- elem_filteractiveThe type of elements to include in the count (active, total). Default == active
Default:active
C++ Type:MooseEnum
Unit:(no unit assumed)
Controllable:No
Description:The type of elements to include in the count (active, total). Default == active
- execute_onTIMESTEP_ENDThe list of flag(s) indicating when this object should be executed. For a description of each flag, see https://mooseframework.inl.gov/source/interfaces/SetupInterface.html.
Default:TIMESTEP_END
C++ Type:ExecFlagEnum
Unit:(no unit assumed)
Controllable:No
Description:The list of flag(s) indicating when this object should be executed. For a description of each flag, see https://mooseframework.inl.gov/source/interfaces/SetupInterface.html.
- prop_getter_suffixAn optional suffix parameter that can be appended to any attempt to retrieve/get material properties. The suffix will be prepended with a '_' character.
C++ Type:MaterialPropertyName
Unit:(no unit assumed)
Controllable:No
Description:An optional suffix parameter that can be appended to any attempt to retrieve/get material properties. The suffix will be prepended with a '_' character.
- use_interpolated_stateFalseFor the old and older state use projected material properties interpolated at the quadrature points. To set up projection use the ProjectedStatefulMaterialStorageAction.
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:For the old and older state use projected material properties interpolated at the quadrature points. To set up projection use the ProjectedStatefulMaterialStorageAction.
NumElements
Return the number of active or total elements in the simulation.
The NumElements
Postprocessor provides information about the number of elements in the simulation. This postprocessor is capable of providing either the active number of elements in the simulation (i.e. only the elements that are being used for calculations), or the total number of elements (i.e. includes parent elements of refined elements, which are maintained for the purpose of coarsening).
This postprocessor returns the aggregate number of elements when using DistributedMesh.
Input Parameters
- allow_duplicate_execution_on_initialFalseIn the case where this UserObject is depended upon by an initial condition, allow it to be executed twice during the initial setup (once before the IC and again after mesh adaptivity (if applicable).
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:In the case where this UserObject is depended upon by an initial condition, allow it to be executed twice during the initial setup (once before the IC and again after mesh adaptivity (if applicable).
- control_tagsAdds user-defined labels for accessing object parameters via control logic.
C++ Type:std::vector<std::string>
Unit:(no unit assumed)
Controllable:No
Description:Adds user-defined labels for accessing object parameters via control logic.
- enableTrueSet the enabled status of the MooseObject.
Default:True
C++ Type:bool
Unit:(no unit assumed)
Controllable:Yes
Description:Set the enabled status of the MooseObject.
- execution_order_group0Execution order groups are executed in increasing order (e.g., the lowest number is executed first). Note that negative group numbers may be used to execute groups before the default (0) group. Please refer to the user object documentation for ordering of user object execution within a group.
Default:0
C++ Type:int
Unit:(no unit assumed)
Controllable:No
Description:Execution order groups are executed in increasing order (e.g., the lowest number is executed first). Note that negative group numbers may be used to execute groups before the default (0) group. Please refer to the user object documentation for ordering of user object execution within a group.
- force_postauxFalseForces the UserObject to be executed in POSTAUX
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Forces the UserObject to be executed in POSTAUX
- force_preauxFalseForces the UserObject to be executed in PREAUX
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Forces the UserObject to be executed in PREAUX
- force_preicFalseForces the UserObject to be executed in PREIC during initial setup
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Forces the UserObject to be executed in PREIC during initial setup
- outputsVector of output names where you would like to restrict the output of variables(s) associated with this object
C++ Type:std::vector<OutputName>
Unit:(no unit assumed)
Controllable:No
Description:Vector of output names where you would like to restrict the output of variables(s) associated with this object
- use_displaced_meshFalseWhether or not this object should use the displaced mesh for computation. Note that in the case this is true but no displacements are provided in the Mesh block the undisplaced mesh will still be used.
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Whether or not this object should use the displaced mesh for computation. Note that in the case this is true but no displacements are provided in the Mesh block the undisplaced mesh will still be used.
Advanced Parameters
Input Files
- (test/tests/markers/reporter_point_marker/reporter_marker_adapt_test.i)
- (test/tests/postprocessors/num_residual_eval/num_residual_eval.i)
- (test/tests/postprocessors/difference_pps/difference_depend_check.i)
- (modules/phase_field/examples/ebsd_reconstruction/IN100-111grn.i)
- (modules/phase_field/test/tests/GBType/GB_Type_Phase1.i)
- (modules/phase_field/test/tests/grain_tracker_test/split_grain.i)
- (test/tests/outputs/hide_vector_pp/hide_vector_pp.i)
- (test/tests/mesh/splitting/geometric_neighbors.i)
- (test/tests/postprocessors/relative_difference/relative_difference.i)
- (test/tests/postprocessors/num_elems/num_elems.i)
- (modules/phase_field/test/tests/reconstruction/euler2rgb_non_uniform_orientation.i)
- (test/tests/outputs/perf_graph/perf_graph.i)
- (modules/combined/examples/phase_field-mechanics/EBSD_reconstruction_grain_growth_mech.i)
- (modules/xfem/test/tests/moment_fitting/solid_mechanics_moment_fitting.i)
- (modules/phase_field/examples/grain_growth/3D_6000_gr.i)
- (test/tests/postprocessors/linear_combination/linear_combination.i)
References
No citations exist within this document.(test/tests/markers/reporter_point_marker/reporter_marker_adapt_test.i)
[Mesh]
type = GeneratedMesh
dim = 2
nx = 5
ny = 5
[]
[Problem]
solve = false
[]
[Executioner]
type = Transient
num_steps = 6
dt = 0.1
[]
[Reporters]
[coords]
type=ConstantReporter
real_vector_names = 'y z'
real_vector_values = '.51 .91; 0 0;'
outputs=none
[]
[]
[Functions]
[xfcn]
type = ParsedFunction
expression = t+0.01 #offset so marker is not on element edge
[]
[]
[Postprocessors]
[xfcn_pp]
type = FunctionValuePostprocessor
function = xfcn
execute_on = timestep_end
outputs = none
[]
[x_pp]
type = Receiver
default = .91
outputs = none
[]
[n_elements]
type = NumElements
execute_on = 'timestep_end'
[]
[]
[VectorPostprocessors]
[xfcn_vpp]
type = VectorOfPostprocessors
postprocessors = 'xfcn_pp x_pp'
outputs = none
[]
[]
[Adaptivity]
marker = x_moving
max_h_level = 2
[Markers]
[x_moving]
type = ReporterPointMarker
x_coord_name = xfcn_vpp/xfcn_vpp
y_coord_name = coords/y
z_coord_name = coords/z
inside = REFINE
empty = COARSEN
[]
[]
[]
[Outputs]
csv = true
[]
(test/tests/postprocessors/num_residual_eval/num_residual_eval.i)
[Mesh]
type = GeneratedMesh
dim = 2
nx = 5
ny = 5
xmin = 0
xmax = 2
ymin = 0
ymax = 2
# Since this test prints the number of residual evaluations, its
# output strongly depends on the number of processors you run it on,
# and, apparently, the type of Mesh. To reduce this variability, we
# limit it to run with ReplicatedMesh only.
parallel_type = replicated
[]
[Variables]
active = 'u'
[./u]
order = FIRST
family = LAGRANGE
[../]
[]
[Kernels]
active = 'diff'
[./diff]
type = Diffusion
variable = u
[../]
[]
[BCs]
active = 'left right'
[./left]
type = DirichletBC
variable = u
boundary = 3
value = 0
[../]
[./right]
type = DirichletBC
variable = u
boundary = 1
value = 1
[../]
[]
[Executioner]
type = Steady
solve_type = 'NEWTON'
[]
[Postprocessors]
[./nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[../]
[./elements]
type = NumElements
execute_on = 'initial timestep_end'
[../]
[./dofs]
type = NumDOFs
execute_on = 'initial timestep_end'
[../]
[./residuals]
type = NumResidualEvaluations
execute_on = 'initial timestep_end'
[../]
[]
[Outputs]
file_base = out
exodus = false
csv = true
[]
(test/tests/postprocessors/difference_pps/difference_depend_check.i)
[Mesh]
type = GeneratedMesh
dim = 2
xmin = 0
xmax = 1
ymin = 0
ymax = 1
nx = 2
ny = 2
[]
[Variables]
[./u]
[../]
[]
[AuxVariables]
[./v]
[../]
[]
[AuxKernels]
[./one]
type = ConstantAux
variable = v
value = 1
[../]
[]
[Postprocessors]
# This postprocessor is listed first on purpose to give the resolver something to do
[./diff]
type = DifferencePostprocessor
value1 = nodes
value2 = elems
execute_on = 'initial timestep_end'
[../]
[./nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[../]
[./elems]
type = NumElements
execute_on = 'initial timestep_end'
[../]
[]
[Problem]
type = FEProblem
solve = false
kernel_coverage_check = false
[]
[Executioner]
type = Steady
[]
[Outputs]
csv = true
[]
(modules/phase_field/examples/ebsd_reconstruction/IN100-111grn.i)
[Mesh]
[ebsd_mesh]
type = EBSDMeshGenerator
filename = IN100_120x120.txt
pre_refine = 2
[]
[]
[GlobalParams]
op_num = 8
var_name_base = gr
[]
[UserObjects]
[ebsd_reader]
type = EBSDReader
[]
[ebsd]
type = PolycrystalEBSD
coloring_algorithm = bt
ebsd_reader = ebsd_reader
enable_var_coloring = true
[]
[grain_tracker]
type = GrainTracker
flood_entity_type = ELEMENTAL
compute_halo_maps = true # For displaying HALO fields
polycrystal_ic_uo = ebsd
[]
[]
[ICs]
[PolycrystalICs]
[PolycrystalColoringIC]
polycrystal_ic_uo = ebsd
[]
[]
[]
[Variables]
[PolycrystalVariables]
[]
[]
[AuxVariables]
[bnds]
[]
[unique_grains_ic]
order = CONSTANT
family = MONOMIAL
[]
[unique_grains]
order = CONSTANT
family = MONOMIAL
[]
[ghost_elements]
order = CONSTANT
family = MONOMIAL
[]
[halos]
order = CONSTANT
family = MONOMIAL
[]
[var_indices_ic]
order = CONSTANT
family = MONOMIAL
[]
[var_indices]
order = CONSTANT
family = MONOMIAL
[]
[ebsd_grains]
family = MONOMIAL
order = CONSTANT
[]
[]
[Kernels]
[PolycrystalKernel]
[]
[]
[AuxKernels]
[BndsCalc]
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[]
[ghost_elements]
type = FeatureFloodCountAux
variable = ghost_elements
field_display = GHOSTED_ENTITIES
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[]
[halos]
type = FeatureFloodCountAux
variable = halos
field_display = HALOS
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[]
[var_indices_ic]
type = FeatureFloodCountAux
variable = var_indices_ic
execute_on = 'initial'
flood_counter = ebsd
field_display = VARIABLE_COLORING
[]
[unique_grains_ic]
type = FeatureFloodCountAux
variable = unique_grains_ic
execute_on = 'initial'
flood_counter = ebsd
field_display = UNIQUE_REGION
[]
[var_indices]
type = FeatureFloodCountAux
variable = var_indices
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = VARIABLE_COLORING
[]
[unique_grains]
type = FeatureFloodCountAux
variable = unique_grains
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = UNIQUE_REGION
[]
[grain_aux]
type = EBSDReaderPointDataAux
variable = ebsd_grains
ebsd_reader = ebsd_reader
data_name = 'feature_id'
execute_on = 'initial timestep_end'
[]
[]
[Modules]
[PhaseField]
[EulerAngles2RGB]
crystal_structure = cubic
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
[]
[]
[]
[Materials]
[Copper]
# T = 500 # K
type = GBEvolution
T = 500
wGB = 0.6 # um
GBmob0 = 2.5e-6 # m^4/(Js) from Schoenfelder 1997
Q = 0.23 # Migration energy in eV
GBenergy = 0.708 # GB energy in J/m^2
molar_volume = 7.11e-6 # Molar volume in m^3/mol
length_scale = 1.0e-6
time_scale = 1.0e-6
[]
[]
[Postprocessors]
[dt]
type = TimestepSize
[]
[n_elements]
type = NumElements
execute_on = 'initial timestep_end'
[]
[n_nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[]
[DOFs]
type = NumDOFs
[]
[]
[Executioner]
type = Transient
scheme = bdf2
solve_type = PJFNK
petsc_options_iname = '-pc_type -pc_hypre_type -pc_hypre_boomeramg_strong_threshold'
petsc_options_value = 'hypre boomeramg 0.7'
l_tol = 1.0e-4
l_max_its = 20
nl_max_its = 20
nl_rel_tol = 1.0e-8
start_time = 0.0
num_steps = 30
[TimeStepper]
type = IterationAdaptiveDT
cutback_factor = 0.9
dt = 10.0
growth_factor = 1.1
optimal_iterations = 7
[]
[Adaptivity]
initial_adaptivity = 2
refine_fraction = 0.7
coarsen_fraction = 0.1
max_h_level = 2
[]
[]
[Outputs]
exodus = true
checkpoint = true
perf_graph = true
[]
(modules/phase_field/test/tests/GBType/GB_Type_Phase1.i)
# MOOSE input file
# Written by Pierre-Clement Simon - Idaho National Laboratory
#
# Project:
# TRISO fuel fission gas transport: Silver diffusion in silicon carbide
#
# Published with:
# ---
#
# Phase Field Model: Isotropic diffusion equation
# type: Transient
# Grain structure: Single grain
# BCs: Fixed value on the right, flux on the left
#
#
# Info:
# - Input file used to generate polycrystals for SiC
#
# Updates from previous file:
# -
#
# Units
# length: --
# time: --
# energy: --
# quantity: --
# This simulation predicts GB migration of a 2D copper polycrystal with 15 grains
# Mesh adaptivity (new system) and time step adaptivity are used
# An AuxVariable is used to calculate the grain boundary locations
# Postprocessors are used to record time step and the number of grains
# We are not using the GrainTracker in this example so the number
# of order paramaters must match the number of grains.
[Mesh]
[ebsd_mesh]
type = EBSDMeshGenerator
# Two Parallel Grains
filename = 'EBSD_ThreeGrains.txt'
[]
[]
[GlobalParams]
# Parameters used by several kernels that are defined globally to simplify input file
op_num = 6 # Number of grains
var_name_base = gr # Base name of grains
[]
[UserObjects]
[ebsd_reader]
type = EBSDReader
[]
[ebsd]
type = PolycrystalEBSD
coloring_algorithm = bt
ebsd_reader = ebsd_reader
enable_var_coloring = true
# output_adjacency_matrix = true
[]
[grain_tracker]
type = GrainTracker
threshold = 0.001
connecting_threshold = 0.008
compute_var_to_feature_map = true
compute_halo_maps = true # For displaying HALO fields
remap_grains = true
polycrystal_ic_uo = ebsd
[]
[]
[ICs]
[PolycrystalICs]
[PolycrystalColoringIC]
polycrystal_ic_uo = ebsd
[]
[]
[]
[Variables]
# Variable block, where all variables in the simulation are declared
[./PolycrystalVariables]
# Custom action that created all of the grain variables and sets their initial condition
[../]
[]
[AuxVariables]
# Dependent variables
[./bnds]
# Variable used to visualize the grain boundaries in the simulation
[../]
[./unique_grains]
order = CONSTANT
family = MONOMIAL
[../]
[./aphi1]
order = CONSTANT
family = MONOMIAL
[../]
[./bPhi]
order = CONSTANT
family = MONOMIAL
[../]
[./cphi2]
order = CONSTANT
family = MONOMIAL
[../]
[./ebsd_numbers]
order = CONSTANT
family = MONOMIAL
[../]
[]
[Kernels]
# Kernel block, where the kernels defining the residual equations are set up.
[./PolycrystalKernel]
# Custom action creating all necessary kernels for grain growth. All input parameters are up in GlobalParams
[../]
[]
[AuxKernels]
# AuxKernel block, defining the equations used to calculate the auxvars
[./bnds_aux]
# AuxKernel that calculates the GB term
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[../]
# generate the unique ID from grain_tracker
[./unique_grains]
type = FeatureFloodCountAux
variable = unique_grains
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = UNIQUE_REGION
[../]
# The phi will output the Euler angle from EBSD data, and the data structure
# will change with the guide from grain_tracker
[./aphi1]
type = OutputEulerAngles
variable = aphi1
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
output_euler_angle = 'phi1'
execute_on = 'INITIAL TIMESTEP_END'
[../]
[./bPhi]
type = OutputEulerAngles
variable = bPhi
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
output_euler_angle = 'Phi'
execute_on = 'INITIAL TIMESTEP_END'
[../]
[./cphi2]
type = OutputEulerAngles
variable = cphi2
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
output_euler_angle = 'phi2'
execute_on = 'INITIAL TIMESTEP_END'
[../]
# Import the unique grain ID from ebsd data, and the data structure
# will change with the guide from grain_tracker
[ebsd_numbers]
type = EBSDReaderAvgDataAux
data_name = feature_id
ebsd_reader = ebsd_reader
grain_tracker = grain_tracker
variable = ebsd_numbers
execute_on = 'initial timestep_end'
[../]
[]
[BCs]
# Boundary Condition block
[./Periodic]
[./top_bottom]
auto_direction = 'x y' # Makes problem periodic in the x and y directions
[../]
[../]
[]
[Materials]
[./CuGrGr]
# Material properties
type = GBEvolution # Quantitative material properties for copper grain growth. Dimensions are nm and ns
GBmob0 = 2.5e-6 # Mobility prefactor for Cu from schonfelder1997molecular bibtex entry
GBenergy = 0.708 # GB energy for Cu from schonfelder1997molecular bibtex entry
Q = 0.23 # Activation energy for grain growth from Schonfelder 1997
T = 450 # Constant temperature of the simulation (for mobility calculation)
wGB = 6 # Width of the diffuse GB
[../]
[./GB_type]
# The new developed Miso Bnds Aux Kernel
type = ComputeGBMisorientationType
ebsd_reader = ebsd_reader
grain_tracker = grain_tracker
output_properties = 'gb_type'
outputs = exodus
[../]
[]
[Postprocessors]
# Scalar postprocessors
[./dt]
# Outputs the current time step
type = TimestepSize
[../]
[n_elements]
type = NumElements
execute_on = 'initial timestep_end'
[]
[n_nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[]
[DOFs]
type = NumDOFs
[]
[]
[Adaptivity]
initial_steps = 1
max_h_level = 1
marker = combined
[./Indicators]
[./error]
type = GradientJumpIndicator
variable = bnds
[../]
[../]
[./Markers]
[./bound_adapt]
type = ValueThresholdMarker
third_state = DO_NOTHING
coarsen = 0.999 #1.0
refine = 0.95 #0.95
variable = bnds
invert = true
[../]
[./errorfrac]
type = ErrorFractionMarker
coarsen = 0.1
indicator = error
refine = 0.7
[../]
[./combined]
type = ComboMarker
markers = 'bound_adapt errorfrac'
[../]
[../]
[]
[Executioner]
type = Transient # Type of executioner, here it is transient with an adaptive time step
scheme = bdf2 # Type of time integration (2nd order backward euler), defaults to 1st order backward euler
#Preconditioned JFNK (default)
solve_type = 'PJFNK'
petsc_options_iname = '-pc_type -pc_hypre_type -pc_hypre_boomeramg_strong_threshold'
petsc_options_value = ' hypre boomeramg 0.7'
l_max_its = 30 # Max number of linear iterations
l_tol = 1e-4 # Relative tolerance for linear solves
nl_max_its = 40 # Max number of nonlinear iterations
nl_abs_tol = 1e-11 # Relative tolerance for nonlienar solves
nl_rel_tol = 1e-10 # Absolute tolerance for nonlienar solves
[TimeStepper]
type = IterationAdaptiveDT
cutback_factor = 0.9
dt = 1
growth_factor = 1.1
optimal_iterations = 7
[]
start_time = 0.0
num_steps = 2
[]
[Outputs]
perf_graph = true
exodus = true
[./console]
type = Console
max_rows = 10
[../]
[]
(modules/phase_field/test/tests/grain_tracker_test/split_grain.i)
[Mesh]
[ebsd_mesh]
type = EBSDMeshGenerator
filename = EBSD_split_grain.txt
[]
[]
[GlobalParams]
op_num = 4
var_name_base = gr
[]
[UserObjects]
[ebsd_reader]
type = EBSDReader
[]
[ebsd]
type = PolycrystalEBSD
coloring_algorithm = bt
ebsd_reader = ebsd_reader
enable_var_coloring = true
output_adjacency_matrix = true
[]
[grain_tracker]
type = GrainTracker
flood_entity_type = ELEMENTAL
compute_halo_maps = true # For displaying HALO fields
polycrystal_ic_uo = ebsd
[]
[]
[ICs]
[PolycrystalICs]
[PolycrystalColoringIC]
polycrystal_ic_uo = ebsd
[]
[]
[]
[Variables]
[PolycrystalVariables]
[]
[]
[AuxVariables]
[bnds]
[]
[unique_grains]
order = CONSTANT
family = MONOMIAL
[]
[ghost_elements]
order = CONSTANT
family = MONOMIAL
[]
[halos]
order = CONSTANT
family = MONOMIAL
[]
[var_indices]
order = CONSTANT
family = MONOMIAL
[]
[ebsd_grains]
family = MONOMIAL
order = CONSTANT
[]
[]
[Kernels]
[PolycrystalKernel]
[]
[]
[AuxKernels]
[BndsCalc]
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[]
[ghost_elements]
type = FeatureFloodCountAux
variable = ghost_elements
field_display = GHOSTED_ENTITIES
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[]
[halos]
type = FeatureFloodCountAux
variable = halos
field_display = HALOS
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[]
[var_indices]
type = FeatureFloodCountAux
variable = var_indices
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = VARIABLE_COLORING
[]
[unique_grains]
type = FeatureFloodCountAux
variable = unique_grains
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = UNIQUE_REGION
[]
[grain_aux]
type = EBSDReaderPointDataAux
variable = ebsd_grains
ebsd_reader = ebsd_reader
data_name = 'feature_id'
execute_on = 'initial timestep_end'
[]
[]
[Modules]
[PhaseField]
[EulerAngles2RGB]
crystal_structure = cubic
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
[]
[]
[]
[Materials]
[Copper]
# T = 500 # K
type = GBEvolution
T = 500
wGB = 0.6 # um
GBmob0 = 2.5e-6 # m^4/(Js) from Schoenfelder 1997
Q = 0.23 # Migration energy in eV
GBenergy = 0.708 # GB energy in J/m^2
molar_volume = 7.11e-6 # Molar volume in m^3/mol
length_scale = 1.0e-6
time_scale = 1.0e-6
[]
[]
[Postprocessors]
[n_elements]
type = NumElements
execute_on = 'initial timestep_end'
[]
[n_nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[]
[DOFs]
type = NumDOFs
[]
[]
[Executioner]
type = Transient
scheme = bdf2
solve_type = PJFNK
petsc_options_iname = '-pc_type -pc_hypre_type -pc_hypre_boomeramg_strong_threshold'
petsc_options_value = 'hypre boomeramg 0.7'
l_tol = 1.0e-4
l_max_its = 20
nl_max_its = 20
nl_rel_tol = 1.0e-8
start_time = 0.0
num_steps = 2
[TimeStepper]
type = IterationAdaptiveDT
cutback_factor = 0.9
dt = 10.0
growth_factor = 1.1
optimal_iterations = 7
[]
[]
[Outputs]
exodus = true
csv = true
perf_graph = true
[]
(test/tests/outputs/hide_vector_pp/hide_vector_pp.i)
[Mesh]
type = GeneratedMesh
dim = 2
nx = 10
ny = 10
[]
[Variables]
[./u]
[../]
[]
[Kernels]
[./diff]
type = CoefDiffusion
variable = u
coef = 0.1
[../]
[./time]
type = TimeDerivative
variable = u
[../]
[]
[BCs]
[./left]
type = DirichletBC
variable = u
boundary = left
value = 0
[../]
[./right]
type = DirichletBC
variable = u
boundary = right
value = 1
[../]
[]
[Postprocessors]
[./pp]
type = NumElements
outputs = csv
[../]
[]
[VectorPostprocessors]
[./vpp]
type = LineValueSampler
variable = u
start_point = '0 0 0'
end_point = '1 1 0'
num_points = 10
sort_by = id
outputs = 'test'
[../]
[]
[Executioner]
type = Transient
num_steps = 20
dt = 0.1
solve_type = PJFNK
petsc_options_iname = '-pc_type -pc_hypre_type'
petsc_options_value = 'hypre boomeramg'
[]
[Outputs]
csv = true
[./test]
type = CSV
execute_on = 'FINAL'
[../]
[]
(test/tests/mesh/splitting/geometric_neighbors.i)
[Mesh]
type = GeneratedMesh
dim = 2
nx = 8
ny = 2
xmax = 8
ymax = 2
# We are testing geometric ghosted functors
# so we have to use distributed mesh
parallel_type = distributed
[]
[Variables]
[./u]
[../]
[]
[AuxVariables]
[./ghosted_elements]
order = CONSTANT
family = MONOMIAL
[../]
[./proc]
order = CONSTANT
family = MONOMIAL
[../]
[]
[AuxKernels]
[./random_elemental]
type = ElementUOAux
variable = ghosted_elements
element_user_object = ghost_uo
field_name = "ghosted"
execute_on = initial
[../]
[./proc]
type = ProcessorIDAux
variable = proc
execute_on = initial
[../]
[]
[UserObjects]
[./ghost_uo]
type = ElemSideNeighborLayersGeomTester
execute_on = initial
element_side_neighbor_layers = 2
[../]
[]
[Postprocessors]
[./num_elems]
type = NumElements
[../]
[]
[Executioner]
type = Steady
[]
[Outputs]
exodus = true
[]
[Problem]
solve = false
kernel_coverage_check = false
[]
(test/tests/postprocessors/relative_difference/relative_difference.i)
# Tests the RelativeDifferencePostprocessor post-processor, which computes
# the relative difference between 2 post-processor values.
[Mesh]
type = GeneratedMesh
dim = 1
nx = 2
[]
[Problem]
solve = false
[]
[Executioner]
type = Steady
[]
[Postprocessors]
[./num_elems]
# number of elements, equal to 2
type = NumElements
[../]
[./num_nodes]
# number of nodes, equal to 3
type = NumNodes
[../]
[./zero]
# zero post-processor value
type = EmptyPostprocessor
[../]
# For the case in this input file, this will be computed as
# y = abs((num_nodes - num_elems) / num_elems)
# y = abs((3 - 2 ) / 2 ) = 0.5
# When the command-line modification "Postprocessors/relative_difference/value2=zero" is used,
# y = abs(num_nodes - zero)
# y = abs(3 - 0 ) = 3
[./relative_difference]
type = RelativeDifferencePostprocessor
value1 = num_nodes
value2 = num_elems
[../]
[]
[Outputs]
[./out]
type = CSV
show = relative_difference
[../]
[]
(test/tests/postprocessors/num_elems/num_elems.i)
[Mesh]
type = GeneratedMesh
dim = 2
nx = 4
ny = 4
nz = 0
zmax = 0
elem_type = QUAD4
uniform_refine = 1
[]
[Variables]
[./u]
order = FIRST
family = LAGRANGE
[../]
[]
[AuxVariables]
[./u_aux]
order = FIRST
family = LAGRANGE
[../]
[./v_aux]
order = FIRST
family = LAGRANGE
[../]
[]
[Functions]
[./force]
type = ParsedFunction
expression = t
[../]
[]
[Kernels]
[./diff]
type = Diffusion
variable = u
[../]
[./force]
type = BodyForce
variable = u
function = force
[../]
[]
[BCs]
[./right]
type = DirichletBC
variable = u
boundary = right
value = 1
[../]
[./left]
type = DirichletBC
variable = u
boundary = left
value = 0
[../]
[]
[Executioner]
type = Transient
num_steps = 3
dt = 1
solve_type = PJFNK
[]
[Adaptivity]
steps = 1
marker = box
max_h_level = 3
[./Markers]
[./box]
bottom_left = '0.3 0.3 0'
inside = refine
top_right = '0.6 0.6 0'
outside = do_nothing
type = BoxMarker
[../]
[../]
[]
[Postprocessors]
[./num_elems_active]
type = NumElements
elem_filter = 'ACTIVE'
execute_on = 'initial timestep_end'
[../]
[./num_elems_total]
type = NumElements
elem_filter = 'TOTAL'
execute_on = 'initial timestep_end'
[../]
[]
[Outputs]
csv = true
[]
(modules/phase_field/test/tests/reconstruction/euler2rgb_non_uniform_orientation.i)
[Mesh]
[ebsd_mesh]
type = EBSDMeshGenerator
filename = ebsd_scan.txt
[]
[]
[GlobalParams]
op_num = 10
var_name_base = gr
[]
[UserObjects]
[ebsd_reader]
type = EBSDReader
bins = 40
[]
[ebsd]
type = PolycrystalEBSD
coloring_algorithm = jp
ebsd_reader = ebsd_reader
enable_var_coloring = true
[]
[grain_tracker]
type = GrainTracker
flood_entity_type = ELEMENTAL
compute_halo_maps = true # For displaying HALO fields
polycrystal_ic_uo = ebsd
[]
[]
[ICs]
[PolycrystalICs]
[PolycrystalColoringIC]
polycrystal_ic_uo = ebsd
[]
[]
[]
[Variables]
[PolycrystalVariables]
[]
[]
[AuxVariables]
[bnds]
[]
[]
[Kernels]
[PolycrystalKernel]
[]
[]
[AuxKernels]
[BndsCalc]
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[]
[]
[Modules]
[PhaseField]
[EulerAngles2RGB]
crystal_structure = cubic
euler_angle_provider = ebsd_reader
grain_tracker = grain_tracker
[]
[]
[]
[Materials]
[Copper]
# T = 500 # K
type = GBEvolution
T = 500
wGB = 0.6 # um
GBmob0 = 2.5e-6 # m^4/(Js) from Schoenfelder 1997
Q = 0.23 # Migration energy in eV
GBenergy = 0.708 # GB energy in J/m^2
molar_volume = 7.11e-6 # Molar volume in m^3/mol
length_scale = 1.0e-6
time_scale = 1.0e-6
[]
[]
[Postprocessors]
[dt]
type = TimestepSize
[]
[n_elements]
type = NumElements
execute_on = 'initial timestep_end'
[]
[n_nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[]
[DOFs]
type = NumDOFs
[]
[]
[Executioner]
type = Transient
scheme = bdf2
solve_type = Newton
petsc_options_iname = '-pc_type -pc_hypre_type -pc_hypre_boomeramg_strong_threshold'
petsc_options_value = 'hypre boomeramg 0.7'
l_tol = 1.0e-6
l_max_its = 100
nl_max_its = 20
nl_rel_tol = 1.0e-8
start_time = 0.0
num_steps = 0
[]
[Outputs]
exodus = true
perf_graph = true
[]
(test/tests/outputs/perf_graph/perf_graph.i)
[Mesh]
type = GeneratedMesh
dim = 3
nx = 20
ny = 20
nz = 20
[]
[Variables]
[./u]
[../]
[]
[Kernels]
[./diff]
type = Diffusion
variable = u
[../]
[]
[BCs]
[./left]
type = DirichletBC
variable = u
boundary = left
value = 0
[../]
[./right]
type = DirichletBC
variable = u
boundary = right
value = 1
[../]
[]
[Postprocessors]
[./num_dofs]
type = NumElements
[../]
[../]
[Executioner]
type = Steady
solve_type = 'PJFNK'
petsc_options_iname = '-pc_type -pc_hypre_type'
petsc_options_value = 'hypre boomeramg'
[]
[Outputs]
# perf_graph = true
[./pgraph]
type = PerfGraphOutput
level = 1
heaviest_branch = true
heaviest_sections = 10
[]
[]
(modules/combined/examples/phase_field-mechanics/EBSD_reconstruction_grain_growth_mech.i)
# This example reconstructs the grain structure from an EBSD data file
# Then, an isotropic grain model is run with linear elasticity and an anisotropic
# elasticity tensor that uses the measured EBSD angles.
[Mesh]
[ebsd_mesh]
type = EBSDMeshGenerator
uniform_refine = 2 #Mesh can go two levels coarser than the EBSD grid
filename = IN100_128x128.txt
[]
[]
[GlobalParams]
op_num = 8
var_name_base = gr
displacements = 'disp_x disp_y'
[]
[Variables]
[PolycrystalVariables] #Polycrystal variable generation (30 order parameters)
[]
[disp_x]
[]
[disp_y]
[]
[]
[AuxVariables]
[bnds]
[]
[gt_indices]
order = CONSTANT
family = MONOMIAL
[]
[unique_grains]
order = CONSTANT
family = MONOMIAL
[]
[vonmises_stress]
order = CONSTANT
family = MONOMIAL
[]
[C1111]
order = CONSTANT
family = MONOMIAL
[]
[phi1]
order = CONSTANT
family = MONOMIAL
[]
[Phi]
order = CONSTANT
family = MONOMIAL
[]
[phi2]
order = CONSTANT
family = MONOMIAL
[]
[EBSD_grain]
family = MONOMIAL
order = CONSTANT
[]
[]
[ICs]
[PolycrystalICs]
[ReconVarIC]
ebsd_reader = ebsd
coloring_algorithm = bt
[]
[]
[]
[Kernels]
[PolycrystalKernel]
[]
[PolycrystalElasticDrivingForce]
[]
[TensorMechanics]
[]
[]
[AuxKernels]
[BndsCalc]
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[]
[gt_indices]
type = FeatureFloodCountAux
variable = gt_indices
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = VARIABLE_COLORING
[]
[unique_grains]
type = FeatureFloodCountAux
variable = unique_grains
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
field_display = UNIQUE_REGION
[]
[C1111]
type = RankFourAux
variable = C1111
rank_four_tensor = elasticity_tensor
index_l = 0
index_j = 0
index_k = 0
index_i = 0
execute_on = timestep_end
[]
[vonmises_stress]
type = RankTwoScalarAux
variable = vonmises_stress
rank_two_tensor = stress
scalar_type = VonMisesStress
execute_on = timestep_end
[]
[phi1]
type = OutputEulerAngles
variable = phi1
euler_angle_provider = ebsd
grain_tracker = grain_tracker
output_euler_angle = 'phi1'
execute_on = 'initial'
[]
[Phi]
type = OutputEulerAngles
variable = Phi
euler_angle_provider = ebsd
grain_tracker = grain_tracker
output_euler_angle = 'Phi'
execute_on = 'initial'
[]
[phi2]
type = OutputEulerAngles
variable = phi2
euler_angle_provider = ebsd
grain_tracker = grain_tracker
output_euler_angle = 'phi2'
execute_on = 'initial'
[]
[grain_aux]
type = EBSDReaderPointDataAux
variable = EBSD_grain
ebsd_reader = ebsd
data_name = 'feature_id'
execute_on = 'initial'
[]
[]
[BCs]
[top_displacement]
type = DirichletBC
variable = disp_y
boundary = top
value = -2.0
[]
[x_anchor]
type = DirichletBC
variable = disp_x
boundary = 'left right'
value = 0.0
[]
[y_anchor]
type = DirichletBC
variable = disp_y
boundary = bottom
value = 0.0
[]
[]
[Modules]
[PhaseField]
[EulerAngles2RGB]
crystal_structure = cubic
euler_angle_provider = ebsd
grain_tracker = grain_tracker
[]
[]
[]
[Materials]
[Copper]
# T = 500 # K
type = GBEvolution
block = 0
T = 500
wGB = 0.6 # um
GBmob0 = 2.5e-6 # m^4/(Js) from Schoenfelder 1997
Q = 0.23 # Migration energy in eV
GBenergy = 0.708 # GB energy in J/m^2
molar_volume = 7.11e-6; # Molar volume in m^3/mol
length_scale = 1.0e-6
time_scale = 1.0e-6
[]
[ElasticityTensor]
type = ComputePolycrystalElasticityTensor
grain_tracker = grain_tracker
[]
[strain]
type = ComputeSmallStrain
block = 0
displacements = 'disp_x disp_y'
[]
[stress]
type = ComputeLinearElasticStress
block = 0
[]
[]
[Postprocessors]
[dt]
type = TimestepSize
[]
[n_elements]
type = NumElements
execute_on = 'initial timestep_end'
[]
[n_nodes]
type = NumNodes
execute_on = 'initial timestep_end'
[]
[DOFs]
type = NumDOFs
[]
[]
[UserObjects]
[ebsd]
type = EBSDReader
[]
[grain_tracker]
type = GrainTrackerElasticity
compute_var_to_feature_map = true
ebsd_reader = ebsd
fill_method = symmetric9
C_ijkl = '1.27e5 0.708e5 0.708e5 1.27e5 0.708e5 1.27e5 0.7355e5 0.7355e5 0.7355e5'
euler_angle_provider = ebsd
[]
[]
[Executioner]
type = Transient
scheme = bdf2
solve_type = PJFNK
petsc_options_iname = '-pc_type -pc_hypre_type -pc_hypre_boomeramg_strong_threshold'
petsc_options_value = ' hypre boomeramg 0.7'
l_tol = 1.0e-4
l_max_its = 20
nl_max_its = 20
nl_rel_tol = 1.0e-8
start_time = 0.0
num_steps = 30
dt = 10
[Adaptivity]
initial_adaptivity = 0
refine_fraction = 0.7
coarsen_fraction = 0.1
max_h_level = 2
[]
[TimeStepper]
type = IterationAdaptiveDT
cutback_factor = 0.9
dt = 10.0
growth_factor = 1.1
optimal_iterations = 7
[]
[]
[Outputs]
csv = true
exodus = true
[]
(modules/xfem/test/tests/moment_fitting/solid_mechanics_moment_fitting.i)
# Test for a mechanics problem which uses four points moment_fitting approach.
# See this paper (https://doi.org/10.1007/s00466-018-1544-2) for more details about moment_fitting approach.
[GlobalParams]
order = FIRST
family = LAGRANGE
displacements = 'disp_x disp_y'
volumetric_locking_correction = true
[]
[XFEM]
qrule = moment_fitting
output_cut_plane = true
[]
[Mesh]
type = GeneratedMesh
dim = 2
nx = 10
ny = 10
xmin = 0.0
xmax = 1.0
ymin = 0.0
ymax = 1.0
elem_type = QUAD4
[]
[UserObjects]
[./line_seg_cut_uo0]
type = LineSegmentCutUserObject
cut_data = '0.0000e+00 6.3330e-01 3.9000e-01 6.3330e-01'
time_start_cut = 0.0
time_end_cut = 0.0
[../]
[./line_seg_cut_uo1]
type = LineSegmentCutUserObject
cut_data = '3.9000e-01 6.3330e-01 6.8000e-01 6.3330e-01'
time_start_cut = 0.0
time_end_cut = 0.0
[../]
[]
[Variables]
[./disp_x]
[../]
[./disp_y]
[../]
[]
[Physics/SolidMechanics/QuasiStatic]
[./all]
strain = SMALL
[../]
[]
[Functions]
[./right_trac_x]
type = ParsedFunction
expression = '-(t*M*y)/I'
symbol_names = 'M E I'
symbol_values = '2e4 1e6 0.666666667'
[../]
[./bottom_disp_y]
type = ParsedFunction
expression = '((t*M)/(2*E*I))*(1-nu*nu)*(x*x-0.25*l*l)'
symbol_names = 'M E I l nu'
symbol_values = '2e4 1e6 0.666666667 2.0 0.3'
[../]
[./soln_x]
type = ParsedFunction
expression = '-(M/(E*I))*(1-nu*nu)*x*y'
symbol_names = 'M E I nu'
symbol_values = '2e4 1e6 0.666666667 0.3'
[../]
[./soln_y]
type = ParsedFunction
expression = '(M/(2*E*I))*(1-nu*nu)*(x*x-0.25*l*l+(nu/(1-nu))*y*y)'
symbol_names = 'M E I l nu'
symbol_values = '2e4 1e6 0.666666667 2.0 0.3'
[../]
[]
[BCs]
[./right_x]
type = FunctionNeumannBC
boundary = 1
variable = disp_x
function = right_trac_x
[../]
[./bottom_y]
type = FunctionDirichletBC
boundary = 0
variable = disp_y
function = bottom_disp_y
[../]
[./left_x]
type = DirichletBC
boundary = 3
variable = disp_x
value = 0.0
[../]
[]
[Materials]
[./elasticity_tensor]
type = ComputeIsotropicElasticityTensor
youngs_modulus = 1e6
poissons_ratio = 0.3
[../]
[./stress]
type = ComputeLinearElasticStress
[../]
[]
[Executioner]
type = Transient
solve_type = 'PJFNK'
petsc_options_iname = '-ksp_gmres_restart -pc_type -pc_hypre_type -pc_hypre_boomeramg_max_iter'
petsc_options_value = '201 hypre boomeramg 8'
line_search = 'none'
# [./Quadrature]
# order = FOURTH
# type = MONOMIAL
# [../]
[./Predictor]
type = SimplePredictor
scale = 1.0
[../]
# controls for linear iterations
l_max_its = 100
l_tol = 1e-2
# controls for nonlinear iterations
nl_max_its = 15
nl_rel_tol = 1e-16
nl_abs_tol = 1e-10
# time control
start_time = 0.0
dt = 0.5
end_time = 1.0
num_steps = 5000
[]
[Postprocessors]
[./numel]
type = NumElements
execute_on = timestep_end
[../]
[./integral]
type = ElementVectorL2Error
var_x = disp_x
var_y = disp_y
function_x = soln_x
function_y = soln_y
execute_on = timestep_end
[../]
[]
[Outputs]
exodus = true
[./console]
type = Console
output_linear = true
[../]
[]
(modules/phase_field/examples/grain_growth/3D_6000_gr.i)
[Mesh]
type = GeneratedMesh
dim = 3
nx = 180
ny = 180
nz = 180
xmin = 0
xmax = 180
ymin = 0
ymax = 180
zmin = 0
zmax = 180
elem_type = HEX8
[]
[GlobalParams]
op_num = 28
var_name_base = gr
[]
[Variables]
[./PolycrystalVariables]
order = FIRST
family = LAGRANGE
[../]
[]
[UserObjects]
[./voronoi]
type = PolycrystalVoronoi
grain_num = 6000 # Number of grains
rand_seed = 8675 # 301
coloring_algorithm = jp
[../]
[./term]
type = Terminator
expression = 'grain_tracker < 218'
[../]
[]
[ICs]
[./PolycrystalICs]
[./PolycrystalColoringIC]
polycrystal_ic_uo = voronoi
[../]
[../]
[]
[AuxVariables]
[./bnds]
order = FIRST
family = LAGRANGE
[../]
[./unique_grains]
order = CONSTANT
family = MONOMIAL
[../]
[./ghost_elements]
order = CONSTANT
family = MONOMIAL
[../]
[./halos]
order = CONSTANT
family = MONOMIAL
[../]
[./var_indices]
order = CONSTANT
family = MONOMIAL
[../]
[]
[Kernels]
[./PolycrystalKernel]
[../]
[]
[AuxKernels]
[./BndsCalc]
type = BndsCalcAux
variable = bnds
execute_on = 'initial timestep_end'
[../]
[./unique_grains]
type = FeatureFloodCountAux
variable = unique_grains
field_display = UNIQUE_REGION
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[../]
[./ghost_elements]
type = FeatureFloodCountAux
variable = ghost_elements
field_display = GHOSTED_ENTITIES
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[../]
[./halos]
type = FeatureFloodCountAux
variable = halos
field_display = HALOS
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[../]
[./var_indices]
type = FeatureFloodCountAux
variable = var_indices
field_display = VARIABLE_COLORING
execute_on = 'initial timestep_end'
flood_counter = grain_tracker
[../]
[]
#[BCs]
# [./Periodic]
# [./All]
# auto_direction = 'x y'
# [../]
# [../]
#[]
[Materials]
[./Copper]
type = GBEvolution
T = 500
wGB = 3 # um
GBmob0 = 2.5e-6 #m^4/(Js) from Schoenfelder 1997
Q = 0.23 #Migration energy in eV
GBenergy = 0.708 #GB energy in J/m^2
molar_volume = 7.11e-6 #Molar volume in m^3/mol
length_scale = 1.0e-6
time_scale = 1.0
[../]
[]
[Postprocessors]
[./dt]
type = TimestepSize
[../]
[./n_elements]
type = NumElements
execute_on = timestep_end
[../]
[./n_nodes]
type = NumNodes
execute_on = timestep_end
[../]
[./DOFs]
type = NumDOFs
[../]
[./grain_tracker]
type = GrainTracker
threshold = 0.1
compute_halo_maps = true
[../]
[]
#[Preconditioning]
# [./SMP]
# type = SMP
# full = true
# [../]
#[]
[Executioner]
type = Transient
scheme = bdf2
solve_type = PJFNK #Preconditioned JFNK (default)
petsc_options_iname = '-pc_type'
petsc_options_value = 'asm'
l_tol = 1.0e-4
l_max_its = 30
nl_max_its = 20
nl_rel_tol = 1.0e-8
start_time = 0.0
num_steps = 500
dt = 0.0002
[./TimeStepper]
type = IterationAdaptiveDT
cutback_factor = 0.9
dt = 0.0002
growth_factor = 1.1
optimal_iterations = 8
[../]
#[./Adaptivity]
# initial_adaptivity = 4
# refine_fraction = 0.6
# coarsen_fraction = 0.1
# max_h_level = 4
# print_changed_info = true
#[../]
[]
[Outputs]
nemesis = true
checkpoint = true
csv = true
[./console]
type = Console
[../]
[]
(test/tests/postprocessors/linear_combination/linear_combination.i)
# Tests the LinearCombinationPostprocessor post-processor, which computes
# a linear combination of an arbitrary number of post-processor values.
[Mesh]
type = GeneratedMesh
dim = 1
nx = 2
[]
[Problem]
solve = false
[]
[Executioner]
type = Steady
[]
[Postprocessors]
[./pp1]
# number of elements, equal to 2
type = NumElements
[../]
[./pp2]
# number of nodes, equal to 3
type = NumNodes
[../]
# post-processor value being tested; value should be the following:
# value = c1 * pp1 + c2 * pp2 + b
# = 2 * 2 + -1 * 3 + 5 = 6
[./linear_combination]
type = LinearCombinationPostprocessor
pp_names = 'pp1 pp2'
pp_coefs = '2 -1'
b = 5
[../]
[]
[Outputs]
show = linear_combination
csv = true
[]