diff --git a/VERSION b/VERSION
index bbcfb4711..503e3894e 100644
--- a/VERSION
+++ b/VERSION
@@ -1 +1 @@
-v3.0.0-alpha2-602-ge2d4ab427
+v3.0.0-alpha2-646-gee8015cd5
diff --git a/examples/ConfigFiles/Phase_Isotropic_FreeSurface.yaml b/examples/ConfigFiles/Phase_Isotropic_FreeSurface.yaml
index df3a352cb..8d8d1354d 100644
--- a/examples/ConfigFiles/Phase_Isotropic_FreeSurface.yaml
+++ b/examples/ConfigFiles/Phase_Isotropic_FreeSurface.yaml
@@ -1,4 +1,4 @@
-Air:
+FreeSurface:
lattice: aP
mechanical:
output: [F, P, F_e, F_p, L_p]
diff --git a/examples/ConfigFiles/Phase_Phenopowerlaw_Magnesium.yaml b/examples/ConfigFiles/Phase_Phenopowerlaw_Magnesium.yaml
index d298ae201..6540fb880 100644
--- a/examples/ConfigFiles/Phase_Phenopowerlaw_Magnesium.yaml
+++ b/examples/ConfigFiles/Phase_Phenopowerlaw_Magnesium.yaml
@@ -20,9 +20,6 @@ Magnesium:
xi_0_sl: [10.0e6, 55.0e6, 0, 60.0e6, 0.0, 60.0e6]
xi_inf_sl: [40.0e6, 135.0e6, 0, 150.0e6, 0.0, 150.0e6]
xi_0_tw: [40e6, 0.0, 0.0, 60.0e6]
-####################################################
-# open for discussion
-####################################################
a_sl: 2.25
dot_gamma_0_sl: 0.001
dot_gamma_0_tw: 0.001
diff --git a/examples/ConfigFiles/Phase_Phenopowerlaw_cpTi.yaml b/examples/ConfigFiles/Phase_Phenopowerlaw_cpTi.yaml
index 9bc82ea92..2a444d570 100644
--- a/examples/ConfigFiles/Phase_Phenopowerlaw_cpTi.yaml
+++ b/examples/ConfigFiles/Phase_Phenopowerlaw_cpTi.yaml
@@ -8,7 +8,7 @@ cpTi:
output: [F, P, F_e, F_p, L_p, O]
elastic: {C_11: 160.0e9, C_12: 90.0e9, C_13: 66.0e9, C_33: 181.7e9, C_44: 46.5e9, type: hooke}
plastic:
- N_sl: [3, 3, 0, 0, 12]
+ N_sl: [3, 3, 0, 6, 12]
a_sl: 2.0
dot_gamma_0_sl: 0.001
h_0_sl_sl: 200e6
diff --git a/examples/FEM/polyXtal/material.yaml b/examples/mesh/material.yaml
similarity index 100%
rename from examples/FEM/polyXtal/material.yaml
rename to examples/mesh/material.yaml
diff --git a/examples/FEM/polyXtal/numerics.config b/examples/mesh/numerics.config
similarity index 100%
rename from examples/FEM/polyXtal/numerics.config
rename to examples/mesh/numerics.config
diff --git a/examples/FEM/polyXtal/polyXtal_100grains.msh b/examples/mesh/polyXtal_100grains.msh
similarity index 100%
rename from examples/FEM/polyXtal/polyXtal_100grains.msh
rename to examples/mesh/polyXtal_100grains.msh
diff --git a/examples/FEM/polyXtal/polyXtal_20grains.msh b/examples/mesh/polyXtal_20grains.msh
similarity index 100%
rename from examples/FEM/polyXtal/polyXtal_20grains.msh
rename to examples/mesh/polyXtal_20grains.msh
diff --git a/examples/FEM/polyXtal/tensionZ.load b/examples/mesh/tensionZ.load
similarity index 100%
rename from examples/FEM/polyXtal/tensionZ.load
rename to examples/mesh/tensionZ.load
diff --git a/processing/pre/geom_fromDREAM3D.py b/processing/pre/geom_fromDREAM3D.py
index d51a2b51e..e4840fc80 100755
--- a/processing/pre/geom_fromDREAM3D.py
+++ b/processing/pre/geom_fromDREAM3D.py
@@ -65,7 +65,7 @@ if filenames == []: parser.error('no input file specified.')
for name in filenames:
damask.util.report(scriptName,name)
- geom = damask.Grid.load_DREAM3D(name,options.basegroup,options.pointwise)
+ geom = damask.Grid.load_DREAM3D(name,'FeatureIds')
damask.util.croak(geom)
geom.save_ASCII(os.path.splitext(name)[0]+'.geom')
diff --git a/python/damask/_colormap.py b/python/damask/_colormap.py
index 7e8860dae..639a5a04c 100644
--- a/python/damask/_colormap.py
+++ b/python/damask/_colormap.py
@@ -27,12 +27,14 @@ class Colormap(mpl.colors.ListedColormap):
References
----------
- [1] DAMASK colormap theory
- https://www.kennethmoreland.com/color-maps/ColorMapsExpanded.pdf
- [2] DAMASK colormaps first use
- https://doi.org/10.1016/j.ijplas.2012.09.012
- [3] Matplotlib colormaps overview
- https://matplotlib.org/tutorials/colors/colormaps.html
+ K. Moreland, Proceedings of the 5th International Symposium on Advances in Visual Computing, 2009
+ https://doi.org/10.1007/978-3-642-10520-3_9
+
+ P. Eisenlohr et al., International Journal of Plasticity 46:37–53, 2013
+ https://doi.org/10.1016/j.ijplas.2012.09.012
+
+ Matplotlib colormaps overview
+ https://matplotlib.org/tutorials/colors/colormaps.html
"""
@@ -524,7 +526,7 @@ class Colormap(mpl.colors.ListedColormap):
References
----------
- http://www.ryanjuckett.com/programming/rgb-color-space-conversion
+ https://www.easyrgb.com/en/math.php
"""
rgb_lin = np.dot(np.array([
@@ -544,7 +546,7 @@ class Colormap(mpl.colors.ListedColormap):
References
----------
- http://www.ryanjuckett.com/programming/rgb-color-space-conversion
+ https://www.easyrgb.com/en/math.php
"""
rgb_lin = np.where(rgb>0.04045,((rgb+0.0555)/1.0555)**2.4,rgb/12.92)
diff --git a/python/damask/_configmaterial.py b/python/damask/_configmaterial.py
index e2f34e92a..fb9b41932 100644
--- a/python/damask/_configmaterial.py
+++ b/python/damask/_configmaterial.py
@@ -1,4 +1,7 @@
+import os.path
+
import numpy as np
+import h5py
from . import Config
from . import Rotation
@@ -49,7 +52,7 @@ class ConfigMaterial(Config):
@staticmethod
def from_table(table,**kwargs):
"""
- Load from an ASCII table.
+ Generate from an ASCII table.
Parameters
----------
@@ -85,7 +88,7 @@ class ConfigMaterial(Config):
phase: {}
"""
- kwargs_ = {k:table.get(v) for k,v in kwargs.items()}
+ kwargs_ = {k:table.get(v) for k,v in kwargs.items()}
_,idx = np.unique(np.hstack(list(kwargs_.values())),return_index=True,axis=0)
idx = np.sort(idx)
@@ -94,6 +97,79 @@ class ConfigMaterial(Config):
return ConfigMaterial().material_add(**kwargs_)
+ @staticmethod
+ def load_DREAM3D(fname,
+ grain_data=None,cell_data=None,cell_ensemble_data='CellEnsembleData',
+ phases='Phases',Euler_angles='EulerAngles',phase_names='PhaseName',
+ base_group=None):
+ """
+ Load DREAM.3D (HDF5) file.
+
+ Data in DREAM.3D files can be stored per cell ('CellData')
+ and/or per grain ('Grain Data'). Per default, cell-wise data
+ is assumed.
+
+ damask.Grid.load_DREAM3D allows to get the corresponding geometry
+ for the grid solver.
+
+ Parameters
+ ----------
+ fname : str
+ Filename of the DREAM.3D (HDF5) file.
+ grain_data : str
+ Name of the group (folder) containing grain-wise data. Defaults
+ to None, in which case cell-wise data is used.
+ cell_data : str
+ Name of the group (folder) containing cell-wise data. Defaults to
+ None in wich case it is automatically detected.
+ cell_ensemble_data : str
+ Name of the group (folder) containing data of cell ensembles. This
+ group is used to inquire the name of the phases. Phases will get
+ numeric IDs if this group is not found. Defaults to 'CellEnsembleData'.
+ phases : str
+ Name of the dataset containing the phase ID (cell-wise or grain-wise).
+ Defaults to 'Phases'.
+ Euler_angles : str
+ Name of the dataset containing the crystallographic orientation as
+ Euler angles in radians (cell-wise or grain-wise). Defaults to 'EulerAngles'.
+ phase_names : str
+ Name of the dataset containing the phase names. Phases will get
+ numeric IDs if this dataset is not found. Defaults to 'PhaseName'.
+ base_group : str
+ Path to the group (folder) that contains geometry (_SIMPL_GEOMETRY),
+ and grain- or cell-wise data. Defaults to None, in which case
+ it is set as the path that contains _SIMPL_GEOMETRY/SPACING.
+
+ """
+ b = util.DREAM3D_base_group(fname) if base_group is None else base_group
+ c = util.DREAM3D_cell_data_group(fname) if cell_data is None else cell_data
+ f = h5py.File(fname,'r')
+
+ if grain_data is None:
+ phase = f[os.path.join(b,c,phases)][()].flatten()
+ O = Rotation.from_Euler_angles(f[os.path.join(b,c,Euler_angles)]).as_quaternion().reshape(-1,4) # noqa
+ _,idx = np.unique(np.hstack([O,phase.reshape(-1,1)]),return_index=True,axis=0)
+ idx = np.sort(idx)
+ else:
+ phase = f[os.path.join(b,grain_data,phases)][()]
+ O = Rotation.from_Euler_angles(f[os.path.join(b,grain_data,Euler_angles)]).as_quaternion() # noqa
+ idx = np.arange(phase.size)
+
+ if cell_ensemble_data is not None and phase_names is not None:
+ try:
+ names = np.array([s.decode() for s in f[os.path.join(b,cell_ensemble_data,phase_names)]])
+ phase = names[phase]
+ except KeyError:
+ pass
+
+
+ base_config = ConfigMaterial({'phase':{k if isinstance(k,int) else str(k):'t.b.d.' for k in np.unique(phase)},
+ 'homogenization':{'direct':{'N_constituents':1}}})
+ constituent = {k:np.atleast_1d(v[idx].squeeze()) for k,v in zip(['O','phase'],[O,phase])}
+
+ return base_config.material_add(**constituent,homogenization='direct')
+
+
@property
def is_complete(self):
"""Check for completeness."""
diff --git a/python/damask/_grid.py b/python/damask/_grid.py
index a58f2ca2c..a76f7f2c4 100644
--- a/python/damask/_grid.py
+++ b/python/damask/_grid.py
@@ -256,35 +256,62 @@ class Grid:
@staticmethod
- def load_DREAM3D(fname,base_group,point_data=None,material='FeatureIds'):
+ def load_DREAM3D(fname,
+ feature_IDs=None,cell_data=None,
+ phases='Phases',Euler_angles='EulerAngles',
+ base_group=None):
"""
- Load from DREAM.3D file.
+ Load DREAM.3D (HDF5) file.
+
+ Data in DREAM.3D files can be stored per cell ('CellData')
+ and/or per grain ('Grain Data'). Per default, cell-wise data
+ is assumed.
+
+ damask.ConfigMaterial.load_DREAM3D allows to get the
+ corresponding material definition.
Parameters
----------
fname : str
- Filename of the DREAM.3D file
+ Filename of the DREAM.3D (HDF5) file.
+ feature_IDs : str
+ Name of the dataset containing the mapping between cells and
+ grain-wise data. Defaults to 'None', in which case cell-wise
+ data is used.
+ cell_data : str
+ Name of the group (folder) containing cell-wise data. Defaults to
+ None in wich case it is automatically detected.
+ phases : str
+ Name of the dataset containing the phase ID. It is not used for
+ grain-wise data, i.e. when feature_IDs is not None.
+ Defaults to 'Phases'.
+ Euler_angles : str
+ Name of the dataset containing the crystallographic orientation as
+ Euler angles in radians It is not used for grain-wise data, i.e.
+ when feature_IDs is not None. Defaults to 'EulerAngles'.
base_group : str
- Name of the group (folder) below 'DataContainers',
- for example 'SyntheticVolumeDataContainer'.
- point_data : str, optional
- Name of the group (folder) containing the pointwise material data,
- for example 'CellData'. Defaults to None, in which case points are consecutively numbered.
- material : str, optional
- Name of the dataset containing the material ID.
- Defaults to 'FeatureIds'.
+ Path to the group (folder) that contains geometry (_SIMPL_GEOMETRY),
+ and grain- or cell-wise data. Defaults to None, in which case
+ it is set as the path that contains _SIMPL_GEOMETRY/SPACING.
+
"""
- root_dir ='DataContainers'
+ b = util.DREAM3D_base_group(fname) if base_group is None else base_group
+ c = util.DREAM3D_cell_data_group(fname) if cell_data is None else cell_data
f = h5py.File(fname, 'r')
- g = os.path.join(root_dir,base_group,'_SIMPL_GEOMETRY')
- cells = f[os.path.join(g,'DIMENSIONS')][()]
- size = f[os.path.join(g,'SPACING')][()] * cells
- origin = f[os.path.join(g,'ORIGIN')][()]
- ma = np.arange(cells.prod(),dtype=int) \
- if point_data is None else \
- np.reshape(f[os.path.join(root_dir,base_group,point_data,material)],cells.prod())
+ cells = f[os.path.join(b,'_SIMPL_GEOMETRY','DIMENSIONS')][()]
+ size = f[os.path.join(b,'_SIMPL_GEOMETRY','SPACING')] * cells
+ origin = f[os.path.join(b,'_SIMPL_GEOMETRY','ORIGIN')][()]
+
+ if feature_IDs is None:
+ phase = f[os.path.join(b,c,phases)][()].reshape(-1,1)
+ O = Rotation.from_Euler_angles(f[os.path.join(b,c,Euler_angles)]).as_quaternion().reshape(-1,4) # noqa
+ unique,unique_inverse = np.unique(np.hstack([O,phase]),return_inverse=True,axis=0)
+ ma = np.arange(cells.prod()) if len(unique) == cells.prod() else \
+ np.arange(unique.size)[np.argsort(pd.unique(unique_inverse))][unique_inverse]
+ else:
+ ma = f[os.path.join(b,c,feature_IDs)][()].flatten()
return Grid(ma.reshape(cells,order='F'),size,origin,util.execution_stamp('Grid','load_DREAM3D'))
@@ -482,18 +509,13 @@ class Grid:
References
----------
- Sébastien B G Blanquer, Maike Werner, Markus Hannula, Shahriar Sharifi,
- Guillaume P R Lajoinie, David Eglin, Jari Hyttinen, André A Poot, and Dirk W Grijpma
- Surface curvature in triply-periodic minimal surface architectures as
- a distinct design parameter in preparing advanced tissue engineering scaffolds
+ S.B.G. Blanquer et al., Biofabrication 9(2):025001, 2017
https://doi.org/10.1088/1758-5090/aa6553
- Meinhard Wohlgemuth, Nataliya Yufa, James Hoffman, and Edwin L. Thomas
- Triply Periodic Bicontinuous Cubic Microdomain Morphologies by Symmetries
+ M. Wohlgemuth et al., Macromolecules 34(17):6083-6089, 2001
https://doi.org/10.1021/ma0019499
- Meng-Ting Hsieh, Lorenzo Valdevit
- Minisurf – A minimal surface generator for finite element modeling and additive manufacturing
+ M.-T. Hsieh and L. Valdevit, Software Impacts 6:100026, 2020
https://doi.org/10.1016/j.simpa.2020.100026
"""
diff --git a/python/damask/_orientation.py b/python/damask/_orientation.py
index a14af98af..f05f47544 100644
--- a/python/damask/_orientation.py
+++ b/python/damask/_orientation.py
@@ -742,8 +742,7 @@ class Orientation(Rotation):
References
----------
- C.T. Young and J.L. Lytton, J. Appl. Phys. 43:1408–1417, 1972
- "Computer Generation and Identification of Kikuchi Projections"
+ C.T. Young and J.L. Lytton, Journal of Applied Physics 43:1408–1417, 1972
https://doi.org/10.1063/1.1661333
"""
@@ -1070,8 +1069,7 @@ class Orientation(Rotation):
References
----------
- J.C. Glez and J. Driver, J. Appl. Cryst. 34:280-288, 2001
- "Orientation distribution analysis in deformed grains"
+ J.C. Glez and J. Driver, Journal of Applied Crystallography 34:280-288, 2001
https://doi.org/10.1107/S0021889801003077
"""
diff --git a/python/damask/_result.py b/python/damask/_result.py
index 26dc59b0e..f247a8d07 100644
--- a/python/damask/_result.py
+++ b/python/damask/_result.py
@@ -66,12 +66,14 @@ class Result:
self.times = [round(f[i].attrs['time/s'],12) for i in self.increments] if self.version_minor < 12 else \
[round(f[i].attrs['t/s'],12) for i in self.increments]
- self.N_materialpoints, self.N_constituents = np.shape(f['mapping/phase'])
+ grp = 'mapping' if self.version_minor < 12 else 'cell_to'
- self.homogenizations = [m.decode() for m in np.unique(f['mapping/homogenization']
- ['Name' if self.version_minor < 12 else 'name'])]
- self.phases = [c.decode() for c in np.unique(f['mapping/phase']
- ['Name' if self.version_minor < 12 else 'name'])]
+ self.N_materialpoints, self.N_constituents = np.shape(f[f'{grp}/phase'])
+
+ self.homogenizations = [m.decode() for m in np.unique(f[f'{grp}/homogenization']
+ ['Name' if self.version_minor < 12 else 'label'])]
+ self.phases = [c.decode() for c in np.unique(f[f'{grp}/phase']
+ ['Name' if self.version_minor < 12 else 'label'])]
self.out_type_ph = []
for c in self.phases:
@@ -375,8 +377,9 @@ class Result:
inGeom = {}
inData = {}
# compatibility hack
- name = 'Name' if self.version_minor < 12 else 'name'
- member = 'Position' if self.version_minor < 12 else 'member'
+ name = 'Name' if self.version_minor < 12 else 'label'
+ member = 'Position' if self.version_minor < 12 else 'entry'
+ grp = 'mapping' if self.version_minor < 12 else 'cell_to'
with h5py.File(self.fname,'r') as f:
for dataset in sets:
for group in self.groups_with_datasets(dataset):
@@ -387,11 +390,11 @@ class Result:
if prop == 'geometry':
inGeom[key] = inData[key] = np.arange(self.N_materialpoints)
elif prop == 'phase':
- inGeom[key] = np.where(f['mapping/phase'][:,constituent][name] == str.encode(name))[0]
- inData[key] = f['mapping/phase'][inGeom[key],constituent][member]
+ inGeom[key] = np.where(f[f'{grp}/phase'][:,constituent][name] == str.encode(name))[0]
+ inData[key] = f[f'{grp}/phase'][inGeom[key],constituent][member]
elif prop == 'homogenization':
- inGeom[key] = np.where(f['mapping/homogenization'][name] == str.encode(name))[0]
- inData[key] = f['mapping/homogenization'][inGeom[key].tolist()][member]
+ inGeom[key] = np.where(f[f'{grp}/homogenization'][name] == str.encode(name))[0]
+ inData[key] = f[f'{grp}/homogenization'][inGeom[key].tolist()][member]
shape = np.shape(f[path])
data = np.full((self.N_materialpoints,) + (shape[1:] if len(shape)>1 else (1,)),
np.nan,
@@ -542,8 +545,9 @@ class Result:
"""
# compatibility hack
- name = 'Name' if self.version_minor < 12 else 'name'
- member = 'Position' if self.version_minor < 12 else 'member'
+ name = 'Name' if self.version_minor < 12 else 'label'
+ member = 'Position' if self.version_minor < 12 else 'entry'
+ grp = 'mapping' if self.version_minor < 12 else 'cell_to'
with h5py.File(self.fname,'r') as f:
shape = (self.N_materialpoints,) + np.shape(f[path[0]])[1:]
if len(shape) == 1: shape = shape +(1,)
@@ -555,17 +559,17 @@ class Result:
dataset = np.array(f[pa])
continue
- p = np.where(f['mapping/phase'][:,c][name] == str.encode(label))[0]
+ p = np.where(f[f'{grp}/phase'][:,c][name] == str.encode(label))[0]
if len(p)>0:
- u = (f['mapping/phase'][member][p,c])
+ u = (f[f'{grp}/phase'][member][p,c])
a = np.array(f[pa])
if len(a.shape) == 1:
a=a.reshape([a.shape[0],1])
dataset[p,:] = a[u,:]
- p = np.where(f['mapping/homogenization'][name] == str.encode(label))[0]
+ p = np.where(f[f'{grp}/homogenization'][name] == str.encode(label))[0]
if len(p)>0:
- u = (f['mapping/homogenization'][member][p.tolist()])
+ u = (f[f'{grp}/homogenization'][member][p.tolist()])
a = np.array(f[pa])
if len(a.shape) == 1:
a=a.reshape([a.shape[0],1])
@@ -1346,7 +1350,7 @@ class Result:
for o in self.iterate('out_type_ph'):
for c in range(self.N_constituents):
prefix = '' if self.N_constituents == 1 else f'constituent{c}/'
- if o not in ['mechanics', 'mechanical']: # compatitbility hack
+ if o not in ['mechanics', 'mechanical']: # compatibility hack
for _ in self.iterate('phases'):
path = self.get_dataset_location(label)
if len(path) == 0:
diff --git a/python/damask/_rotation.py b/python/damask/_rotation.py
index 34a5f81b7..40078e4d5 100644
--- a/python/damask/_rotation.py
+++ b/python/damask/_rotation.py
@@ -357,10 +357,8 @@ class Rotation:
References
----------
- Quaternion averaging
- F. Landis Markley, Yang Cheng, John L. Crassidis, Yaakov Oshman
- Journal of Guidance, Control, and Dynamics 30(4):1193-1197, 2007
- 10.2514/1.28949
+ F. Landis Markley et al., Journal of Guidance, Control, and Dynamics 30(4):1193-1197, 2007
+ https://doi.org/10.2514/1.28949
"""
def _M(quat):
@@ -859,7 +857,7 @@ class Rotation:
References
----------
- P. Eisenlohr, F. Roters, Computational Materials Science 42(4), 670-678, 2008
+ P. Eisenlohr and F. Roters, Computational Materials Science 42(4):670-678, 2008
https://doi.org/10.1016/j.commatsci.2007.09.015
"""
diff --git a/python/damask/util.py b/python/damask/util.py
index 3722fe33f..56143cc5e 100644
--- a/python/damask/util.py
+++ b/python/damask/util.py
@@ -9,6 +9,7 @@ from functools import reduce
from optparse import Option
import numpy as np
+import h5py
from . import version
@@ -27,7 +28,8 @@ __all__=[
'extendableOption',
'execution_stamp',
'shapeshifter', 'shapeblender',
- 'extend_docstring', 'extended_docstring'
+ 'extend_docstring', 'extended_docstring',
+ 'DREAM3D_base_group', 'DREAM3D_cell_data_group'
]
####################################################################################################
@@ -376,6 +378,53 @@ def extended_docstring(f,extra_docstring):
return _decorator
+def DREAM3D_base_group(fname):
+ """
+ Determine the base group of a DREAM.3D file.
+
+ The base group is defined as the group (folder) that contains
+ a 'SPACING' dataset in a '_SIMPL_GEOMETRY' group.
+
+ Parameters
+ ----------
+ fname : str
+ Filename of the DREAM.3D (HDF5) file.
+
+ """
+ with h5py.File(fname,'r') as f:
+ base_group = f.visit(lambda path: path.rsplit('/',2)[0] if '_SIMPL_GEOMETRY/SPACING' in path else None)
+
+ if base_group is None:
+ raise ValueError(f'Could not determine base group in file {fname}.')
+
+ return base_group
+
+def DREAM3D_cell_data_group(fname):
+ """
+ Determine the cell data group of a DREAM.3D file.
+
+ The cell data group is defined as the group (folder) that contains
+ a dataset in the base group whose length matches the total number
+ of points as specified in '_SIMPL_GEOMETRY/DIMENSIONS'.
+
+ Parameters
+ ----------
+ fname : str
+ Filename of the DREAM.3D (HDF5) file.
+
+ """
+ base_group = DREAM3D_base_group(fname)
+ with h5py.File(fname,'r') as f:
+ cells = tuple(f[os.path.join(base_group,'_SIMPL_GEOMETRY','DIMENSIONS')][()][::-1])
+ cell_data_group = f[base_group].visititems(lambda path,obj: path.split('/')[0] \
+ if isinstance(obj,h5py._hl.dataset.Dataset) and np.shape(obj)[:-1] == cells \
+ else None)
+
+ if cell_data_group is None:
+ raise ValueError(f'Could not determine cell data group in file {fname}/{base_group}.')
+
+ return cell_data_group
+
####################################################################################################
# Classes
####################################################################################################
diff --git a/python/tests/reference/ConfigMaterial/2phase_irregularGrid.dream3d b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.dream3d
new file mode 120000
index 000000000..94f337206
--- /dev/null
+++ b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.dream3d
@@ -0,0 +1 @@
+../Grid/2phase_irregularGrid.dream3d
\ No newline at end of file
diff --git a/python/tests/reference/ConfigMaterial/2phase_irregularGrid.json b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.json
new file mode 120000
index 000000000..66071ae27
--- /dev/null
+++ b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.json
@@ -0,0 +1 @@
+../Grid/2phase_irregularGrid.json
\ No newline at end of file
diff --git a/python/tests/reference/ConfigMaterial/2phase_irregularGrid.xdmf b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.xdmf
new file mode 120000
index 000000000..3736e65db
--- /dev/null
+++ b/python/tests/reference/ConfigMaterial/2phase_irregularGrid.xdmf
@@ -0,0 +1 @@
+../Grid/2phase_irregularGrid.xdmf
\ No newline at end of file
diff --git a/python/tests/reference/ConfigMaterial/measured.dream3d b/python/tests/reference/ConfigMaterial/measured.dream3d
new file mode 120000
index 000000000..51ed3e080
--- /dev/null
+++ b/python/tests/reference/ConfigMaterial/measured.dream3d
@@ -0,0 +1 @@
+../Grid/measured.dream3d
\ No newline at end of file
diff --git a/python/tests/reference/ConfigMaterial/measured.material_yaml b/python/tests/reference/ConfigMaterial/measured.material_yaml
new file mode 100644
index 000000000..bc7e73968
--- /dev/null
+++ b/python/tests/reference/ConfigMaterial/measured.material_yaml
@@ -0,0 +1,66831 @@
+phase: {'1': t.b.d., '2': t.b.d.}
+
+homogenization:
+ direct: {N_constituents: 1}
+
+material:
+ - constituents:
+ - O: [0.5567207566708297, -0.13535259297790672, 0.018612347301180162, -0.8193871216915458]
+ phase: 1
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+ homogenization: direct
+ - constituents:
+ - O: [0.5679576379716631, 0.5911734235875267, 0.4846749663178027, 0.3050053798513867]
+ phase: 1
+ v: 1.0
+ homogenization: direct
+ - constituents:
+ - O: [0.568130957548908, 0.5917703909810392, 0.4817404920345456, 0.308157618382254]
+ phase: 1
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+ - constituents:
+ - O: [0.6309112583743439, -0.7461527187815757, 0.2020468097335775, -0.06621322366301328]
+ phase: 1
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+ homogenization: direct
+ - constituents:
+ - O: [0.25299105247701736, 0.37817041427803905, 0.8835807136044798, 0.11076004549270393]
+ phase: 1
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+ homogenization: direct
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+ phase: 1
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+ phase: 1
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+ - O: [0.8811663152521274, 0.10967007128648089, -0.2437605342610061, -0.3899989772624993]
+ phase: 1
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+ phase: 1
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+ phase: 1
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+ phase: 1
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+ phase: 1
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+ phase: 1
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BQAAAACAAABoegAAHBcAAJEWAAA1FwAAsRYAAEsVAAA=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diff --git a/python/tests/reference/Grid/measured.xdmf b/python/tests/reference/Grid/measured.xdmf
new file mode 100644
index 000000000..79929e7ae
--- /dev/null
+++ b/python/tests/reference/Grid/measured.xdmf
@@ -0,0 +1,77 @@
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+ 0 35 -294.7
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+ 0.35 0.35 0.35
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+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Confidence Index
+
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+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/EulerAngles
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/FeatureIds
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Fit
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/IPFColor
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Image Quality
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Mask
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/ParentIds
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Phases
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/SEM Signal
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/X Position
+
+
+
+
+ measured.dream3d:/DataContainers/Small IN100/EBSD Scan Data/Y Position
+
+
+
+
+
+
diff --git a/python/tests/reference/Result/12grains6x7x8_tensionY.hdf5 b/python/tests/reference/Result/12grains6x7x8_tensionY.hdf5
index 3419e3b30..9fa9006ad 100644
Binary files a/python/tests/reference/Result/12grains6x7x8_tensionY.hdf5 and b/python/tests/reference/Result/12grains6x7x8_tensionY.hdf5 differ
diff --git a/python/tests/reference/Result/6grains6x7x8_single_phase_tensionY.hdf5 b/python/tests/reference/Result/6grains6x7x8_single_phase_tensionY.hdf5
index 10730af62..44410447b 100644
Binary files a/python/tests/reference/Result/6grains6x7x8_single_phase_tensionY.hdf5 and b/python/tests/reference/Result/6grains6x7x8_single_phase_tensionY.hdf5 differ
diff --git a/python/tests/test_ConfigMaterial.py b/python/tests/test_ConfigMaterial.py
index 5eb9a6c85..5ac0e546a 100644
--- a/python/tests/test_ConfigMaterial.py
+++ b/python/tests/test_ConfigMaterial.py
@@ -1,11 +1,11 @@
import os
-
import pytest
import numpy as np
from damask import ConfigMaterial
from damask import Table
from damask import Rotation
+from damask import Grid
@pytest.fixture
def ref_path(ref_path_base):
@@ -108,3 +108,35 @@ class TestConfigMaterial:
m = ConfigMaterial().material_add(**kw)
assert len(m['material']) == N
assert len(m['material'][0]['constituents']) == n
+
+
+ @pytest.mark.parametrize('cell_ensemble_data',[None,'CellEnsembleData'])
+ def test_load_DREAM3D(self,ref_path,cell_ensemble_data):
+ grain_c = ConfigMaterial.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d','Grain Data',
+ cell_ensemble_data = cell_ensemble_data)
+ point_c = ConfigMaterial.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d',
+ cell_ensemble_data = cell_ensemble_data)
+
+ assert point_c.is_valid and grain_c.is_valid and \
+ len(point_c['material'])+1 == len(grain_c['material'])
+
+ grain_m = Grid.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d','FeatureIds').material.flatten()
+ point_m = Grid.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d').material.flatten()
+
+ for i in np.unique(point_m):
+ j = int(grain_m[(point_m==i).nonzero()[0][0]])
+ assert np.allclose(point_c['material'][i]['constituents'][0]['O'],
+ grain_c['material'][j]['constituents'][0]['O'])
+ assert point_c['material'][i]['constituents'][0]['phase'] == \
+ grain_c['material'][j]['constituents'][0]['phase']
+
+
+ def test_load_DREAM3D_reference(self,tmp_path,ref_path,update):
+ cur = ConfigMaterial.load_DREAM3D(ref_path/'measured.dream3d')
+ ref = ConfigMaterial.load(ref_path/'measured.material_yaml')
+ if update:
+ cur.save(ref_path/'measured.material_yaml')
+ for i,m in enumerate(ref['material']):
+ assert Rotation(m['constituents'][0]['O']) == \
+ Rotation(cur['material'][i]['constituents'][0]['O'])
+ assert cur.is_valid and cur['phase'] == ref['phase'] and cur['homogenization'] == ref['homogenization']
diff --git a/python/tests/test_Grid.py b/python/tests/test_Grid.py
index a239165db..7e94686ee 100644
--- a/python/tests/test_Grid.py
+++ b/python/tests/test_Grid.py
@@ -420,12 +420,31 @@ class TestGrid:
t = Table(np.column_stack((coords.reshape(-1,3,order='F'),grid.material.flatten(order='F'))),{'c':3,'m':1})
assert grid_equal(grid.sort().renumber(),Grid.from_table(t,'c',['m']))
+
@pytest.mark.parametrize('periodic',[True,False])
@pytest.mark.parametrize('direction',['x','y','z',['x','y'],'zy','xz',['x','y','z']])
def test_get_grain_boundaries(self,update,ref_path,periodic,direction):
- grid=Grid.load(ref_path/'get_grain_boundaries_8g12x15x20.vtr')
- current=grid.get_grain_boundaries(periodic,direction)
+ grid = Grid.load(ref_path/'get_grain_boundaries_8g12x15x20.vtr')
+ current = grid.get_grain_boundaries(periodic,direction)
if update:
current.save(ref_path/f'get_grain_boundaries_8g12x15x20_{direction}_{periodic}.vtu',parallel=False)
- reference=VTK.load(ref_path/f'get_grain_boundaries_8g12x15x20_{"".join(direction)}_{periodic}.vtu')
+ reference = VTK.load(ref_path/f'get_grain_boundaries_8g12x15x20_{"".join(direction)}_{periodic}.vtu')
assert current.__repr__() == reference.__repr__()
+
+
+ def test_load_DREAM3D(self,ref_path):
+ grain = Grid.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d','FeatureIds')
+ point = Grid.load_DREAM3D(ref_path/'2phase_irregularGrid.dream3d')
+
+ assert np.allclose(grain.origin,point.origin) and \
+ np.allclose(grain.size,point.size) and \
+ (grain.sort().material == point.material+1).all()
+
+
+ def test_load_DREAM3D_reference(self,ref_path,update):
+ current = Grid.load_DREAM3D(ref_path/'measured.dream3d')
+ reference = Grid.load(ref_path/'measured')
+ if update:
+ current.save(ref_path/'measured.vtr')
+
+ assert grid_equal(current,reference)
diff --git a/python/tests/test_util.py b/python/tests/test_util.py
index 397926682..93044b31d 100644
--- a/python/tests/test_util.py
+++ b/python/tests/test_util.py
@@ -1,6 +1,10 @@
+import random
+import os
+
import pytest
import numpy as np
from scipy import stats
+import h5py
from damask import util
@@ -102,3 +106,36 @@ class TestUtil:
@pytest.mark.parametrize('style',[util.emph,util.deemph,util.warn,util.strikeout])
def test_decorate(self,style):
assert 'DAMASK' in style('DAMASK')
+
+ @pytest.mark.parametrize('complete',[True,False])
+ def test_D3D_base_group(self,tmp_path,complete):
+ base_group = ''.join(random.choices('DAMASK', k=10))
+ with h5py.File(tmp_path/'base_group.dream3d','w') as f:
+ f.create_group(os.path.join(base_group,'_SIMPL_GEOMETRY'))
+ if complete:
+ f[os.path.join(base_group,'_SIMPL_GEOMETRY')].create_dataset('SPACING',data=np.ones(3))
+
+ if complete:
+ assert base_group == util.DREAM3D_base_group(tmp_path/'base_group.dream3d')
+ else:
+ with pytest.raises(ValueError):
+ util.DREAM3D_base_group(tmp_path/'base_group.dream3d')
+
+ @pytest.mark.parametrize('complete',[True,False])
+ def test_D3D_cell_data_group(self,tmp_path,complete):
+ base_group = ''.join(random.choices('DAMASK', k=10))
+ cell_data_group = ''.join(random.choices('KULeuven', k=10))
+ cells = np.random.randint(1,50,3)
+ with h5py.File(tmp_path/'cell_data_group.dream3d','w') as f:
+ f.create_group(os.path.join(base_group,'_SIMPL_GEOMETRY'))
+ f[os.path.join(base_group,'_SIMPL_GEOMETRY')].create_dataset('SPACING',data=np.ones(3))
+ f[os.path.join(base_group,'_SIMPL_GEOMETRY')].create_dataset('DIMENSIONS',data=cells[::-1])
+ f[base_group].create_group(cell_data_group)
+ if complete:
+ f[os.path.join(base_group,cell_data_group)].create_dataset('data',shape=np.append(cells,1))
+
+ if complete:
+ assert cell_data_group == util.DREAM3D_cell_data_group(tmp_path/'cell_data_group.dream3d')
+ else:
+ with pytest.raises(ValueError):
+ util.DREAM3D_cell_data_group(tmp_path/'cell_data_group.dream3d')
diff --git a/src/DAMASK_interface.f90 b/src/DAMASK_interface.f90
index ab64dcf01..b7cb1d80f 100644
--- a/src/DAMASK_interface.f90
+++ b/src/DAMASK_interface.f90
@@ -93,7 +93,7 @@ subroutine DAMASK_interface_init
#endif
print*, achar(27)//'[0m'
- print*, 'Roters et al., Computational Materials Science 158:420–478, 2019'
+ print*, 'F. Roters et al., Computational Materials Science 158:420–478, 2019'
print*, 'https://doi.org/10.1016/j.commatsci.2018.04.030'
print'(/,a)', ' Version: '//DAMASKVERSION
diff --git a/src/grid/DAMASK_grid.f90 b/src/grid/DAMASK_grid.f90
index 32b43308d..abf86e161 100644
--- a/src/grid/DAMASK_grid.f90
+++ b/src/grid/DAMASK_grid.f90
@@ -117,7 +117,7 @@ program DAMASK_grid
call CPFEM_initAll
print'(/,a)', ' <<<+- DAMASK_grid init -+>>>'; flush(IO_STDOUT)
- print*, 'Shanthraj et al., Handbook of Mechanics of Materials, 2019'
+ print*, 'P. Shanthraj et al., Handbook of Mechanics of Materials, 2019'
print*, 'https://doi.org/10.1007/978-981-10-6855-3_80'
diff --git a/src/grid/grid_damage_spectral.f90 b/src/grid/grid_damage_spectral.f90
index 8d3f913fa..6f99365f7 100644
--- a/src/grid/grid_damage_spectral.f90
+++ b/src/grid/grid_damage_spectral.f90
@@ -75,7 +75,7 @@ subroutine grid_damage_spectral_init
print'(/,a)', ' <<<+- grid_spectral_damage init -+>>>'
- print*, 'Shanthraj et al., Handbook of Mechanics of Materials, 2019'
+ print*, 'P. Shanthraj et al., Handbook of Mechanics of Materials, 2019'
print*, 'https://doi.org/10.1007/978-981-10-6855-3_80'
!-------------------------------------------------------------------------------------------------
diff --git a/src/grid/grid_mech_spectral_basic.f90 b/src/grid/grid_mech_spectral_basic.f90
index faf58c85e..e7690eb55 100644
--- a/src/grid/grid_mech_spectral_basic.f90
+++ b/src/grid/grid_mech_spectral_basic.f90
@@ -105,10 +105,10 @@ subroutine grid_mechanical_spectral_basic_init
print'(/,a)', ' <<<+- grid_mechanical_spectral_basic init -+>>>'; flush(IO_STDOUT)
- print*, 'Eisenlohr et al., International Journal of Plasticity 46:37–53, 2013'
+ print*, 'P. Eisenlohr et al., International Journal of Plasticity 46:37–53, 2013'
print*, 'https://doi.org/10.1016/j.ijplas.2012.09.012'//IO_EOL
- print*, 'Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
+ print*, 'P. Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
print*, 'https://doi.org/10.1016/j.ijplas.2014.02.006'
!-------------------------------------------------------------------------------------------------
diff --git a/src/grid/grid_mech_spectral_polarisation.f90 b/src/grid/grid_mech_spectral_polarisation.f90
index 31f69b4c5..478df7fdf 100644
--- a/src/grid/grid_mech_spectral_polarisation.f90
+++ b/src/grid/grid_mech_spectral_polarisation.f90
@@ -118,7 +118,7 @@ subroutine grid_mechanical_spectral_polarisation_init
print'(/,a)', ' <<<+- grid_mechanical_spectral_polarization init -+>>>'; flush(IO_STDOUT)
- print*, 'Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
+ print*, 'P. Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
print*, 'https://doi.org/10.1016/j.ijplas.2014.02.006'
!-------------------------------------------------------------------------------------------------
diff --git a/src/grid/grid_thermal_spectral.f90 b/src/grid/grid_thermal_spectral.f90
index 5ac043a67..dd431ad9b 100644
--- a/src/grid/grid_thermal_spectral.f90
+++ b/src/grid/grid_thermal_spectral.f90
@@ -75,7 +75,7 @@ subroutine grid_thermal_spectral_init(T_0)
print'(/,a)', ' <<<+- grid_thermal_spectral init -+>>>'
- print*, 'Shanthraj et al., Handbook of Mechanics of Materials, 2019'
+ print*, 'P. Shanthraj et al., Handbook of Mechanics of Materials, 2019'
print*, 'https://doi.org/10.1007/978-981-10-6855-3_80'
!-------------------------------------------------------------------------------------------------
diff --git a/src/grid/spectral_utilities.f90 b/src/grid/spectral_utilities.f90
index e8bae223a..97801cfb3 100644
--- a/src/grid/spectral_utilities.f90
+++ b/src/grid/spectral_utilities.f90
@@ -176,16 +176,16 @@ subroutine spectral_utilities_init
print'(/,a)', ' <<<+- spectral_utilities init -+>>>'
- print*, 'Diehl, Diploma Thesis TU München, 2010'
+ print*, 'M. Diehl, Diploma Thesis TU München, 2010'
print*, 'https://doi.org/10.13140/2.1.3234.3840'//IO_EOL
- print*, 'Eisenlohr et al., International Journal of Plasticity 46:37–53, 2013'
+ print*, 'P. Eisenlohr et al., International Journal of Plasticity 46:37–53, 2013'
print*, 'https://doi.org/10.1016/j.ijplas.2012.09.012'//IO_EOL
- print*, 'Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
+ print*, 'P. Shanthraj et al., International Journal of Plasticity 66:31–45, 2015'
print*, 'https://doi.org/10.1016/j.ijplas.2014.02.006'//IO_EOL
- print*, 'Shanthraj et al., Handbook of Mechanics of Materials, 2019'
+ print*, 'P. Shanthraj et al., Handbook of Mechanics of Materials, 2019'
print*, 'https://doi.org/10.1007/978-981-10-6855-3_80'
!--------------------------------------------------------------------------------------------------
diff --git a/src/homogenization.f90 b/src/homogenization.f90
index 6cbdac2a5..7dfaf5b37 100644
--- a/src/homogenization.f90
+++ b/src/homogenization.f90
@@ -276,8 +276,8 @@ subroutine materialpoint_stressAndItsTangent(dt,FEsolving_execIP,FEsolving_execE
call phase_restore(ce,.false.) ! wrong name (is more a forward function)
- if(homogState(ho)%sizeState > 0) homogState(ho)%State(:,me) = homogState(ho)%State0(:,me)
- if(damageState_h(ho)%sizeState > 0) damageState_h(ho)%State(:,me) = damageState_h(ho)%State0(:,me)
+ if(homogState(ho)%sizeState > 0) homogState(ho)%state(:,me) = homogState(ho)%state0(:,me)
+ if(damageState_h(ho)%sizeState > 0) damageState_h(ho)%state(:,me) = damageState_h(ho)%state0(:,me)
call damage_partition(ce)
doneAndHappy = [.false.,.true.]
@@ -287,20 +287,17 @@ subroutine materialpoint_stressAndItsTangent(dt,FEsolving_execIP,FEsolving_execE
.and. NiterationMPstate < num%nMPstate)
NiterationMPstate = NiterationMPstate + 1
+ call mechanical_partition(homogenization_F(1:3,1:3,ce),ce)
+ converged = .true.
+ do co = 1, myNgrains
+ converged = converged .and. crystallite_stress(dt,co,ip,el)
+ enddo
- if (.not. doneAndHappy(1)) then
- call mechanical_partition(homogenization_F(1:3,1:3,ce),ce)
- converged = .true.
- do co = 1, myNgrains
- converged = converged .and. crystallite_stress(dt,co,ip,el)
- enddo
-
- if (.not. converged) then
- doneAndHappy = [.true.,.false.]
- else
- doneAndHappy = mechanical_updateState(dt,homogenization_F(1:3,1:3,ce),ce)
- converged = all(doneAndHappy)
- endif
+ if (converged) then
+ doneAndHappy = mechanical_updateState(dt,homogenization_F(1:3,1:3,ce),ce)
+ converged = all(doneAndHappy)
+ else
+ doneAndHappy = [.true.,.false.]
endif
enddo convergenceLooping
@@ -450,7 +447,7 @@ subroutine homogenization_restartRead(fileHandle)
groupHandle(2) = HDF5_openGroup(groupHandle(1),material_name_homogenization(ho))
- call HDF5_read(groupHandle(2),homogState(ho)%state,'omega') ! ToDo: should be done by mech
+ call HDF5_read(groupHandle(2),homogState(ho)%state0,'omega') ! ToDo: should be done by mech
call HDF5_closeGroup(groupHandle(2))
diff --git a/src/homogenization_mechanical_RGC.f90 b/src/homogenization_mechanical_RGC.f90
index 29e05f981..b35c41d62 100644
--- a/src/homogenization_mechanical_RGC.f90
+++ b/src/homogenization_mechanical_RGC.f90
@@ -91,12 +91,11 @@ module subroutine mechanical_RGC_init(num_homogMech)
print'(a,i2)', ' # instances: ',count(homogenization_type == HOMOGENIZATION_RGC_ID); flush(IO_STDOUT)
- print*, 'Tjahjanto et al., International Journal of Material Forming 2(1):939–942, 2009'
+ print*, 'D.D. Tjahjanto et al., International Journal of Material Forming 2(1):939–942, 2009'
print*, 'https://doi.org/10.1007/s12289-009-0619-1'//IO_EOL
- print*, 'Tjahjanto et al., Modelling and Simulation in Materials Science and Engineering 18:015006, 2010'
- print*, 'https://doi.org/10.1088/0965-0393/18/1/015006'//IO_EOL
-
+ print*, 'D.D. Tjahjanto et al., Modelling and Simulation in Materials Science and Engineering 18:015006, 2010'
+ print*, 'https://doi.org/10.1088/0965-0393/18/1/015006'//IO_EOL
material_homogenization => config_material%get('homogenization')
diff --git a/src/phase_mechanical.f90 b/src/phase_mechanical.f90
index 7d8f6e463..d461ab9db 100644
--- a/src/phase_mechanical.f90
+++ b/src/phase_mechanical.f90
@@ -492,7 +492,7 @@ function integrateStress(F,subFp0,subFi0,Delta_t,co,ip,el) result(broken)
cycle LpLoop
endif
- calculateJacobiLi: if (mod(jacoCounterLp, num%iJacoLpresiduum) == 0) then
+ calculateJacobiLp: if (mod(jacoCounterLp, num%iJacoLpresiduum) == 0) then
jacoCounterLp = jacoCounterLp + 1
do o=1,3; do p=1,3
@@ -504,7 +504,7 @@ function integrateStress(F,subFp0,subFi0,Delta_t,co,ip,el) result(broken)
call dgesv(9,1,dRLp_dLp,9,devNull_9,temp_9,9,ierr) ! solve dRLp/dLp * delta Lp = -res for delta Lp
if (ierr /= 0) return ! error
deltaLp = - math_9to33(temp_9)
- endif calculateJacobiLi
+ endif calculateJacobiLp
Lpguess = Lpguess &
+ deltaLp * steplengthLp
@@ -532,7 +532,7 @@ function integrateStress(F,subFp0,subFi0,Delta_t,co,ip,el) result(broken)
cycle LiLoop
endif
- calculateJacobiLp: if (mod(jacoCounterLi, num%iJacoLpresiduum) == 0) then
+ calculateJacobiLi: if (mod(jacoCounterLi, num%iJacoLpresiduum) == 0) then
jacoCounterLi = jacoCounterLi + 1
temp_33 = matmul(matmul(A,B),invFi_current)
@@ -551,7 +551,7 @@ function integrateStress(F,subFp0,subFi0,Delta_t,co,ip,el) result(broken)
call dgesv(9,1,dRLi_dLi,9,devNull_9,temp_9,9,ierr) ! solve dRLi/dLp * delta Li = -res for delta Li
if (ierr /= 0) return ! error
deltaLi = - math_9to33(temp_9)
- endif calculateJacobiLp
+ endif calculateJacobiLi
Liguess = Liguess &
+ deltaLi * steplengthLi
diff --git a/src/phase_mechanical_plastic_dislotungsten.f90 b/src/phase_mechanical_plastic_dislotungsten.f90
index 614b44d54..86d965ecc 100644
--- a/src/phase_mechanical_plastic_dislotungsten.f90
+++ b/src/phase_mechanical_plastic_dislotungsten.f90
@@ -103,8 +103,8 @@ module function plastic_dislotungsten_init() result(myPlasticity)
print'(/,a)', ' <<<+- phase:mechanical:plastic:dislotungsten init -+>>>'
print'(a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
- print*, 'Cereceda et al., International Journal of Plasticity 78:242–256, 2016'
- print*, 'https://dx.doi.org/10.1016/j.ijplas.2015.09.002'
+ print*, 'D. Cereceda et al., International Journal of Plasticity 78:242–256, 2016'
+ print*, 'https://doi.org/10.1016/j.ijplas.2015.09.002'
phases => config_material%get('phase')
diff --git a/src/phase_mechanical_plastic_dislotwin.f90 b/src/phase_mechanical_plastic_dislotwin.f90
index 2fce4d129..a897011f6 100644
--- a/src/phase_mechanical_plastic_dislotwin.f90
+++ b/src/phase_mechanical_plastic_dislotwin.f90
@@ -150,13 +150,13 @@ module function plastic_dislotwin_init() result(myPlasticity)
print'(/,a)', ' <<<+- phase:mechanical:plastic:dislotwin init -+>>>'
print'(a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
- print*, 'Ma and Roters, Acta Materialia 52(12):3603–3612, 2004'
+ print*, 'A. Ma and F. Roters, Acta Materialia 52(12):3603–3612, 2004'
print*, 'https://doi.org/10.1016/j.actamat.2004.04.012'//IO_EOL
- print*, 'Roters et al., Computational Materials Science 39:91–95, 2007'
+ print*, 'F. Roters et al., Computational Materials Science 39:91–95, 2007'
print*, 'https://doi.org/10.1016/j.commatsci.2006.04.014'//IO_EOL
- print*, 'Wong et al., Acta Materialia 118:140–151, 2016'
+ print*, 'S.L. Wong et al., Acta Materialia 118:140–151, 2016'
print*, 'https://doi.org/10.1016/j.actamat.2016.07.032'
diff --git a/src/phase_mechanical_plastic_isotropic.f90 b/src/phase_mechanical_plastic_isotropic.f90
index f31101e6f..206944304 100644
--- a/src/phase_mechanical_plastic_isotropic.f90
+++ b/src/phase_mechanical_plastic_isotropic.f90
@@ -71,7 +71,7 @@ module function plastic_isotropic_init() result(myPlasticity)
print'(/,a)', ' <<<+- phase:mechanical:plastic:isotropic init -+>>>'
print'(a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
- print*, 'Maiti and Eisenlohr, Scripta Materialia 145:37–40, 2018'
+ print*, 'T. Maiti and P. Eisenlohr, Scripta Materialia 145:37–40, 2018'
print*, 'https://doi.org/10.1016/j.scriptamat.2017.09.047'
phases => config_material%get('phase')
diff --git a/src/phase_mechanical_plastic_nonlocal.f90 b/src/phase_mechanical_plastic_nonlocal.f90
index a05053c6d..654cf08a3 100644
--- a/src/phase_mechanical_plastic_nonlocal.f90
+++ b/src/phase_mechanical_plastic_nonlocal.f90
@@ -203,10 +203,10 @@ module function plastic_nonlocal_init() result(myPlasticity)
print'(/,a)', ' <<<+- phase:mechanical:plastic:nonlocal init -+>>>'
print'(a,i0)', ' # phases: ',Ninstances; flush(IO_STDOUT)
- print*, 'Reuber et al., Acta Materialia 71:333–348, 2014'
+ print*, 'C. Reuber et al., Acta Materialia 71:333–348, 2014'
print*, 'https://doi.org/10.1016/j.actamat.2014.03.012'//IO_EOL
- print*, 'Kords, Dissertation RWTH Aachen, 2014'
+ print*, 'C. Kords, Dissertation RWTH Aachen, 2014'
print*, 'http://publications.rwth-aachen.de/record/229993'
diff --git a/src/results.f90 b/src/results.f90
index 4fec6694e..90727b9c3 100644
--- a/src/results.f90
+++ b/src/results.f90
@@ -61,7 +61,7 @@ subroutine results_init(restart)
print'(/,a)', ' <<<+- results init -+>>>'; flush(IO_STDOUT)
- print*, 'Diehl et al., Integrating Materials and Manufacturing Innovation 6(1):83–91, 2017'
+ print*, 'M. Diehl et al., Integrating Materials and Manufacturing Innovation 6(1):83–91, 2017'
print*, 'https://doi.org/10.1007/s40192-017-0084-5'//IO_EOL
if(.not. restart) then
@@ -71,7 +71,8 @@ subroutine results_init(restart)
call results_addAttribute('DAMASK_version',DAMASKVERSION)
call get_command(commandLine)
call results_addAttribute('call',trim(commandLine))
- call results_closeGroup(results_addGroup('mapping'))
+ call results_closeGroup(results_addGroup('cell_to'))
+ call results_addAttribute('description','mappings to place data in space','cell_to')
call results_closeJobFile
endif
@@ -431,8 +432,8 @@ subroutine results_mapping_phase(phaseAt,memberAtLocal,label)
integer(HID_T) :: &
loc_id, & !< identifier of group in file
dtype_id, & !< identifier of compound data type
- name_id, & !< identifier of name (string) in compound data type
- position_id, & !< identifier of position/index (integer) in compound data type
+ label_id, & !< identifier of label (string) in compound data type
+ entry_id, & !< identifier of entry (integer) in compound data type
dset_id, &
memspace_id, &
filespace_id, &
@@ -497,21 +498,21 @@ subroutine results_mapping_phase(phaseAt,memberAtLocal,label)
call h5tcreate_f(H5T_COMPOUND_F, type_size_string + type_size_int, dtype_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(dtype_id, 'name', 0_SIZE_T, dt_id,hdferr)
+ call h5tinsert_f(dtype_id, 'label', 0_SIZE_T, dt_id,hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(dtype_id, 'member', type_size_string, H5T_NATIVE_INTEGER, hdferr)
+ call h5tinsert_f(dtype_id, 'entry', type_size_string, H5T_NATIVE_INTEGER, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
!--------------------------------------------------------------------------------------------------
! create memory types for each component of the compound type
- call h5tcreate_f(H5T_COMPOUND_F, type_size_string, name_id, hdferr)
+ call h5tcreate_f(H5T_COMPOUND_F, type_size_string, label_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(name_id, 'name', 0_SIZE_T, dt_id, hdferr)
+ call h5tinsert_f(label_id, 'label', 0_SIZE_T, dt_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tcreate_f(H5T_COMPOUND_F, type_size_int, position_id, hdferr)
+ call h5tcreate_f(H5T_COMPOUND_F, type_size_int, entry_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(position_id, 'member', 0_SIZE_T, H5T_NATIVE_INTEGER, hdferr)
+ call h5tinsert_f(entry_id, 'entry', 0_SIZE_T, H5T_NATIVE_INTEGER, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
call h5tclose_f(dt_id, hdferr)
@@ -533,14 +534,14 @@ subroutine results_mapping_phase(phaseAt,memberAtLocal,label)
call h5pset_preserve_f(plist_id, .true., hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- loc_id = results_openGroup('/mapping')
+ loc_id = results_openGroup('/cell_to')
call h5dcreate_f(loc_id, 'phase', dtype_id, filespace_id, dset_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5dwrite_f(dset_id, name_id, reshape(label(pack(phaseAtMaterialpoint,.true.)),myShape), &
+ call h5dwrite_f(dset_id, label_id, reshape(label(pack(phaseAtMaterialpoint,.true.)),myShape), &
myShape, hdferr, file_space_id = filespace_id, mem_space_id = memspace_id, xfer_prp = plist_id)
if(hdferr < 0) error stop 'HDF5 error'
- call h5dwrite_f(dset_id, position_id, reshape(pack(memberAtGlobal,.true.),myShape), &
+ call h5dwrite_f(dset_id, entry_id, reshape(pack(memberAtGlobal,.true.),myShape), &
myShape, hdferr, file_space_id = filespace_id, mem_space_id = memspace_id, xfer_prp = plist_id)
if(hdferr < 0) error stop 'HDF5 error'
@@ -557,9 +558,11 @@ subroutine results_mapping_phase(phaseAt,memberAtLocal,label)
if(hdferr < 0) error stop 'HDF5 error'
call h5tclose_f(dtype_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tclose_f(name_id, hdferr)
+ call h5tclose_f(label_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tclose_f(position_id, hdferr)
+ call h5tclose_f(entry_id, hdferr)
+
+ call executionStamp('cell_to/phase','cell ID and constituent ID to phase results')
end subroutine results_mapping_phase
@@ -586,8 +589,8 @@ subroutine results_mapping_homogenization(homogenizationAt,memberAtLocal,label)
integer(HID_T) :: &
loc_id, & !< identifier of group in file
dtype_id, & !< identifier of compound data type
- name_id, & !< identifier of name (string) in compound data type
- position_id, & !< identifier of position/index (integer) in compound data type
+ label_id, & !< identifier of label (string) in compound data type
+ entry_id, & !< identifier of entry (integer) in compound data type
dset_id, &
memspace_id, &
filespace_id, &
@@ -653,21 +656,21 @@ subroutine results_mapping_homogenization(homogenizationAt,memberAtLocal,label)
call h5tcreate_f(H5T_COMPOUND_F, type_size_string + type_size_int, dtype_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(dtype_id, 'name', 0_SIZE_T, dt_id,hdferr)
+ call h5tinsert_f(dtype_id, 'label', 0_SIZE_T, dt_id,hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(dtype_id, 'member', type_size_string, H5T_NATIVE_INTEGER, hdferr)
+ call h5tinsert_f(dtype_id, 'entry', type_size_string, H5T_NATIVE_INTEGER, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
!--------------------------------------------------------------------------------------------------
! create memory types for each component of the compound type
- call h5tcreate_f(H5T_COMPOUND_F, type_size_string, name_id, hdferr)
+ call h5tcreate_f(H5T_COMPOUND_F, type_size_string, label_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(name_id, 'name', 0_SIZE_T, dt_id, hdferr)
+ call h5tinsert_f(label_id, 'label', 0_SIZE_T, dt_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tcreate_f(H5T_COMPOUND_F, type_size_int, position_id, hdferr)
+ call h5tcreate_f(H5T_COMPOUND_F, type_size_int, entry_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tinsert_f(position_id, 'member', 0_SIZE_T, H5T_NATIVE_INTEGER, hdferr)
+ call h5tinsert_f(entry_id, 'entry', 0_SIZE_T, H5T_NATIVE_INTEGER, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
call h5tclose_f(dt_id, hdferr)
@@ -689,14 +692,14 @@ subroutine results_mapping_homogenization(homogenizationAt,memberAtLocal,label)
call h5pset_preserve_f(plist_id, .true., hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- loc_id = results_openGroup('/mapping')
+ loc_id = results_openGroup('/cell_to')
call h5dcreate_f(loc_id, 'homogenization', dtype_id, filespace_id, dset_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5dwrite_f(dset_id, name_id, reshape(label(pack(homogenizationAtMaterialpoint,.true.)),myShape), &
+ call h5dwrite_f(dset_id, label_id, reshape(label(pack(homogenizationAtMaterialpoint,.true.)),myShape), &
myShape, hdferr, file_space_id = filespace_id, mem_space_id = memspace_id, xfer_prp = plist_id)
if(hdferr < 0) error stop 'HDF5 error'
- call h5dwrite_f(dset_id, position_id, reshape(pack(memberAtGlobal,.true.),myShape), &
+ call h5dwrite_f(dset_id, entry_id, reshape(pack(memberAtGlobal,.true.),myShape), &
myShape, hdferr, file_space_id = filespace_id, mem_space_id = memspace_id, xfer_prp = plist_id)
if(hdferr < 0) error stop 'HDF5 error'
@@ -713,11 +716,13 @@ subroutine results_mapping_homogenization(homogenizationAt,memberAtLocal,label)
if(hdferr < 0) error stop 'HDF5 error'
call h5tclose_f(dtype_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tclose_f(name_id, hdferr)
+ call h5tclose_f(label_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
- call h5tclose_f(position_id, hdferr)
+ call h5tclose_f(entry_id, hdferr)
if(hdferr < 0) error stop 'HDF5 error'
+ call executionStamp('cell_to/homogenization','cell ID to homogenization results')
+
end subroutine results_mapping_homogenization
diff --git a/src/rotations.f90 b/src/rotations.f90
index 57dd16b53..171db2466 100644
--- a/src/rotations.f90
+++ b/src/rotations.f90
@@ -105,7 +105,7 @@ subroutine rotations_init
print'(/,a)', ' <<<+- rotations init -+>>>'; flush(IO_STDOUT)
- print*, 'Rowenhorst et al., Modelling and Simulation in Materials Science and Engineering 23:083501, 2015'
+ print*, 'D. Rowenhorst et al., Modelling and Simulation in Materials Science and Engineering 23:083501, 2015'
print*, 'https://doi.org/10.1088/0965-0393/23/8/083501'
call selfTest