Merge branch 'development' into 3-adding-plastic-constitutive-law-with-kinematic-hardening
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566cf3d855
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[Air]
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## Isotropic Material model to simulate free surfaces ##
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## For more information see paper Maiti+Eisenlohr2018, Scripta Materialia,
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## "Fourier-based spectral method solution to finite strain crystal plasticity with free surfaces"
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elasticity hooke
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plasticity isotropic
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/dilatation/
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(output) flowstress
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(output) strainrate
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lattice_structure isotropic
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c11 110.9e9
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c12 0.0
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taylorfactor 3
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tau0 31e6
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gdot0 0.001
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n 20
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h0 75e6
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tausat 63e6
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w0 2.25
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atol_resistance 1
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@ -22,7 +22,13 @@ parser.add_option('-t','--tensor',
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dest = 'tensor',
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action = 'extend', metavar = '<string LIST>',
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help = 'heading of columns containing tensor field values')
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parser.add_option('--no-check',
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dest = 'rh',
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action = 'store_false',
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help = 'skip check for right-handed eigenvector basis')
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parser.set_defaults(rh = True,
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)
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(options,filenames) = parser.parse_args()
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if options.tensor is None:
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@ -57,8 +63,10 @@ for name in filenames:
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if dim != data['dim']: remarks.append('column {} is not a {}...'.format(what,type))
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else:
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items[type]['column'].append(table.label_index(what))
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table.labels_append(['{}_eigval({})'.format(i+1,what) for i in range(3)]) # extend ASCII header with new labels
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table.labels_append(['{}_eigvec({})'.format(i+1,what) for i in range(9)]) # extend ASCII header with new labels
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for order in ['Min','Mid','Max']:
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table.labels_append(['eigval{}({})'.format(order,what)]) # extend ASCII header with new labels
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for order in ['Min','Mid','Max']:
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table.labels_append(['{}_eigvec{}({})'.format(i+1,order,what) for i in range(3)]) # extend ASCII header with new labels
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if remarks != []: damask.util.croak(remarks)
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if errors != []:
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@ -78,10 +86,10 @@ for name in filenames:
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for type, data in items.iteritems():
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for column in data['column']:
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(u,v) = np.linalg.eigh(np.array(map(float,table.data[column:column+data['dim']])).reshape(data['shape']))
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if np.dot(np.cross(v[:,0], v[:,1]), v[:,2]) < 0.0 : v[:, 2] *= -1.0 # ensure right-handed coordinate system
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table.data_append(list(u))
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table.data_append(list(v.transpose().reshape(data['dim'])))
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outputAlive = table.data_write() # output processed line
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if options.rh and np.dot(np.cross(v[:,0], v[:,1]), v[:,2]) < 0.0 : v[:, 2] *= -1.0 # ensure right-handed eigenvector basis
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table.data_append(list(u)) # vector of max,mid,min eigval
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table.data_append(list(v.transpose().reshape(data['dim']))) # 3x3=9 combo vector of max,mid,min eigvec coordinates
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outputAlive = table.data_write() # output processed line in accordance with column labeling
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# ------------------------------------------ output finalization -----------------------------------
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@ -60,15 +60,18 @@ module plastic_isotropic
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flowstress, &
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accumulatedShear
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end type
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type, private :: tIsotropicAbsTol !< internal alias for abs tolerance in state
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real(pReal), pointer :: & ! scalars
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flowstress, &
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accumulatedShear
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end type
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type(tIsotropicState), allocatable, dimension(:), private :: & !< state aliases per instance
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state, &
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state0, &
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dotState
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type(tIsotropicAbsTol), allocatable, dimension(:), private :: & !< state aliases per instance
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stateAbsTol
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@ -140,7 +143,7 @@ subroutine plastic_isotropic_init(fileUnit)
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extmsg = ''
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character(len=64) :: &
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outputtag = ''
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integer(pInt) :: NipcMyPhase
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integer(pInt) :: NipcMyPhase
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write(6,'(/,a)') ' <<<+- constitutive_'//PLASTICITY_ISOTROPIC_label//' init -+>>>'
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write(6,'(a15,a)') ' Current time: ',IO_timeStamp()
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@ -293,9 +296,9 @@ subroutine plastic_isotropic_init(fileUnit)
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!--------------------------------------------------------------------------------------------------
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! allocate state arrays
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sizeState = 2_pInt ! flowstress, accumulated_shear
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sizeDotState = sizeState ! both evolve
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sizeDotState = 2_pInt ! flowstress, accumulated_shear
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sizeDeltaState = 0_pInt ! no sudden jumps in state
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sizeState = sizeDotState + sizeDeltaState
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plasticState(phase)%sizeState = sizeState
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plasticState(phase)%sizeDotState = sizeDotState
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plasticState(phase)%sizeDeltaState = sizeDeltaState
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