadcast_to(np.random.random((3,3)), tuple(grid)+(3,3))
assert np.allclose(function(size,F),0.0)
def test_regrid(self):
size = np.random.random(3)

59
src/LAPACK_interface.f90 Normal file
View File

@ -0,0 +1,59 @@
!--------------------------------------------------------------------------------------------------
!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
!> @brief Fortran interfaces for LAPACK routines
!> @details https://www.netlib.org/lapack/
!--------------------------------------------------------------------------------------------------
module LAPACK_interface
interface
subroutine dgeev(jobvl,jobvr,n,a,lda,wr,wi,vl,ldvl,vr,ldvr,work,lwork,info)
use prec
character, intent(in) :: jobvl,jobvr
integer, intent(in) :: n,lda,ldvl,ldvr,lwork
real(pReal), intent(inout), dimension(lda,n) :: a
real(pReal), intent(out), dimension(n) :: wr,wi
real(pReal), intent(out), dimension(ldvl,n) :: vl
real(pReal), intent(out), dimension(ldvr,n) :: vr
real(pReal), intent(out), dimension(max(1,lwork)) :: work
integer, intent(out) :: info
end subroutine dgeev
subroutine dgesv(n,nrhs,a,lda,ipiv,b,ldb,info)
use prec
integer, intent(in) :: n,nrhs,lda,ldb
real(pReal), intent(inout), dimension(lda,n) :: a
integer, intent(out), dimension(n) :: ipiv
real(pReal), intent(out), dimension(ldb,nrhs) :: b
integer, intent(out) :: info
end subroutine dgesv
subroutine dgetrf(m,n,a,lda,ipiv,info)
use prec
integer, intent(in) :: m,n,lda
real(pReal), intent(inout), dimension(lda,n) :: a
integer, intent(out), dimension(min(m,n)) :: ipiv
integer, intent(out) :: info
end subroutine dgetrf
subroutine dgetri(n,a,lda,ipiv,work,lwork,info)
use prec
integer, intent(in) :: n,lda,lwork
real(pReal), intent(inout), dimension(lda,n) :: a
integer, intent(out), dimension(n) :: ipiv
real(pReal), intent(out), dimension(max(1,lwork)) :: work
integer, intent(out) :: info
end subroutine dgetri
subroutine dsyev(jobz,uplo,n,a,lda,w,work,lwork,info)
use prec
character, intent(in) :: jobz,uplo
integer, intent(in) :: n,lda,lwork
real(pReal), intent(inout), dimension(lda,n) :: a
real(pReal), intent(out), dimension(n) :: w
real(pReal), intent(out), dimension(max(1,lwork)) :: work
integer, intent(out) :: info
end subroutine dsyev
end interface
end module LAPACK_interface

View File

@ -9,6 +9,7 @@
#include "list.f90"
#include "future.f90"
#include "config.f90"
#include "LAPACK_interface.f90"
#include "math.f90"
#include "quaternions.f90"
#include "Lambert.f90"

View File

@ -835,8 +835,6 @@ logical function integrateStress(ipc,ip,el,timeFraction)
jacoCounterLp, &
jacoCounterLi ! counters to check for Jacobian update
logical :: error
external :: &
dgesv
integrateStress = .false.

View File

@ -27,33 +27,22 @@ module homogenization
implicit none
private
!--------------------------------------------------------------------------------------------------
! General variables for the homogenization at a material point
logical, public :: &
terminallyIll = .false. !< at least one material point is terminally ill
real(pReal), dimension(:,:,:,:), allocatable, public :: &
materialpoint_F0, & !< def grad of IP at start of FE increment
materialpoint_F, & !< def grad of IP to be reached at end of FE increment
materialpoint_P !< first P--K stress of IP
real(pReal), dimension(:,:,:,:,:,:), allocatable, public :: &
materialpoint_dPdF !< tangent of first P--K stress at IP
real(pReal), dimension(:,:,:,:), allocatable :: &
materialpoint_subF0, & !< def grad of IP at beginning of homogenization increment
materialpoint_subF !< def grad of IP to be reached at end of homog inc
real(pReal), dimension(:,:), allocatable :: &
materialpoint_subFrac, &
materialpoint_subStep, &
materialpoint_subdt
logical, dimension(:,:), allocatable :: &
materialpoint_requested, &
materialpoint_converged
logical, dimension(:,:,:), allocatable :: &
materialpoint_doneAndHappy
!--------------------------------------------------------------------------------------------------
! General variables for the homogenization at a material point
real(pReal), dimension(:,:,:,:), allocatable, public :: &
materialpoint_F0, & !< def grad of IP at start of FE increment
materialpoint_F !< def grad of IP to be reached at end of FE increment
real(pReal), dimension(:,:,:,:), allocatable, public, protected :: &
materialpoint_P !< first P--K stress of IP
real(pReal), dimension(:,:,:,:,:,:), allocatable, public, protected :: &
materialpoint_dPdF !< tangent of first P--K stress at IP
type :: tNumerics
integer :: &
nMPstate !< materialpoint state loop limit
nMPstate !< materialpoint state loop limit
real(pReal) :: &
subStepMinHomog, & !< minimum (relative) size of sub-step allowed during cutback in homogenization
subStepSizeHomog, & !< size of first substep when cutback in homogenization
@ -161,15 +150,7 @@ subroutine homogenization_init
allocate(materialpoint_dPdF(3,3,3,3,discretization_nIP,discretization_nElem), source=0.0_pReal)
materialpoint_F0 = spread(spread(math_I3,3,discretization_nIP),4,discretization_nElem) ! initialize to identity
materialpoint_F = materialpoint_F0 ! initialize to identity
allocate(materialpoint_subF0(3,3,discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_subF(3,3,discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_P(3,3,discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_subFrac(discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_subStep(discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_subdt(discretization_nIP,discretization_nElem), source=0.0_pReal)
allocate(materialpoint_requested(discretization_nIP,discretization_nElem), source=.false.)
allocate(materialpoint_converged(discretization_nIP,discretization_nElem), source=.true.)
allocate(materialpoint_doneAndHappy(2,discretization_nIP,discretization_nElem), source=.true.)
write(6,'(/,a)') ' <<<+- homogenization init -+>>>'; flush(6)
@ -203,6 +184,14 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
e, & !< element number
mySource, &
myNgrains
real(pReal), dimension(discretization_nIP,discretization_nElem) :: &
subFrac, &
subStep
logical, dimension(discretization_nIP,discretization_nElem) :: &
requested, &
converged
logical, dimension(2,discretization_nIP,discretization_nElem) :: &
doneAndHappy
#ifdef DEBUG
if (iand(debug_level(debug_homogenization), debug_levelBasic) /= 0) then
@ -216,7 +205,7 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
#endif
!--------------------------------------------------------------------------------------------------
! initialize restoration points of ...
! initialize restoration points
do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(material_homogenizationAt(e))
do i = FEsolving_execIP(1),FEsolving_execIP(2);
@ -238,74 +227,60 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
enddo
materialpoint_subF0(1:3,1:3,i,e) = materialpoint_F0(1:3,1:3,i,e)
materialpoint_subFrac(i,e) = 0.0_pReal
materialpoint_subStep(i,e) = 1.0_pReal/num%subStepSizeHomog ! <<added to adopt flexibility in cutback size>>
materialpoint_converged(i,e) = .false. ! pretend failed step of twice the required size
materialpoint_requested(i,e) = .true. ! everybody requires calculation
subFrac(i,e) = 0.0_pReal
converged(i,e) = .false. ! pretend failed step ...
subStep(i,e) = 1.0_pReal/num%subStepSizeHomog ! ... larger then the requested calculation
requested(i,e) = .true. ! everybody requires calculation
if (homogState(material_homogenizationAt(e))%sizeState > 0) &
homogState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e)) = &
homogState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e)) ! ...internal homogenization state
homogState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e))
if (thermalState(material_homogenizationAt(e))%sizeState > 0) &
thermalState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e)) = &
thermalState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e)) ! ...internal thermal state
thermalState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e))
if (damageState(material_homogenizationAt(e))%sizeState > 0) &
damageState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e)) = &
damageState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e)) ! ...internal damage state
damageState(material_homogenizationAt(e))%State0( :,material_homogenizationMemberAt(i,e))
enddo
enddo
NiterationHomog = 0
cutBackLooping: do while (.not. terminallyIll .and. &
any(materialpoint_subStep(:,FEsolving_execELem(1):FEsolving_execElem(2)) > num%subStepMinHomog))
any(subStep(:,FEsolving_execELem(1):FEsolving_execElem(2)) > num%subStepMinHomog))
!$OMP PARALLEL DO PRIVATE(myNgrains)
elementLooping1: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(material_homogenizationAt(e))
IpLooping1: do i = FEsolving_execIP(1),FEsolving_execIP(2)
converged: if (materialpoint_converged(i,e)) then
if (converged(i,e)) then
#ifdef DEBUG
if (iand(debug_level(debug_homogenization), debug_levelExtensive) /= 0 &
.and. ((e == debug_e .and. i == debug_i) &
.or. .not. iand(debug_level(debug_homogenization),debug_levelSelective) /= 0)) then
write(6,'(a,1x,f12.8,1x,a,1x,f12.8,1x,a,i8,1x,i2/)') '<< HOMOG >> winding forward from', &
materialpoint_subFrac(i,e), 'to current materialpoint_subFrac', &
materialpoint_subFrac(i,e)+materialpoint_subStep(i,e),'in materialpoint_stressAndItsTangent at el ip',e,i
subFrac(i,e), 'to current subFrac', &
subFrac(i,e)+subStep(i,e),'in materialpoint_stressAndItsTangent at el ip',e,i
endif
#endif
!---------------------------------------------------------------------------------------------------
! calculate new subStep and new subFrac
materialpoint_subFrac(i,e) = materialpoint_subFrac(i,e) + materialpoint_subStep(i,e)
materialpoint_subStep(i,e) = min(1.0_pReal-materialpoint_subFrac(i,e), &
num%stepIncreaseHomog*materialpoint_subStep(i,e)) ! introduce flexibility for step increase/acceleration
subFrac(i,e) = subFrac(i,e) + subStep(i,e)
subStep(i,e) = min(1.0_pReal-subFrac(i,e),num%stepIncreaseHomog*subStep(i,e)) ! introduce flexibility for step increase/acceleration
steppingNeeded: if (materialpoint_subStep(i,e) > num%subStepMinHomog) then
steppingNeeded: if (subStep(i,e) > num%subStepMinHomog) then
! wind forward grain starting point of...
crystallite_partionedF0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedF(1:3,1:3,1:myNgrains,i,e)
crystallite_partionedFp0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_Fp (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedLp0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_Lp (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedFi0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_Fi (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedLi0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_Li (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedS0 (1:3,1:3,1:myNgrains,i,e) = &
crystallite_S (1:3,1:3,1:myNgrains,i,e)
! wind forward grain starting point
crystallite_partionedF0 (1:3,1:3,1:myNgrains,i,e) = crystallite_partionedF(1:3,1:3,1:myNgrains,i,e)
crystallite_partionedFp0(1:3,1:3,1:myNgrains,i,e) = crystallite_Fp (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedLp0(1:3,1:3,1:myNgrains,i,e) = crystallite_Lp (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedFi0(1:3,1:3,1:myNgrains,i,e) = crystallite_Fi (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedLi0(1:3,1:3,1:myNgrains,i,e) = crystallite_Li (1:3,1:3,1:myNgrains,i,e)
crystallite_partionedS0 (1:3,1:3,1:myNgrains,i,e) = crystallite_S (1:3,1:3,1:myNgrains,i,e)
do g = 1,myNgrains
plasticState (material_phaseAt(g,e))%partionedState0(:,material_phasememberAt(g,i,e)) = &
@ -326,15 +301,12 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
damageState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e)) = &
damageState(material_homogenizationAt(e))%State (:,material_homogenizationMemberAt(i,e))
materialpoint_subF0(1:3,1:3,i,e) = materialpoint_subF(1:3,1:3,i,e)
endif steppingNeeded
else converged
if ( (myNgrains == 1 .and. materialpoint_subStep(i,e) <= 1.0 ) .or. & ! single grain already tried internal subStepping in crystallite
num%subStepSizeHomog * materialpoint_subStep(i,e) <= num%subStepMinHomog ) then ! would require too small subStep
else
if ( (myNgrains == 1 .and. subStep(i,e) <= 1.0 ) .or. & ! single grain already tried internal subStepping in crystallite
num%subStepSizeHomog * subStep(i,e) <= num%subStepMinHomog ) then ! would require too small subStep
! cutback makes no sense
!$OMP FLUSH(terminallyIll)
if (.not. terminallyIll) then ! so first signals terminally ill...
!$OMP CRITICAL (write2out)
write(6,*) 'Integration point ', i,' at element ', e, ' terminally ill'
@ -342,32 +314,27 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
endif
terminallyIll = .true. ! ...and kills all others
else ! cutback makes sense
materialpoint_subStep(i,e) = num%subStepSizeHomog * materialpoint_subStep(i,e) ! crystallite had severe trouble, so do a significant cutback
subStep(i,e) = num%subStepSizeHomog * subStep(i,e) ! crystallite had severe trouble, so do a significant cutback
#ifdef DEBUG
if (iand(debug_level(debug_homogenization), debug_levelExtensive) /= 0 &
.and. ((e == debug_e .and. i == debug_i) &
.or. .not. iand(debug_level(debug_homogenization), debug_levelSelective) /= 0)) then
write(6,'(a,1x,f12.8,a,i8,1x,i2/)') &
'<< HOMOG >> cutback step in materialpoint_stressAndItsTangent with new materialpoint_subStep:',&
materialpoint_subStep(i,e),' at el ip',e,i
'<< HOMOG >> cutback step in materialpoint_stressAndItsTangent with new subStep:',&
subStep(i,e),' at el ip',e,i
endif
#endif
!--------------------------------------------------------------------------------------------------
! restore...
if (materialpoint_subStep(i,e) < 1.0_pReal) then ! protect against fake cutback from \Delta t = 2 to 1. Maybe that "trick" is not necessary anymore at all? I.e. start with \Delta t = 1
crystallite_Lp(1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedLp0(1:3,1:3,1:myNgrains,i,e)
crystallite_Li(1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedLi0(1:3,1:3,1:myNgrains,i,e)
! restore
if (subStep(i,e) < 1.0_pReal) then ! protect against fake cutback from \Delta t = 2 to 1. Maybe that "trick" is not necessary anymore at all? I.e. start with \Delta t = 1
crystallite_Lp(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedLp0(1:3,1:3,1:myNgrains,i,e)
crystallite_Li(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedLi0(1:3,1:3,1:myNgrains,i,e)
endif ! maybe protecting everything from overwriting (not only L) makes even more sense
crystallite_Fp(1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedFp0(1:3,1:3,1:myNgrains,i,e)
crystallite_Fi(1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedFi0(1:3,1:3,1:myNgrains,i,e)
crystallite_S(1:3,1:3,1:myNgrains,i,e) = &
crystallite_partionedS0(1:3,1:3,1:myNgrains,i,e)
crystallite_Fp(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedFp0(1:3,1:3,1:myNgrains,i,e)
crystallite_Fi(1:3,1:3,1:myNgrains,i,e) = crystallite_partionedFi0(1:3,1:3,1:myNgrains,i,e)
crystallite_S (1:3,1:3,1:myNgrains,i,e) = crystallite_partionedS0 (1:3,1:3,1:myNgrains,i,e)
do g = 1, myNgrains
plasticState (material_phaseAt(g,e))%state( :,material_phasememberAt(g,i,e)) = &
plasticState (material_phaseAt(g,e))%partionedState0(:,material_phasememberAt(g,i,e))
@ -386,15 +353,11 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
damageState(material_homogenizationAt(e))%State( :,material_homogenizationMemberAt(i,e)) = &
damageState(material_homogenizationAt(e))%subState0(:,material_homogenizationMemberAt(i,e))
endif
endif converged
endif
if (materialpoint_subStep(i,e) > num%subStepMinHomog) then
materialpoint_requested(i,e) = .true.
materialpoint_subF(1:3,1:3,i,e) = materialpoint_subF0(1:3,1:3,i,e) &
+ materialpoint_subStep(i,e) * (materialpoint_F(1:3,1:3,i,e) &
- materialpoint_F0(1:3,1:3,i,e))
materialpoint_subdt(i,e) = materialpoint_subStep(i,e) * dt
materialpoint_doneAndHappy(1:2,i,e) = [.false.,.true.]
if (subStep(i,e) > num%subStepMinHomog) then
requested(i,e) = .true.
doneAndHappy(1:2,i,e) = [.false.,.true.]
endif
enddo IpLooping1
enddo elementLooping1
@ -403,24 +366,24 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
NiterationMPstate = 0
convergenceLooping: do while (.not. terminallyIll .and. &
any( materialpoint_requested(:,FEsolving_execELem(1):FEsolving_execElem(2)) &
.and. .not. materialpoint_doneAndHappy(1,:,FEsolving_execELem(1):FEsolving_execElem(2)) &
any( requested(:,FEsolving_execELem(1):FEsolving_execElem(2)) &
.and. .not. doneAndHappy(1,:,FEsolving_execELem(1):FEsolving_execElem(2)) &
) .and. &
NiterationMPstate < num%nMPstate)
NiterationMPstate = NiterationMPstate + 1
!--------------------------------------------------------------------------------------------------
! deformation partitioning
! based on materialpoint_subF0,.._subF,crystallite_partionedF0, and homogenization_state,
! results in crystallite_partionedF
!$OMP PARALLEL DO PRIVATE(myNgrains)
elementLooping2: do e = FEsolving_execElem(1),FEsolving_execElem(2)
myNgrains = homogenization_Ngrains(material_homogenizationAt(e))
IpLooping2: do i = FEsolving_execIP(1),FEsolving_execIP(2)
if ( materialpoint_requested(i,e) .and. & ! process requested but...
.not. materialpoint_doneAndHappy(1,i,e)) then ! ...not yet done material points
call partitionDeformation(i,e) ! partition deformation onto constituents
crystallite_dt(1:myNgrains,i,e) = materialpoint_subdt(i,e) ! propagate materialpoint dt to grains
if(requested(i,e) .and. .not. doneAndHappy(1,i,e)) then ! requested but not yet done
call partitionDeformation(materialpoint_F0(1:3,1:3,i,e) &
+ (materialpoint_F(1:3,1:3,i,e)-materialpoint_F0(1:3,1:3,i,e))&
*(subStep(i,e)+subFrac(i,e)), &
i,e)
crystallite_dt(1:myNgrains,i,e) = dt*subStep(i,e) ! propagate materialpoint dt to grains
crystallite_requested(1:myNgrains,i,e) = .true. ! request calculation for constituents
else
crystallite_requested(1:myNgrains,i,e) = .false. ! calculation for constituents not required anymore
@ -431,23 +394,23 @@ subroutine materialpoint_stressAndItsTangent(updateJaco,dt)
!--------------------------------------------------------------------------------------------------
! crystallite integration
! based on crystallite_partionedF0,.._partionedF
! incrementing by crystallite_dt
materialpoint_converged = crystallite_stress() !ToDo: MD not sure if that is the best logic
converged = crystallite_stress() !ToDo: MD not sure if that is the best logic
!--------------------------------------------------------------------------------------------------
! state update
!$OMP PARALLEL DO
elementLooping3: do e = FEsolving_execElem(1),FEsolving_execElem(2)
IpLooping3: do i = FEsolving_execIP(1),FEsolving_execIP(2)
if ( materialpoint_requested(i,e) .and. &
.not. materialpoint_doneAndHappy(1,i,e)) then
if (.not. materialpoint_converged(i,e)) then
materialpoint_doneAndHappy(1:2,i,e) = [.true.,.false.]
if (requested(i,e) .and. .not. doneAndHappy(1,i,e)) then
if (.not. converged(i,e)) then
doneAndHappy(1:2,i,e) = [.true.,.false.]
else
materialpoint_doneAndHappy(1:2,i,e) = updateState(i,e)
materialpoint_converged(i,e) = all(materialpoint_doneAndHappy(1:2,i,e)) ! converged if done and happy
doneAndHappy(1:2,i,e) = updateState(dt*subStep(i,e), &
materialpoint_F0(1:3,1:3,i,e) &
+ (materialpoint_F(1:3,1:3,i,e)-materialpoint_F0(1:3,1:3,i,e)) &
*(subStep(i,e)+subFrac(i,e)), &
i,e)
converged(i,e) = all(doneAndHappy(1:2,i,e)) ! converged if done and happy
endif
endif
enddo IpLooping3
@ -481,29 +444,31 @@ end subroutine materialpoint_stressAndItsTangent
!--------------------------------------------------------------------------------------------------
!> @brief partition material point def grad onto constituents
!--------------------------------------------------------------------------------------------------
subroutine partitionDeformation(ip,el)
subroutine partitionDeformation(subF,ip,el)
integer, intent(in) :: &
ip, & !< integration point
el !< element number
real(pReal), intent(in), dimension(3,3) :: &
subF
integer, intent(in) :: &
ip, & !< integration point
el !< element number
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
case (HOMOGENIZATION_NONE_ID) chosenHomogenization
crystallite_partionedF(1:3,1:3,1,ip,el) = materialpoint_subF(1:3,1:3,ip,el)
case (HOMOGENIZATION_NONE_ID) chosenHomogenization
crystallite_partionedF(1:3,1:3,1,ip,el) = subF
case (HOMOGENIZATION_ISOSTRAIN_ID) chosenHomogenization
call mech_isostrain_partitionDeformation(&
case (HOMOGENIZATION_ISOSTRAIN_ID) chosenHomogenization
call mech_isostrain_partitionDeformation(&
crystallite_partionedF(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
subF)
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
call mech_RGC_partitionDeformation(&
crystallite_partionedF(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
materialpoint_subF(1:3,1:3,ip,el))
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
call mech_RGC_partitionDeformation(&
crystallite_partionedF(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
materialpoint_subF(1:3,1:3,ip,el),&
ip, &
el)
end select chosenHomogenization
subF,&
ip, &
el)
end select chosenHomogenization
end subroutine partitionDeformation
@ -512,45 +477,49 @@ end subroutine partitionDeformation
!> @brief update the internal state of the homogenization scheme and tell whether "done" and
!> "happy" with result
!--------------------------------------------------------------------------------------------------
function updateState(ip,el)
function updateState(subdt,subF,ip,el)
integer, intent(in) :: &
ip, & !< integration point
el !< element number
logical, dimension(2) :: updateState
real(pReal), intent(in) :: &
subdt !< current time step
real(pReal), intent(in), dimension(3,3) :: &
subF
integer, intent(in) :: &
ip, & !< integration point
el !< element number
logical, dimension(2) :: updateState
updateState = .true.
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
updateState = &
updateState .and. &
mech_RGC_updateState(crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_partionedF(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_partionedF0(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el),&
materialpoint_subF(1:3,1:3,ip,el),&
materialpoint_subdt(ip,el), &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
ip, &
el)
end select chosenHomogenization
updateState = .true.
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
updateState = &
updateState .and. &
mech_RGC_updateState(crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_partionedF(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_partionedF0(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el),&
subF,&
subdt, &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
ip, &
el)
end select chosenHomogenization
chosenThermal: select case (thermal_type(material_homogenizationAt(el)))
case (THERMAL_adiabatic_ID) chosenThermal
updateState = &
updateState .and. &
thermal_adiabatic_updateState(materialpoint_subdt(ip,el), &
ip, &
el)
end select chosenThermal
chosenThermal: select case (thermal_type(material_homogenizationAt(el)))
case (THERMAL_adiabatic_ID) chosenThermal
updateState = &
updateState .and. &
thermal_adiabatic_updateState(subdt, &
ip, &
el)
end select chosenThermal
chosenDamage: select case (damage_type(material_homogenizationAt(el)))
case (DAMAGE_local_ID) chosenDamage
updateState = &
updateState .and. &
damage_local_updateState(materialpoint_subdt(ip,el), &
ip, &
el)
end select chosenDamage
chosenDamage: select case (damage_type(material_homogenizationAt(el)))
case (DAMAGE_local_ID) chosenDamage
updateState = &
updateState .and. &
damage_local_updateState(subdt, &
ip, &
el)
end select chosenDamage
end function updateState
@ -560,31 +529,31 @@ end function updateState
!--------------------------------------------------------------------------------------------------
subroutine averageStressAndItsTangent(ip,el)
integer, intent(in) :: &
ip, & !< integration point
el !< element number
integer, intent(in) :: &
ip, & !< integration point
el !< element number
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
case (HOMOGENIZATION_NONE_ID) chosenHomogenization
materialpoint_P(1:3,1:3,ip,el) = crystallite_P(1:3,1:3,1,ip,el)
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el) = crystallite_dPdF(1:3,1:3,1:3,1:3,1,ip,el)
chosenHomogenization: select case(homogenization_type(material_homogenizationAt(el)))
case (HOMOGENIZATION_NONE_ID) chosenHomogenization
materialpoint_P(1:3,1:3,ip,el) = crystallite_P(1:3,1:3,1,ip,el)
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el) = crystallite_dPdF(1:3,1:3,1:3,1:3,1,ip,el)
case (HOMOGENIZATION_ISOSTRAIN_ID) chosenHomogenization
call mech_isostrain_averageStressAndItsTangent(&
materialpoint_P(1:3,1:3,ip,el), &
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el),&
crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
homogenization_typeInstance(material_homogenizationAt(el)))
case (HOMOGENIZATION_ISOSTRAIN_ID) chosenHomogenization
call mech_isostrain_averageStressAndItsTangent(&
materialpoint_P(1:3,1:3,ip,el), &
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el),&
crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
homogenization_typeInstance(material_homogenizationAt(el)))
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
call mech_RGC_averageStressAndItsTangent(&
materialpoint_P(1:3,1:3,ip,el), &
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el),&
crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
homogenization_typeInstance(material_homogenizationAt(el)))
end select chosenHomogenization
case (HOMOGENIZATION_RGC_ID) chosenHomogenization
call mech_RGC_averageStressAndItsTangent(&
materialpoint_P(1:3,1:3,ip,el), &
materialpoint_dPdF(1:3,1:3,1:3,1:3,ip,el),&
crystallite_P(1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
crystallite_dPdF(1:3,1:3,1:3,1:3,1:homogenization_Ngrains(material_homogenizationAt(el)),ip,el), &
homogenization_typeInstance(material_homogenizationAt(el)))
end select chosenHomogenization
end subroutine averageStressAndItsTangent

View File

@ -9,6 +9,7 @@ module math
use prec
use IO
use numerics
use LAPACK_interface
implicit none
public
@ -485,18 +486,14 @@ function math_invSym3333(A)
real(pReal),dimension(3,3,3,3),intent(in) :: A
integer, dimension(6) :: ipiv6
real(pReal), dimension(6,6) :: temp66
real(pReal), dimension(6*(64+2)) :: work
integer :: ierr_i, ierr_f
external :: &
dgetrf, &
dgetri
integer, dimension(6) :: ipiv6
real(pReal), dimension(6,6) :: temp66
real(pReal), dimension(6*6) :: work
integer :: ierr_i, ierr_f
temp66 = math_sym3333to66(A)
call dgetrf(6,6,temp66,6,ipiv6,ierr_i)
call dgetri(6,temp66,6,ipiv6,work,size(work,1),ierr_f)
if (ierr_i /= 0 .or. ierr_f /= 0) then
call IO_error(400, ext_msg = 'math_invSym3333')
else
@ -515,12 +512,9 @@ subroutine math_invert(InvA, error, A)
real(pReal), dimension(size(A,1),size(A,1)), intent(out) :: invA
logical, intent(out) :: error
integer, dimension(size(A,1)) :: ipiv
real(pReal), dimension(size(A,1)*(64+2)) :: work
integer :: ierr
external :: &
dgetrf, &
dgetri
integer, dimension(size(A,1)) :: ipiv
real(pReal), dimension(size(A,1)**2) :: work
integer :: ierr
invA = A
call dgetrf(size(A,1),size(A,1),invA,size(A,1),ipiv,ierr)
@ -884,9 +878,7 @@ subroutine math_eigh(m,w,v,error)
logical, intent(out) :: error
integer :: ierr
real(pReal), dimension((64+2)*size(m,1)) :: work ! block size of 64 taken from http://www.netlib.org/lapack/double/dsyev.f
external :: &
dsyev
real(pReal), dimension(size(m,1)**2) :: work
v = m ! copy matrix to input (doubles as output) array
call dsyev('V','U',size(m,1),v,size(m,1),w,work,size(work,1),ierr)
@ -1041,9 +1033,7 @@ function math_eigvalsh(m)
real(pReal), dimension(size(m,1),size(m,1)) :: m_
integer :: ierr
real(pReal), dimension((64+2)*size(m,1)) :: work ! block size of 64 taken from http://www.netlib.org/lapack/double/dsyev.f
external :: &
dsyev
real(pReal), dimension(size(m,1)**2) :: work
m_= m ! copy matrix to input (will be destroyed)
call dsyev('N','U',size(m,1),m_,size(m,1),math_eigvalsh,work,size(work,1),ierr)

View File

@ -63,27 +63,27 @@ module quaternions
module procedure assign_quat__
module procedure assign_vec__
end interface assignment (=)
interface quaternion
module procedure init__
end interface quaternion
interface abs
procedure abs__
end interface abs
interface dot_product
procedure dot_product__
end interface dot_product
interface conjg
module procedure conjg__
end interface conjg
interface exp
module procedure exp__
end interface exp
interface log
module procedure log__
end interface log
@ -95,7 +95,7 @@ module quaternions
interface aimag
module procedure aimag__
end interface aimag
public :: &
quaternions_init, &
assignment(=), &
@ -118,7 +118,7 @@ end subroutine quaternions_init
!---------------------------------------------------------------------------------------------------
!> construct a quaternion from a 4-vector
!> @brief construct a quaternion from a 4-vector
!---------------------------------------------------------------------------------------------------
type(quaternion) pure function init__(array)
@ -133,7 +133,7 @@ end function init__
!---------------------------------------------------------------------------------------------------
!> assign a quaternion
!> @brief assign a quaternion
!---------------------------------------------------------------------------------------------------
elemental pure subroutine assign_quat__(self,other)
@ -141,12 +141,12 @@ elemental pure subroutine assign_quat__(self,other)
type(quaternion), intent(in) :: other
self = [other%w,other%x,other%y,other%z]
end subroutine assign_quat__
!---------------------------------------------------------------------------------------------------
!> assign a 4-vector
!> @brief assign a 4-vector
!---------------------------------------------------------------------------------------------------
pure subroutine assign_vec__(self,other)
@ -162,7 +162,7 @@ end subroutine assign_vec__
!---------------------------------------------------------------------------------------------------
!> add a quaternion
!> @brief add a quaternion
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function add__(self,other)
@ -170,24 +170,24 @@ type(quaternion) elemental pure function add__(self,other)
add__ = [ self%w, self%x, self%y ,self%z] &
+ [other%w, other%x, other%y,other%z]
end function add__
!---------------------------------------------------------------------------------------------------
!> return (unary positive operator)
!> @brief return (unary positive operator)
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function pos__(self)
class(quaternion), intent(in) :: self
pos__ = self * (+1.0_pReal)
end function pos__
!---------------------------------------------------------------------------------------------------
!> subtract a quaternion
!> @brief subtract a quaternion
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function sub__(self,other)
@ -195,24 +195,24 @@ type(quaternion) elemental pure function sub__(self,other)
sub__ = [ self%w, self%x, self%y ,self%z] &
- [other%w, other%x, other%y,other%z]
end function sub__
!---------------------------------------------------------------------------------------------------
!> negate (unary negative operator)
!> @brief negate (unary negative operator)
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function neg__(self)
class(quaternion), intent(in) :: self
neg__ = self * (-1.0_pReal)
end function neg__
!---------------------------------------------------------------------------------------------------
!> multiply with a quaternion
!> @brief multiply with a quaternion
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function mul_quat__(self,other)
@ -227,7 +227,7 @@ end function mul_quat__
!---------------------------------------------------------------------------------------------------
!> multiply with a scalar
!> @brief multiply with a scalar
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function mul_scal__(self,scal)
@ -235,12 +235,12 @@ type(quaternion) elemental pure function mul_scal__(self,scal)
real(pReal), intent(in) :: scal
mul_scal__ = [self%w,self%x,self%y,self%z]*scal
end function mul_scal__
!---------------------------------------------------------------------------------------------------
!> divide by a quaternion
!> @brief divide by a quaternion
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function div_quat__(self,other)
@ -252,7 +252,7 @@ end function div_quat__
!---------------------------------------------------------------------------------------------------
!> divide by a scalar
!> @brief divide by a scalar
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function div_scal__(self,scal)
@ -265,7 +265,7 @@ end function div_scal__
!---------------------------------------------------------------------------------------------------
!> test equality
!> @brief test equality
!---------------------------------------------------------------------------------------------------
logical elemental pure function eq__(self,other)
@ -278,7 +278,7 @@ end function eq__
!---------------------------------------------------------------------------------------------------
!> test inequality
!> @brief test inequality
!---------------------------------------------------------------------------------------------------
logical elemental pure function neq__(self,other)
@ -290,7 +290,7 @@ end function neq__
!---------------------------------------------------------------------------------------------------
!> raise to the power of a quaternion
!> @brief raise to the power of a quaternion
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function pow_quat__(self,expon)
@ -303,7 +303,7 @@ end function pow_quat__
!---------------------------------------------------------------------------------------------------
!> raise to the power of a scalar
!> @brief raise to the power of a scalar
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function pow_scal__(self,expon)
@ -316,7 +316,7 @@ end function pow_scal__
!---------------------------------------------------------------------------------------------------
!> take exponential
!> @brief take exponential
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function exp__(a)
@ -336,7 +336,7 @@ end function exp__
!---------------------------------------------------------------------------------------------------
!> take logarithm
!> @brief take logarithm
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function log__(a)
@ -356,7 +356,7 @@ end function log__
!---------------------------------------------------------------------------------------------------
!> return norm
!> @brief return norm
!---------------------------------------------------------------------------------------------------
real(pReal) elemental pure function abs__(self)
@ -368,7 +368,7 @@ end function abs__
!---------------------------------------------------------------------------------------------------
!> calculate dot product
!> @brief calculate dot product
!---------------------------------------------------------------------------------------------------
real(pReal) elemental pure function dot_product__(a,b)
@ -380,7 +380,7 @@ end function dot_product__
!---------------------------------------------------------------------------------------------------
!> take conjugate complex
!> @brief take conjugate complex
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function conjg__(self)
@ -392,7 +392,7 @@ end function conjg__
!---------------------------------------------------------------------------------------------------
!> homomorph
!> @brief homomorph
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function homomorphed(self)
@ -404,7 +404,7 @@ end function homomorphed
!---------------------------------------------------------------------------------------------------
!> return as plain array
!> @brief return as plain array
!---------------------------------------------------------------------------------------------------
pure function asArray(self)
@ -417,7 +417,7 @@ end function asArray
!---------------------------------------------------------------------------------------------------
!> real part (scalar)
!> @brief real part (scalar)
!---------------------------------------------------------------------------------------------------
pure function real__(self)
@ -430,7 +430,7 @@ end function real__
!---------------------------------------------------------------------------------------------------
!> imaginary part (3-vector)
!> @brief imaginary part (3-vector)
!---------------------------------------------------------------------------------------------------
pure function aimag__(self)
@ -443,7 +443,7 @@ end function aimag__
!---------------------------------------------------------------------------------------------------
!> inverse
!> @brief inverse
!---------------------------------------------------------------------------------------------------
type(quaternion) elemental pure function inverse(self)

View File

@ -595,8 +595,6 @@ function om2ax(om) result(ax)
real(pReal), dimension(3,3) :: VR, devNull, om_
integer :: ierr, i
external :: dgeev
om_ = om
! first get the rotation angle