Complete Ferret Syntax

Adaptivity/Indicators

• Moose App
• AddElementalFieldActionAdds elemental auxiliary variable for adaptivity system.
• AddIndicatorActionAdd an Indicator object to a simulation.
• AnalyticalIndicatorCompute the square of the error as the difference between an unknown variable and an analytical solution.
• ArrayMooseVariableUsed for grouping standard field variables with the same finite element family and order
• GradientJumpIndicatorCompute the jump of the solution gradient across element boundaries.
• LaplacianJumpIndicatorCompute the jump of the solution laplacian across element bondaries.
• MooseLinearVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableRepresents standard field variables, e.g. Lagrange, Hermite, or non-constant Monomials
• MooseVariableBaseBase class for Moose variables. This should never be the terminal object type
• MooseVariableConstMonomialSpecialization for constant monomials that avoids unnecessary loops
• MooseVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableScalarMoose wrapper class around scalar variables
• ValueJumpIndicatorCompute the jump of the solution across element bondaries.
• VectorMooseVariableRepresents vector field variables, e.g. Vector Lagrange, Nedelec or Raviart-Thomas
• VectorValueJumpIndicatorCompute the jump of the solution across element bondaries.

Adaptivity/Markers

• Moose App
• AddElementalFieldActionAdds elemental auxiliary variable for adaptivity system.
• AddMarkerActionAdd a Marker object to a simulation.
• ArrayMooseVariableUsed for grouping standard field variables with the same finite element family and order
• BoundaryMarkerMarks all elements with sides on a given boundary for refinement/coarsening
• BoundaryPreservedMarkerMarks elements for refinement or coarsening based on the provided marker value, while preserving the given boundary.
• BoxMarkerMarks the region inside and outside of a 'box' domain for refinement or coarsening.
• ComboMarkerA marker that converts many markers into a single marker by considering the maximum value of the listed markers (i.e., refinement takes precedent).
• ErrorFractionMarkerMarks elements for refinement or coarsening based on the fraction of the min/max error from the supplied indicator.
• ErrorToleranceMarkerCoarsen or refine elements based on an absolute tolerance allowed from the supplied indicator.
• MooseLinearVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableRepresents standard field variables, e.g. Lagrange, Hermite, or non-constant Monomials
• MooseVariableBaseBase class for Moose variables. This should never be the terminal object type
• MooseVariableConstMonomialSpecialization for constant monomials that avoids unnecessary loops
• MooseVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableScalarMoose wrapper class around scalar variables
• OrientedBoxMarkerMarks inside and outside a box that can have arbitrary orientation and center point.
• ReporterPointMarkerMarks the region inside or empty if it contains a reporter defined point for refinement or coarsening.
• UniformMarkerUniformly mark all elements for refinement or coarsening.
• ValueRangeMarkerMark elements for adaptivity based on the supplied upper and lower bounds and the specified variable.
• ValueThresholdMarkerThe refinement state based on a threshold value compared to the specified variable.
• VectorMooseVariableRepresents vector field variables, e.g. Vector Lagrange, Nedelec or Raviart-Thomas
• Phase Field App
• DiscreteNucleationMarkerMark new nucleation sites for refinement
• Ferret App
• PolarDomainMarkerMark elements for adaptivity based on the supplied upper and lower bounds and the specified variable.
• PolarizationNWEMarkerThe the refinement state based on a threshold value compared to the specified variable.

AuxKernels/MatVecRealGradAuxKernel

• Phase Field App
• MatVecRealGradAuxKernelActionOutputs all components of the gradient of the real standard vector-valued properties specified

AuxKernels/MaterialVectorAuxKernel

• Phase Field App
• MaterialVectorAuxKernelActionOutputs all components of the standard vector-valued properties specified

AuxKernels/MaterialVectorGradAuxKernel

• Phase Field App
• MaterialVectorGradAuxKernelActionOutputs all components of the gradient of the real standard vector-valued properties specified

AuxVariables/MultiAuxVariables

• Moose App
• ArrayMooseVariableUsed for grouping standard field variables with the same finite element family and order
• MooseLinearVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableRepresents standard field variables, e.g. Lagrange, Hermite, or non-constant Monomials
• MooseVariableBaseBase class for Moose variables. This should never be the terminal object type
• MooseVariableConstMonomialSpecialization for constant monomials that avoids unnecessary loops
• MooseVariableFVRealBase class for Moose variables. This should never be the terminal object type
• MooseVariableScalarMoose wrapper class around scalar variables
• VectorMooseVariableRepresents vector field variables, e.g. Vector Lagrange, Nedelec or Raviart-Thomas
• Phase Field App
• MultiAuxVariablesActionSet up auxvariables for components of MaterialProperty<std::vector<data_type> > for polycrystal sample.

BCs/CavityPressure

• Solid Mechanics App
• CavityPressureActionAction to setup cavity pressure boundary condition
• CavityPressurePPActionThis Action creates a CavityPressurePostprocessor.
• CavityPressureUOActionAction to add user objects for cavity pressure

BCs/CoupledPressure

• Solid Mechanics App
• CoupledPressureActionSet up pressure boundary condition using the CoupledPressureBC object.

BCs/InclinedNoDisplacementBC

• Solid Mechanics App
• InclinedNoDisplacementBCActionSet up inclined no displacement boundary conditions

BCs/Periodic

• Moose App
• AddPeriodicBCActionAction that adds periodic boundary conditions

BCs/Pressure

• Solid Mechanics App
• PressureActionSet up pressure boundary condition using the Pressure object.

Debug/MaterialDerivativeTest

• Moose App
• MaterialDerivativeTestActionAction for setting up the necessary objects for debugging material property derivatives.

Executioner/Adaptivity

• Moose App
• AdaptivityActionAdd libMesh based adaptation schemes via the Executioner/Adaptivity input syntax.

Executioner/Predictor

• Moose App
• SetupPredictorActionAdd a Predictor object to the simulation.
• AdamsPredictorImplements an explicit Adams predictor based on two old solution vectors.
• SimplePredictorAlgorithm that will predict the next solution based on previous solutions.

Executioner/Quadrature

• Moose App
• SetupQuadratureActionSets the quadrature type for the simulation.

Executioner/TimeIntegrator

• Moose App
• SetupTimeIntegratorActionAdd a TimeIntegrator object to the simulation.
• AStableDirk4Fourth-order diagonally implicit Runge Kutta method (Dirk) with three stages plus an update.
• ActuallyExplicitEulerImplementation of Explicit/Forward Euler without invoking any of the nonlinear solver
• BDF2Second order backward differentiation formula time integration scheme.
• CentralDifferenceImplementation of explicit, Central Difference integration without invoking any of the nonlinear solver
• CrankNicolsonCrank-Nicolson time integrator.
• ExplicitEulerTime integration using the explicit Euler method.
• ExplicitMidpointTime integration using the explicit midpoint method.
• ExplicitSSPRungeKuttaExplicit strong stability preserving Runge-Kutta methods
• ExplicitTVDRK2Explicit TVD (total-variation-diminishing) second-order Runge-Kutta time integration method.
• HeunHeun's (aka improved Euler) time integration method.
• ImplicitEulerTime integration using the implicit Euler method.
• ImplicitMidpointSecond-order Runge-Kutta (implicit midpoint) time integration.
• LStableDirk2Second order diagonally implicit Runge Kutta method (Dirk) with two stages.
• LStableDirk3Third order diagonally implicit Runge Kutta method (Dirk) with three stages.
• LStableDirk4Fourth-order diagonally implicit Runge Kutta method (Dirk) with five stages.
• NewmarkBetaComputes the first and second time derivative of variable using Newmark-Beta method.
• RalstonRalston's time integration method.
• Solid Mechanics App
• DirectCentralDifferenceImplementation of explicit time integration without invoking any of the nonlinear solver.
• ExplicitMixedOrderImplementation of explicit time integration without invoking any of the nonlinear solver.

Executioner/TimeIntegrators

• Moose App
• SetupTimeIntegratorActionAdd a TimeIntegrator object to the simulation.
• AStableDirk4Fourth-order diagonally implicit Runge Kutta method (Dirk) with three stages plus an update.
• ActuallyExplicitEulerImplementation of Explicit/Forward Euler without invoking any of the nonlinear solver
• BDF2Second order backward differentiation formula time integration scheme.
• CentralDifferenceImplementation of explicit, Central Difference integration without invoking any of the nonlinear solver
• CrankNicolsonCrank-Nicolson time integrator.
• ExplicitEulerTime integration using the explicit Euler method.
• ExplicitMidpointTime integration using the explicit midpoint method.
• ExplicitSSPRungeKuttaExplicit strong stability preserving Runge-Kutta methods
• ExplicitTVDRK2Explicit TVD (total-variation-diminishing) second-order Runge-Kutta time integration method.
• HeunHeun's (aka improved Euler) time integration method.
• ImplicitEulerTime integration using the implicit Euler method.
• ImplicitMidpointSecond-order Runge-Kutta (implicit midpoint) time integration.
• LStableDirk2Second order diagonally implicit Runge Kutta method (Dirk) with two stages.
• LStableDirk3Third order diagonally implicit Runge Kutta method (Dirk) with three stages.
• LStableDirk4Fourth-order diagonally implicit Runge Kutta method (Dirk) with five stages.
• NewmarkBetaComputes the first and second time derivative of variable using Newmark-Beta method.
• RalstonRalston's time integration method.
• Solid Mechanics App
• DirectCentralDifferenceImplementation of explicit time integration without invoking any of the nonlinear solver.
• ExplicitMixedOrderImplementation of explicit time integration without invoking any of the nonlinear solver.

Executioner/TimeStepper

• Moose App
• AddTimeStepperActionAdd a TimeStepper object to the simulation.
• AB2PredictorCorrectorImplements second order Adams-Bashforth method for timestep calculation.
• CSVTimeSequenceStepperSolves the Transient problem at a sequence of given time points read in a file.
• CompositionDTThe time stepper takes all the other time steppers as input and returns the minimum time step size.
• ConstantDTTimestepper that takes a constant time step size
• ExodusTimeSequenceStepperSolves the Transient problem at a sequence of time points taken from a specified exodus file.
• FixedPointIterationAdaptiveDTComputes time step size based on a target number of fixed point iterations
• FunctionDTTimestepper whose steps vary over time according to a user-defined function
• IterationAdaptiveDTAdjust the timestep based on the number of iterations
• LogConstantDTTimeStepper which imposes a time step constant in the logarithmic space
• PostprocessorDTComputes timestep based on a Postprocessor value.
• SolutionTimeAdaptiveDTCompute simulation timestep based on actual solution time.
• TimeSequenceFromTimesSolves the Transient problem at a sequence of time points taken from a specified Times object.
• TimeSequenceStepperSolves the Transient problem at a sequence of given time points.

Executioner/TimeSteppers

• Moose App
• ComposeTimeStepperActionAdd the composition time stepper if multiple time steppers have been created.
• AddTimeStepperActionAdd a TimeStepper object to the simulation.
• AB2PredictorCorrectorImplements second order Adams-Bashforth method for timestep calculation.
• CSVTimeSequenceStepperSolves the Transient problem at a sequence of given time points read in a file.
• CompositionDTThe time stepper takes all the other time steppers as input and returns the minimum time step size.
• ConstantDTTimestepper that takes a constant time step size
• ExodusTimeSequenceStepperSolves the Transient problem at a sequence of time points taken from a specified exodus file.
• FixedPointIterationAdaptiveDTComputes time step size based on a target number of fixed point iterations
• FunctionDTTimestepper whose steps vary over time according to a user-defined function
• IterationAdaptiveDTAdjust the timestep based on the number of iterations
• LogConstantDTTimeStepper which imposes a time step constant in the logarithmic space
• PostprocessorDTComputes timestep based on a Postprocessor value.
• SolutionTimeAdaptiveDTCompute simulation timestep based on actual solution time.
• TimeSequenceFromTimesSolves the Transient problem at a sequence of time points taken from a specified Times object.
• TimeSequenceStepperSolves the Transient problem at a sequence of given time points.

Ferret/CubicParentFEPhaseField

• Ferret App
• CubicParentFEPhaseFieldActionSet up a cubic-parent-phase ferroelectric problem: the polarization variables, the Landau bulk and gradient kernels, the optional electrostatic and electrostrictive couplings, the constant material properties and the free energy postprocessors. The mechanics themselves are left to the SolidMechanics QuasiStatic physics, which this action is designed to be used alongside; couple the two by listing 'eigenstrain_name' in its 'eigenstrain_names'.

ICs/PolycrystalICs

InterfaceKernels

• Moose App
• AddInterfaceKernelActionAdd an InterfaceKernel object to the simulation.
• ADMatInterfaceReactionImplements a reaction to establish ReactionRate=k_f*u-k_b*v at interface.
• ADPenaltyInterfaceDiffusionA penalty-based interface condition that forcesthe continuity of variables and the flux equivalence across an interface.
• ADVectorPenaltyInterfaceDiffusionA penalty-based interface condition that forcesthe continuity of variables and the flux equivalence across an interface.
• InterfaceDiffusionThe kernel is utilized to establish flux equivalence on an interface for variables.
• InterfaceEqualityThe kernel is utilized to establish equivalence on an interface for variables.
• InterfaceReactionImplements a reaction to establish ReactionRate=k_f*u-k_b*v at interface.
• PenaltyInterfaceDiffusionA penalty-based interface condition that forcesthe continuity of variables and the flux equivalence across an interface.
• VectorPenaltyInterfaceDiffusionA penalty-based interface condition that forcesthe continuity of variables and the flux equivalence across an interface.
• Electromagnetics App
• ElectrostaticContactConditionInterface condition that describes the current continuity and contact conductance across a boundary formed between two dissimilar materials (resulting in a potential discontinuity). Conductivity on each side of the boundary is defined via the material properties system.
• ParallelElectricFieldInterfaceVectorInterfaceKernel that implements the condition
• PerpendicularElectricFieldInterfaceVectorInterfaceKernel that implements the condition
• Phase Field App
• EqualGradientLagrangeInterfaceEnforce componentwise gradient continuity between two different variables across a subdomain boundary using a Lagrange multiplier
• EqualGradientLagrangeMultiplierLagrange multiplier kernel for EqualGradientLagrangeInterface.
• InterfaceDiffusionBoundaryTermAdd weak form surface terms of the Diffusion equation for two different variables across a subdomain boundary
• InterfaceDiffusionFluxMatchEnforce flux continuity between two different variables across a subdomain boundary
• Solid Mechanics App
• ADCZMInterfaceKernelSmallStrainCZM Interface kernel to use when using the small strain kinematic formulation.
• ADCZMInterfaceKernelTotalLagrangianCZM Interface kernel to use when using the total Lagrangian formulation.
• CZMInterfaceKernelSmallStrainCZM Interface kernel to use when using the Small Strain kinematic formulation.
• CZMInterfaceKernelTotalLagrangianCalculate residual contribution for balancing the traction across an interface (used in the cohesive zone method).

Kernels

• Moose App
• AddKernelActionAdd a Kernel object to the simulation.
• ADArrayDiffusionThe array Laplacian operator (), with the weak form of .
• ADArrayReactionAn automatic differentiation kernel for the array reaction operator ()
• ADBodyForceDemonstrates the multiple ways that scalar values can be introduced into kernels, e.g. (controllable) constants, functions, and postprocessors. Implements the weak form .
• ADCoefReactionImplements the residual term (p*u, test)
• ADConservativeAdvectionConservative form of which in its weak form is given by: . Velocity can be given as 1) a variable, for which the gradient is automatically taken, 2) a vector variable, or a 3) vector material.
• ADCoupledForceImplements a source term proportional to the value of a coupled variable. Weak form: .
• ADCoupledTimeDerivativeTime derivative Kernel that acts on a coupled variable. Weak form: .
• ADDiffusionSame as Diffusion in terms of physics/residual, but the Jacobian is computed using forward automatic differentiation
• ADFluxDivergenceComputes divergence of a flux vector provided by a material.
• ADMatBodyForceKernel that defines a body force modified by a material property
• ADMatCoupledForceKernel representing the contribution of the PDE term , where is a material property coefficient, is a coupled scalar field variable, and Jacobian derivatives are calculated using automatic differentiation.
• ADMatDiffusionDiffusion equation Kernel that takes an isotropic Diffusivity from a material property
• ADMatReactionKernel to add -L*v, where L=reaction rate, v=variable
• ADMaterialPropertyValueResidual term (u - prop) to set variable u equal to a given material property prop
• ADReactionImplements a simple consuming reaction term with weak form .
• ADScalarLMKernelThis class is used to enforce integral of phi = V_0 with a Lagrange multiplier approach.
• ADScaledCoupledTimeDerivativeExtension of the ADCoupledTimeDerivative kernel that calculates the time derivative of a coupled variable scaled by a material property.
• ADTimeDerivativeThe time derivative operator with the weak form of .
• ADVectorDiffusionThe Laplacian operator (), with the weak form of . The Jacobian is computed using automatic differentiation
• ADVectorTimeDerivativeThe time derivative operator with the weak form of .
• AnisotropicDiffusionAnisotropic diffusion kernel with weak form given by .
• ArrayBodyForceApplies body forces specified with functions to an array variable.
• ArrayCoupledForceImplements a source term proportional to the value of a coupled standard or array variable. Weak form: .
• ArrayCoupledTimeDerivativeTime derivative Array Kernel that acts on a coupled variable. Weak form: . The coupled variable and the variable must have the same dimensionality
• ArrayDiffusionThe array Laplacian operator (), with the weak form of .
• ArrayReactionThe array reaction operator with the weak form of .
• ArrayTimeDerivativeArray time derivative operator with the weak form of .
• BodyForceDemonstrates the multiple ways that scalar values can be introduced into kernels, e.g. (controllable) constants, functions, and postprocessors. Implements the weak form .
• CoefReactionImplements the residual term (p*u, test)
• CoefTimeDerivativeThe time derivative operator with the weak form of .
• ConservativeAdvectionConservative form of which in its weak form is given by: . Velocity can be given as 1) a variable, for which the gradient is automatically taken, 2) a vector variable, or a 3) vector material.
• CoupledForceImplements a source term proportional to the value of a coupled variable. Weak form: .
• CoupledTimeDerivativeTime derivative Kernel that acts on a coupled variable. Weak form: .
• DiffusionThe Laplacian operator (), with the weak form of .
• DivDivFieldThe grad-div operator optionally scaled by a constant scalar coefficient.Weak form: .
• DivFieldThe divergence operator optionally scaled by a constant scalar coefficient. Weak form: .
• FunctionDiffusionDiffusion with a function coefficient.
• FunctorKernelAdds a term from a functor.
• GradFieldThe gradient operator optionally scaled by a constant scalar coefficient. Weak form: .
• MassEigenKernelAn eigenkernel with weak form where is the eigenvalue.
• MassLumpedTimeDerivativeLumped formulation of the time derivative . Its corresponding weak form is where denotes the time derivative of the solution coefficient associated with node .
• MassMatrixComputes a finite element mass matrix
• MatBodyForceKernel that defines a body force modified by a material property
• MatCoupledForceImplements a forcing term RHS of the form PDE = RHS, where RHS = Sum_j c_j * m_j * v_j. c_j, m_j, and v_j are provided as real coefficients, material properties, and coupled variables, respectively.
• MatDiffusionDiffusion equation Kernel that takes an isotropic Diffusivity from a material property
• MatReactionKernel to add -L*v, where L=reaction rate, v=variable
• MaterialDerivativeRankFourTestKernelClass used for testing derivatives of a rank four tensor material property.
• MaterialDerivativeRankTwoTestKernelClass used for testing derivatives of a rank two tensor material property.
• MaterialDerivativeTestKernelClass used for testing derivatives of a scalar material property.
• MaterialPropertyValueResidual term (u - prop) to set variable u equal to a given material property prop
• NullKernelKernel that sets a zero residual.
• ReactionImplements a simple consuming reaction term with weak form .
• ScalarLMKernelThis class is used to enforce integral of phi = V_0 with a Lagrange multiplier approach.
• ScalarLagrangeMultiplierThis class is used to enforce integral of phi = V_0 with a Lagrange multiplier approach.
• TimeDerivativeThe time derivative operator with the weak form of .
• UserForcingFunctionDemonstrates the multiple ways that scalar values can be introduced into kernels, e.g. (controllable) constants, functions, and postprocessors. Implements the weak form .
• VectorBodyForceDemonstrates the multiple ways that scalar values can be introduced into kernels, e.g. (controllable) constants, functions, and postprocessors. Implements the weak form .
• VectorCoupledTimeDerivativeTime derivative Kernel that acts on a coupled vector variable. Weak form: .
• VectorDiffusionThe Laplacian operator (), with the weak form of .
• VectorFunctionReactionKernel representing the contribution of the PDE term , where is a function coefficient and is a vector variable.
• VectorTimeDerivativeThe time derivative operator with the weak form of .
• Electromagnetics App
• ADConductionCurrentCalculates the current source term in the Helmholtz wave equation using the conduction formulation of the current.
• ADCurlCurlFieldWeak form term corresponding to .
• ADMatWaveReactionCalculates the current source term in the Helmholtz wave equation using the dielectric formulation of the current.
• CurlCurlFieldWeak form term corresponding to .
• EMJouleHeatingSourceSupplies the heating due to the electic field in the form of
• VectorCurrentSourceKernel to calculate the current source term in the Helmholtz wave equation.
• VectorSecondTimeDerivativeThe second time derivative operator for vector variables.
• Ferret App
• AFDWall2EnergyDerivative
• AFDWallEnergyDerivative
• AFMEasyPlaneAnisotropyCalculates a residual contribution for the magnetic anisotropy energy.
• AFMEasyPlaneAnisotropySCCalculates a residual contribution for the magnetic anisotropy energy.
• AFMHomogeneousSublatticeExchangeCalculates a residual contribution for the sublattice exchange in an antiferromagnet
• AFMInteractionCartLLCalculates a residual contribution for the sublattice exchange in an antiferromagnet
• AFMInteractionCartLLHConstCalculates a residual contribution for the sublattice exchange in an antiferromagnet
• AFMLocalSublatticeExchangeCartLLCalculates a residual contribution for the magnetic exchange energy.
• AFMSingleIonCubicSixthAnisotropyCalculates a residual contribution for the magnetic anisotropy energy.
• AFMSingleIonCubicSixthAnisotropySCCalculates a residual contribution for the magnetic anisotropy energy.
• AFMSublatticeAnisotropyCalculates a residual contribution for the magnetic anisotropy energy.
• AFMSublatticeDMInteractionCalculates a residual contribution for the DMI interaction on an AFM sublattice that supports such a thing
• AFMSublatticeDMInteractionSCCalculates a residual contribution for the DMI interaction on an AFM sublattice that supports such a thing
• AFMSublatticeSuperexchangeCalculates a residual contribution for the sublattice exchange in an antiferromagnet
• AnisotropicElectrostaticsCalculates a residual contribution due to nabla squared Phi = 0
• AnisotropyCartLLCalculates a residual contribution for the magnetic anisotropy energy.
• BulkEnergyDerivativeEighthCalculates the residual for the local free energy which is an eighth order expansion in the polarization.
• BulkEnergyDerivativeSixthCalculates the residual for the local free energy which is an sixth order expansion in the polarization.
• BulkEnergyDerivativeSixthCoupledTCalculates the residual for the local free energy which is an sixth order expansion in the polarization coupled to the thermal field through the first Landau coefficient.
• ConstFieldThis is just a test kernel. It is a residual contribution due to a constant electric field term along the z-direction of polarization
• ConversePiezoelectricStrainCalculates the residual for additional piezoelectric strain arising in the conditions for mechanical equilibrium.
• CorrectedElectrostrictiveCouplingPolarDerivativeCalculates a residual contribution due to the variation w.r.t polarization of the electrostrictive coupling energy. Note: for cubic parent phase only.
• CubicAnisotropyCartLLGLLG torque from cubic magnetocrystalline anisotropy, F = Kc1 (mx^{2 my}2 + my^{2 mz}2 + mz^{2 mx}2), single lattice.
• CubicParentElasticADerivativeCalculates a residual contribution due to the variation w.r.t antiphase tilt of the rotostrictive coupling energy. Note: for cubic parent phase only.
• CubicParentElasticPDerivativeCalculates a residual contribution due to the variation w.r.t polarization of the electrostrictive coupling energy. Note: for cubic parent phase only.
• DivCurrentVCalculates a residual contribution due to modified ohm's law
• ElectrostaticsCalculates a residual contribution due to div*Phi = 0
• ElectrostrictiveCouplingDispDerivativeCalculates a residual contribution due to the spontaneous ferroelectric strain in the condition for mechanical equilibrium.
• ElectrostrictiveCouplingPolarDerivativeCalculates a residual contribution due to the variation w.r.t polarization of the electrostrictive coupling energy. Note: for cubic parent phase only.
• ExchangeCartLLCalculates a residual contribution due to the magnetic exchange energy.
• FluctuationKernelCalculates a residual contribution introducing fluctuations useful in quasi-static hysteretic switching.
• HeatFlowElectricTCalculates a residual contribution due to modified ohm's law
• InPlaneSusceptibilityDerivativeCalculates the residual for the local free energy which is an eighth order expansion in the polarization.
• InteractionCartLLCalculates a residual contribution - MH in the total energy, assuming H = - div * potential.
• LocalConservedLangevinNoiseSource term for noise from a ConservedNoise userobject
• LocalLangevinNoiseSource term for non-conserved Langevin noise
• LongitudinalLLBCalculates a residual contribution for the magnetic anisotropy energy.
• MagHStrongCartCalculates a residual contribution for bound magnetic charge (div M)
• MagHStrongSublatticesCartCalculates a residual contribution for bound magnetic charge (div M1 + div M2)
• MagneticPMLCartCalculates a residual contribution to Laplacian in a stretched region
• MagnetostrictiveCouplingCubicHeffCalculates a residual contribution due to the magnetoelectric effective field. Note for cubic magnets only.
• MagnetostrictiveCouplingDispDerivativeCalculates a residual contribution due to the differentiation w.r.t spartial coordinates of the magnetoelastic self-strain in the condition for mechanical equilibrium. Note for cubic magnets only.
• MasterAnisotropyCartLLGCalculates a residual contribution for the magnetic anisotropy energy.
• MasterExchangeCartLLGCalculates a residual contribution due to the magnetic exchange energy.
• MasterInteractionCartLLGCalculates the Rij contribution (due to energy -M*H), assuming H = - div*Phi.
• MasterInteractionCartLLGHConstCalculates a residual contribution - MH in the total energy, assuming H = - div * potential.
• MasterLongitudinalLLBCalculates a residual contribution for the magnetic anisotropy energy.
• PiezoelectricStrainChargeCalculates a residual contribution due to a charge arising via piezoelectric coupling in the Poisson equation.
• PolarElectricEStrongCalculates a residual contribution due to divP (to be used with the electrostatics (Laplace) kernel).
• PolarElectricPStrongCalculates a residual contribution due to -PE term in the total energy.
• PolarElectricPStrongEConstCalculates a residual contribution due to -PE term in the total energy.
• RotatedBulkEnergyDerivativeSixthCalculates the residual for the local free energy which is an sixth order expansion in the polarization.
• RotoBulkEnergyDerivativeEighthAlt
• RotoPolarCoupledEnergyDistortDerivativeAlt
• RotoPolarCoupledEnergyPolarDerivativeAlt
• RotostrictiveCouplingDispDerivative
• RotostrictiveCouplingDistortDerivative
• SecondTimeDerivativeScaled
• SeebeckEffectCalculates a contribution due to nabla.j = 0
• TensorDivCurrentVCalculates a residual contribution due to modified ohm's law
• TensorHeatFlowElectricTCalculates a residual contribution due to modified ohm's law
• ThermalDiffusionCalculates a residual contribution due to ∇(k∇*T) = 0
• TimeDerivativeScaled
• UniaxialAFMSublatticeCalculates a residual contribution for an uniaxial AFM sublattice
• Wall2EnergyDerivativeCalculates a residual contribution due to the variation w.r.t polarization of the gradient energy. This Kernel should be used in conjunction with WallEnergyDerivative!
• WallEnergyDerivativeCalculates a residual contribution due to the variation w.r.t polarization of the gradient energy. This Kernel should be used in conjunction with Wall2EnergyDerivative!
• Misc App
• ADThermoDiffusionCalculates diffusion due to temperature gradient and Soret Coefficient
• CoefDiffusionKernel for diffusion with diffusivity = coef + function
• ThermoDiffusionKernel for thermo-diffusion (Soret effect, thermophoresis, etc.)
• Phase Field App
• ACBarrierFunctionAllen-Cahn kernel used when 'mu' is a function of variables
• ACGBPolyGrain-Boundary model concentration dependent residual
• ACGrGrElasticDrivingForceAdds elastic energy contribution to the Allen-Cahn equation
• ACGrGrMultiMulti-phase poly-crystalline Allen-Cahn Kernel
• ACGrGrPolyGrain-Boundary model poly-crystalline interface Allen-Cahn Kernel
• ACGrGrPolyLinearizedInterfaceGrain growth model Allen-Cahn Kernel with linearized interface variable transformation
• ACInterfaceGradient energy Allen-Cahn Kernel
• ACInterface2DMultiPhase1Gradient energy Allen-Cahn Kernel where the derivative of interface parameter kappa wrt the gradient of order parameter is considered.
• ACInterface2DMultiPhase2Gradient energy Allen-Cahn Kernel where the interface parameter kappa is considered.
• ACInterfaceChangedVariableGradient energy Allen-Cahn Kernel using a change of variable
• ACInterfaceCleavageFractureGradient energy Allen-Cahn Kernel where crack propagation along weakcleavage plane is preferred
• ACInterfaceKobayashi1Anisotropic gradient energy Allen-Cahn Kernel Part 1
• ACInterfaceKobayashi2Anisotropic Gradient energy Allen-Cahn Kernel Part 2
• ACInterfaceStressInterface stress driving force Allen-Cahn Kernel
• ACKappaFunctionGradient energy term for when kappa as a function of the variable
• ACMultiInterfaceGradient energy Allen-Cahn Kernel with cross terms
• ACSEDGPolyStored Energy contribution to grain growth
• ACSwitchingKernel for Allen-Cahn equation that adds derivatives of switching functions and energies
• ADACBarrierFunctionAllen-Cahn kernel used when 'mu' is a function of variables
• ADACGrGrMultiMulti-phase poly-crystalline Allen-Cahn Kernel
• ADACInterfaceGradient energy Allen-Cahn Kernel
• ADACInterfaceKobayashi1Anisotropic gradient energy Allen-Cahn Kernel Part 1
• ADACInterfaceKobayashi2Anisotropic Gradient energy Allen-Cahn Kernel Part 2
• ADACKappaFunctionGradient energy term for when kappa as a function of the variable
• ADACSwitchingKernel for Allen-Cahn equation that adds derivatives of switching functions and energies
• ADAllenCahnAllen-Cahn Kernel that uses a DerivativeMaterial Free Energy
• ADCHSoretMobilityAdds contribution due to thermo-migration to the Cahn-Hilliard equation using a concentration 'u', temperature 'T', and thermal mobility 'mobility' (in units of length squared per time).
• ADCHSplitChemicalPotentialChemical potential kernel in Split Cahn-Hilliard that solves chemical potential in a weak form
• ADCHSplitConcentrationConcentration kernel in Split Cahn-Hilliard that solves chemical potential in a weak form
• ADCoefCoupledTimeDerivativeScaled time derivative Kernel that acts on a coupled variable
• ADCoupledSwitchingTimeDerivativeCoupled time derivative Kernel that multiplies the time derivative by
• ADGrainGrowthGrain-Boundary model poly-crystalline interface Allen-Cahn Kernel
• ADLaplacianSplitSplit with a variable that holds the Laplacian of a phase field variable.
• ADMatAnisoDiffusionDiffusion equation Kernel that takes an anisotropic Diffusivity from a material property
• ADPhaseFieldAdvectionImplements the phasefield advection equation: , where the weak form is .
• ADPhaseFieldAdvectionSUPGSUPG stablization term for the advection portion of the level set equation.
• ADPhaseFieldCoupledDoubleWellPotentialDouble well potential for Cahn-Hilliard advection.
• ADPhaseFieldForcingFunctionSUPGThe SUPG stablization term for a forcing function.
• ADPhaseFieldTimeDerivativeSUPGSUPG stablization terms for the time derivative of the level set equation.
• ADPhaseFieldTwoPhaseSurfaceTensionPhase field surface tension force for the Navier-Stokes equations.
• ADPrefactorLaplacianSplitLaplacian split with a prefactor.
• ADSplitCHParsedSplit formulation Cahn-Hilliard Kernel that uses a DerivativeMaterial Free Energy
• ADSplitCHWResSplit formulation Cahn-Hilliard Kernel for the chemical potential variable with a scalar (isotropic) mobility
• ADSplitCHWResAnisoSplit formulation Cahn-Hilliard Kernel for the chemical potential variable with a scalar (isotropic) mobility
• ADSusceptibilityTimeDerivativeA modified time derivative Kernel that multiplies the time derivative of a variable by a generalized susceptibility
• AllenCahnAllen-Cahn Kernel that uses a DerivativeMaterial Free Energy
• AllenCahnElasticEnergyOffDiagThis kernel calculates off-diagonal Jacobian of elastic energy in AllenCahn with respect to displacements
• AntitrappingCurrentKernel that provides antitrapping current at the interface for alloy solidification
• CHBulkPFCTradCahn-Hilliard kernel for a polynomial phase field crystal free energy.
• CHInterfaceGradient energy Cahn-Hilliard Kernel with a scalar (isotropic) mobility
• CHInterfaceAnisoGradient energy Cahn-Hilliard Kernel with a tensor (anisotropic) mobility
• CHMathSimple demonstration Cahn-Hilliard Kernel using an algebraic double-well potential
• CHPFCRFFCahn-Hilliard residual for the RFF form of the phase field crystal model
• CHSplitChemicalPotentialChemical potential kernel in Split Cahn-Hilliard that solves chemical potential in a weak form
• CHSplitConcentrationConcentration kernel in Split Cahn-Hilliard that solves chemical potential in a weak form
• CHSplitFluxComputes flux as nodal variable
• CahnHilliardCahn-Hilliard Kernel that uses a DerivativeMaterial Free Energy and a scalar (isotropic) mobility
• CahnHilliardAnisoCahn-Hilliard Kernel that uses a DerivativeMaterial Free Energy and a tensor (anisotropic) mobility
• ChangedVariableTimeDerivativeA modified time derivative Kernel that multiplies the time derivative bythe derivative of the nonlinear preconditioning function
• CoefCoupledTimeDerivativeScaled time derivative Kernel that acts on a coupled variable
• ConservedLangevinNoiseSource term for noise from a ConservedNoise userobject
• CoupledAllenCahnCoupled Allen-Cahn Kernel that uses a DerivativeMaterial Free Energy
• CoupledMaterialDerivativeKernel that implements the first derivative of a function material property with respect to a coupled variable.
• CoupledSusceptibilityTimeDerivativeA modified coupled time derivative Kernel that multiplies the time derivative of a coupled variable by a generalized susceptibility
• CoupledSwitchingTimeDerivativeCoupled time derivative Kernel that multiplies the time derivative by
• DiscreteNucleationForceTerm for inserting grain nuclei or phases in non-conserved order parameter fields
• DoubleWellPotentialSimple demonstration Allen-Cahn Kernel using an algebraic double-well potential
• GradientComponentSet the kernel variable to a specified component of the gradient of a coupled variable.
• HHPFCRFFReaction type kernel for the RFF phase fit crystal model
• KKSACBulkCKKS model kernel (part 2 of 2) for the Bulk Allen-Cahn. This includes all terms dependent on chemical potential.
• KKSACBulkFKKS model kernel (part 1 of 2) for the Bulk Allen-Cahn. This includes all terms NOT dependent on chemical potential.
• KKSCHBulkKKS model kernel for the Bulk Cahn-Hilliard term. This operates on the concentration 'c' as the non-linear variable
• KKSMultiACBulkCMulti-phase KKS model kernel (part 2 of 2) for the Bulk Allen-Cahn. This includes all terms dependent on chemical potential.
• KKSMultiACBulkFKKS model kernel (part 1 of 2) for the Bulk Allen-Cahn. This includes all terms NOT dependent on chemical potential.
• KKSMultiPhaseConcentrationKKS multi-phase model kernel to enforce . The non-linear variable of this kernel is , the final phase concentration in the list.
• KKSPhaseChemicalPotentialKKS model kernel to enforce the pointwise equality of phase chemical potentials . The non-linear variable of this kernel is .
• KKSPhaseConcentrationKKS model kernel to enforce the decomposition of concentration into phase concentration . The non-linear variable of this kernel is .
• KKSSplitCHCResKKS model kernel for the split Bulk Cahn-Hilliard term. This kernel operates on the physical concentration 'c' as the non-linear variable
• LangevinNoiseSource term for non-conserved Langevin noise
• LaplacianSplitSplit with a variable that holds the Laplacian of a phase field variable.
• MaskedBodyForceCustomization of MatBodForce which uses a material property, scalar, and/or postprocessor to provide a source term PDE contribution.
• MaskedExponentialKernel to add dilute solution term to Poisson's equation for electrochemical sintering
• MatAnisoDiffusionDiffusion equation Kernel that takes an anisotropic Diffusivity from a material property
• MatGradSquareCoupledGradient square of a coupled variable.
• MultiGrainRigidBodyMotionAdds rigid body motion to grains
• NestedKKSACBulkCKKS model kernel (part 2 of 2) for the Bulk Allen-Cahn. This includes all terms dependent on chemical potential.
• NestedKKSACBulkFKKS model kernel (part 1 of 2) for the Bulk Allen-Cahn. This includes all terms NOT dependent on chemical potential.
• NestedKKSMultiACBulkCMulti-phase KKS model kernel (part 2 of 2) for the Bulk Allen-Cahn. This includes all terms dependent on chemical potential.
• NestedKKSMultiACBulkFKKS model kernel (part 1 of 2) for the Bulk Allen-Cahn. This includes all terms NOT dependent on chemical potential.
• NestedKKSMultiSplitCHCResKKS model kernel for the split Bulk Cahn-Hilliard term. This kernel operates on the physical concentration 'c' as the non-linear variable.
• NestedKKSSplitCHCResKKS model kernel for the split Bulk Cahn-Hilliard term. This kernel operates on the physical concentration 'c' as the non-linear variable.
• PolycrystalMatAnisoDiffusionDiffusion equation Kernel that takes an anisotropic Diffusivity from a material property
• PolycrystalMatDiffusionDiffusion equation Kernel that takes an isotropic Diffusivity from a material property
• SLKKSChemicalPotentialSLKKS model kernel to enforce the pointwise equality of sublattice chemical potentials in the same phase.
• SLKKSMultiACBulkCMulti-phase SLKKS model kernel for the bulk Allen-Cahn. This includes all terms dependent on chemical potential.
• SLKKSMultiPhaseConcentrationSLKKS multi-phase model kernel to enforce . The non-linear variable of this kernel is a phase's sublattice concentration
• SLKKSPhaseConcentrationSublattice KKS model kernel to enforce the decomposition of concentration into phase and sublattice concentrations The non-linear variable of this kernel is a sublattice concentration of phase b.
• SLKKSSumEnforce the sum of sublattice concentrations to a given phase concentration.
• SimpleACInterfaceGradient energy for Allen-Cahn Kernel with constant Mobility and Interfacial parameter
• SimpleCHInterfaceGradient energy for Cahn-Hilliard equation with constant Mobility and Interfacial parameter
• SimpleCoupledACInterfaceGradient energy for Allen-Cahn Kernel with constant Mobility and Interfacial parameter for a coupled order parameter variable.
• SimpleSplitCHWResGradient energy for split Cahn-Hilliard equation with constant Mobility for a coupled order parameter variable.
• SingleGrainRigidBodyMotionAdds rigid mody motion to a single grain
• SoretDiffusionAdd Soret effect to Split formulation Cahn-Hilliard Kernel
• SplitCHMathSimple demonstration split formulation Cahn-Hilliard Kernel using an algebraic double-well potential
• SplitCHParsedSplit formulation Cahn-Hilliard Kernel that uses a DerivativeMaterial Free Energy
• SplitCHWResSplit formulation Cahn-Hilliard Kernel for the chemical potential variable with a scalar (isotropic) mobility
• SplitCHWResAnisoSplit formulation Cahn-Hilliard Kernel for the chemical potential variable with a tensor (anisotropic) mobility
• SusceptibilityTimeDerivativeA modified time derivative Kernel that multiplies the time derivative of a variable by a generalized susceptibility
• SwitchingFunctionConstraintEtaLagrange multiplier kernel to constrain the sum of all switching functions in a multiphase system. This kernel acts on a non-conserved order parameter eta_i.
• SwitchingFunctionConstraintLagrangeLagrange multiplier kernel to constrain the sum of all switching functions in a multiphase system. This kernel acts on the Lagrange multiplier variable.
• SwitchingFunctionPenaltyPenalty kernel to constrain the sum of all switching functions in a multiphase system.
• CHPFCRFFSplitKernel
• HHPFCRFFSplitKernel
• PFCRFFKernel
• PolycrystalElasticDrivingForce
• PolycrystalKernel
• PolycrystalStoredEnergy
• RigidBodyMultiKernel
• Solid Mechanics App
• ADDistributedLoadShellApplies a distributed load (specified in units of force per area) on the shell plane in a given direction (e.g. self_weight, wind load) or normal to the shell plan (e.g. pressure loads)
• ADDynamicStressDivergenceTensorsResidual due to stress related Rayleigh damping and HHT time integration terms
• ADGeneralizedPlaneStrainAssembles the integrated out-of-plane stress to the scalar residual for generalized plane strain using automatic differentiation.
• ADGravityApply gravity. Value is in units of acceleration.
• ADInertialForceCalculates the residual for the inertial force () and the contribution of mass dependent Rayleigh damping and HHT time integration scheme ($\eta \cdot M \cdot ((1+\alpha)velq2-\alpha \cdot vel-old) $)
• ADInertialForceShellCalculates the residual for the inertial force/moment and the contribution of mass dependent Rayleigh damping and HHT time integration scheme.
• ADStressDivergenceRSphericalTensorsCalculate stress divergence for a spherically symmetric 1D problem in polar coordinates.
• ADStressDivergenceRZTensorsCalculate stress divergence for an axisymmetric problem in cylindrical coordinates.
• ADStressDivergenceShellQuasi-static stress divergence kernel for Shell element
• ADStressDivergenceTensorsStress divergence kernel with automatic differentiation for the Cartesian coordinate system
• ADSymmetricStressDivergenceTensorsStress divergence kernel with automatic differentiation for the Cartesian coordinate system
• ADWeakPlaneStressPlane stress kernel to provide out-of-plane strain contribution.
• AsymptoticExpansionHomogenizationKernelKernel for asymptotic expansion homogenization for elasticity
• CosseratStressDivergenceTensorsStress divergence tensor with the additional Jacobian terms for the Cosserat rotation variables.
• DynamicStressDivergenceTensorsResidual due to stress related Rayleigh damping and HHT time integration terms
• GeneralizedPlaneStrainOffDiagGeneralized Plane Strain kernel to provide contribution of the out-of-plane strain to other kernels
• GravityApply gravity. Value is in units of acceleration.
• HomogenizedTotalLagrangianStressDivergenceTotal Lagrangian stress equilibrium kernel with homogenization constraint Jacobian terms
• InertialForceCalculates the residual for the inertial force () and the contribution of mass dependent Rayleigh damping and HHT time integration scheme ($\eta \cdot M \cdot ((1+\alpha)velq2-\alpha \cdot vel-old) $)
• InertialForceBeamCalculates the residual for the inertial force/moment and the contribution of mass dependent Rayleigh damping and HHT time integration scheme.
• InertialTorqueKernel for inertial torque: density * displacement x acceleration
• MaterialVectorBodyForceApply a body force vector to the coupled displacement component.
• MomentBalancingBalance of momentum for three-dimensional Cosserat media, notably in a Cosserat layered elasticity model.
• OutOfPlanePressureApply pressure in the out-of-plane direction in 2D plane stress or generalized plane strain models
• PhaseFieldFractureMechanicsOffDiagStress divergence kernel for phase-field fracture: Computes off diagonal damage dependent Jacobian components. To be used with StressDivergenceTensors or DynamicStressDivergenceTensors.
• PlasticHeatEnergyPlastic heat energy density = coeff * stress * plastic_strain_rate
• PoroMechanicsCouplingAdds , where the subscript is the component.
• StressDivergenceBeamQuasi-static and dynamic stress divergence kernel for Beam element
• StressDivergenceRSphericalTensorsCalculate stress divergence for a spherically symmetric 1D problem in polar coordinates.
• StressDivergenceRZTensorsCalculate stress divergence for an axisymmetric problem in cylindrical coordinates.
• StressDivergenceTensorsStress divergence kernel for the Cartesian coordinate system
• StressDivergenceTensorsTrussKernel for truss element
• TotalLagrangianStressDivergenceEnforce equilibrium with a total Lagrangian formulation in Cartesian coordinates.
• TotalLagrangianStressDivergenceAxisymmetricCylindricalEnforce equilibrium with a total Lagrangian formulation in axisymmetric cylindrical coordinates.
• TotalLagrangianStressDivergenceCentrosymmetricSphericalEnforce equilibrium with a total Lagrangian formulation in centrosymmetric spherical coordinates.
• TotalLagrangianWeakPlaneStressPlane stress kernel to provide out-of-plane strain contribution.
• UpdatedLagrangianStressDivergenceEnforce equilibrium with an updated Lagrangian formulation in Cartesian coordinates.
• WeakPlaneStressPlane stress kernel to provide out-of-plane strain contribution.
• DynamicSolidMechanics
• DynamicTensorMechanics
• PoroMechanics
• SolidMechanics
• TensorMechanics

LinearFVBCs

• Moose App
• AddLinearFVBCActionAdd a LinearFVBoundaryCondition object to the simulation.
• LinearFVAdvectionDiffusionExtrapolatedBCAdds a boundary condition which calculates the face values and face gradients assuming one or two term expansions from the cell centroid. This kernel is only compatible with advection-diffusion problems.
• LinearFVAdvectionDiffusionFunctorDirichletBCAdds a dirichlet BC which can be used for the assembly of linear finite volume system and whose face values are determined using a functor. This kernel is only designed to work with advection-diffusion problems.
• LinearFVAdvectionDiffusionFunctorNeumannBCAdds a fixed diffusive flux BC which can be used for the assembly of linear finite volume system and whose normal face gradient values are determined using a functor. This kernel is only designed to work with advection-diffusion problems.
• LinearFVAdvectionDiffusionFunctorRobinBCAdds a Robin BC of the form \alpha * \nabla \phi*n + \beta * \phi = \gamma, which can be used for the assembly of linear finite volume system and whose face values are determined using three functors. This kernel is only designed to work with advection-diffusion problems.
• LinearFVAdvectionDiffusionOutflowBCAdds a boundary condition which represents a surface with outflowing material with a constant velocity. This kernel is only compatible with advection-diffusion problems.
• LinearFVAdvectionDiffusionScalarSymmetryBCAdds a symmetry boundary condition for a scalar quantity.
• LinearFVAnisotropicDiffusionFunctorNeumannBCAdds a prescribed anisotropic diffusive flux boundary condition to a linear finite volume system and reconstructs the boundary value using a diagonal diffusion tensor.

LinearFVKernels

• Moose App
• AddLinearFVKernelActionAdd a LinearFVKernel object to the simulation.
• LinearFVAdvectionRepresents the matrix and right hand side contributions of an advection term in a partial differential equation.
• LinearFVAnisotropicDiffusionRepresents the matrix and right hand side contributions of a diffusion term in a partial differential equation.
• LinearFVDiffusionRepresents the matrix and right hand side contributions of a diffusion term in a partial differential equation.
• LinearFVReactionRepresents the matrix and right hand side contributions of a reaction term () in a partial differential equation.
• LinearFVSourceRepresents the matrix and right hand side contributions of a solution-independent source term in a partial differential equation.
• LinearFVTimeDerivativeRepresents the matrix and right hand side contributions of a time derivative term in a partial differential equation.

Materials

• Moose App
• AddMaterialActionAdd a Material object to the simulation.
• ADCoupledGradientMaterialCreates a gradient material equal to the gradient of the coupled variable times a scalar material property.
• ADCoupledValueFunctionMaterialCompute a function value from coupled variables
• ADDerivativeParsedMaterialParsed Function Material with automatic derivatives.
• ADDerivativeSumMaterialMeta-material to sum up multiple derivative materials
• ADFluxFromGradientMaterialComputes a flux vector material property based on the gradient of a coupled variable and a scalar diffusivity.
• ADGenericConstant2DArrayA material evaluating one material property in type of RealEigenMatrix
• ADGenericConstantMaterialDeclares material properties based on names and values prescribed by input parameters.
• ADGenericConstantRankTwoTensorObject for declaring a constant rank two tensor as a material property.
• ADGenericConstantRealVectorValueObject for declaring a constant 3-vector as a material property.
• ADGenericConstantStdVectorMaterialDeclares material properties based on names and vector values prescribed by input parameters.
• ADGenericConstantSymmetricRankTwoTensorObject for declaring a constant symmetric rank two tensor as a material property.
• ADGenericConstantVectorMaterialDeclares material properties based on names and vector values prescribed by input parameters.
• ADGenericFunctionMaterialMaterial object for declaring properties that are populated by evaluation of Function object.
• ADGenericFunctionRankTwoTensorMaterial object for defining rank two tensor properties using functions.
• ADGenericFunctionVectorMaterialMaterial object for declaring vector properties that are populated by evaluation of Function objects.
• ADParsedMaterialParsed expression Material.
• ADPiecewiseConstantByBlockMaterialComputes a property value on a per-subdomain basis
• ADPiecewiseLinearInterpolationMaterialCompute a property using a piecewise linear interpolation to define its dependence on a variable
• ADVectorFromComponentVariablesMaterialComputes a vector material property from coupled variables
• CoupledGradientMaterialCreates a gradient material equal to the gradient of the coupled variable times a scalar material property.
• CoupledValueFunctionMaterialCompute a function value from coupled variables
• DerivativeParsedMaterialParsed Function Material with automatic derivatives.
• DerivativeSumMaterialMeta-material to sum up multiple derivative materials
• GenericConstant2DArrayA material evaluating one material property in type of RealEigenMatrix
• GenericConstantArrayA material evaluating one material property in type of RealEigenVector
• GenericConstantMaterialDeclares material properties based on names and values prescribed by input parameters.
• GenericConstantRankTwoTensorObject for declaring a constant rank two tensor as a material property.
• GenericConstantRealVectorValueObject for declaring a constant 3-vector as a material property.
• GenericConstantStdVectorMaterialDeclares material properties based on names and vector values prescribed by input parameters.
• GenericConstantSymmetricRankTwoTensorObject for declaring a constant symmetric rank two tensor as a material property.
• GenericConstantVectorMaterialDeclares material properties based on names and vector values prescribed by input parameters.
• GenericFunctionMaterialMaterial object for declaring properties that are populated by evaluation of Function object.
• GenericFunctionRankTwoTensorMaterial object for defining rank two tensor properties using functions.
• GenericFunctionVectorMaterialMaterial object for declaring vector properties that are populated by evaluation of Function objects.
• InterpolatedStatefulMaterialRankFourTensorAccess old state from projected data.
• InterpolatedStatefulMaterialRankTwoTensorAccess old state from projected data.
• InterpolatedStatefulMaterialRealAccess old state from projected data.
• InterpolatedStatefulMaterialRealVectorValueAccess old state from projected data.
• MaterialADConverterConverts regular material properties to AD properties and vice versa
• MaterialConverterConverts regular material properties to AD properties and vice versa
• MaterialFunctorConverterConverts functor to non-AD and AD regular material properties
• NEML2ToMOOSERankFourTensorMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type RankFourTensorTempl<double>.
• NEML2ToMOOSERankTwoTensorMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type RankTwoTensorTempl<double>.
• NEML2ToMOOSERealMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type double.
• NEML2ToMOOSERealVectorValueMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type libMesh::VectorValue<double>.
• NEML2ToMOOSESymmetricRankFourTensorMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type SymmetricRankFourTensorTempl<double>.
• NEML2ToMOOSESymmetricRankTwoTensorMaterialPropertyProvide an output (or its derivative) from a NEML2 model as a MOOSE material property of type SymmetricRankTwoTensorTempl<double>.
• ParsedMaterialParsed expression Material.
• PiecewiseConstantByBlockMaterialComputes a property value on a per-subdomain basis
• PiecewiseLinearInterpolationMaterialCompute a property using a piecewise linear interpolation to define its dependence on a variable
• RankFourTensorMaterialADConverterConverts regular material properties to AD properties and vice versa
• RankFourTensorMaterialConverterConverts regular material properties to AD properties and vice versa
• RankTwoTensorFromComponentPropertiesAssembles a RankTwoTensor from scalar material properties or constants
• RankTwoTensorMaterialADConverterConverts regular material properties to AD properties and vice versa
• RankTwoTensorMaterialConverterConverts regular material properties to AD properties and vice versa
• VectorFromComponentVariablesMaterialComputes a vector material property from coupled variables
• VectorMaterialFunctorConverterConverts functor to non-AD and AD regular material properties
• Electromagnetics App
• WaveEquationCoefficientMaterial for use as coefficient (where a is a scalar coefficient) in standard-form Helmholtz wave equation applications with derivatives calculated using automatic differentiation.
• Ferret App
• ADThermoelectricMaterialGeneral-purpose material model for thermoelectrics
• ComputeCubicParentElectrostrictiveStrainCompute the spontaneous polar contribution to the strain.
• ComputeDeltaIndicatrixCompute the adjustments to the indicatrix (beta tensor).
• ComputeDeltaIndicatrixElectroCompute the adjustments to the indicatrix (beta tensor).
• ComputeElastoopticTensorCompute a photostrictive tensor.
• ComputeElectricalConductivityTDepTensorStore a temperature dependent electrical conductivity tensor.
• ComputeElectricalConductivityTensorStore an electric conductivity tensor
• ComputeElectroopticTensorCompute an electrooptic tensor.
• ComputeElectrostrictiveTensorCompute an electrostrictive tensor.
• ComputeFerroelectricStrainCompute the spontaneous polar contribution to the strain.
• ComputeGCoeffTensorCompute a polar-optic (g) tensor.
• ComputeIndicatrixCompute the impermeability tensor, or indicatrix.
• ComputePiezoTensorCompute the converse piezoelectric tensor.
• ComputePiezostrictiveTensorCompute a piezostrictive tensor.
• ComputePolarOpticGCoeffTensorCompute the adjustments to the indicatrix due to the polar-optic effect with gijkl coefficients.
• ComputePolarOpticTensorCompute the adjustments to the indicatrix (beta tensor) due to the polar-optic effect.
• ComputeSeebeckTDepTensorCompute a Seebeck tensor.
• ComputeSeebeckTensorCompute a Seebeck tensor.
• ComputeSpontaneousRotostrictiveStrainCompute the rotostrictive contributuon to the spontaneous strain.
• ComputeThermalConductivityTDepTensorCompute a ThermalConductivity tensor.
• ComputeThermalConductivityTensorCompute a ThermalConductivity tensor.
• ThermoelectricMaterialGeneral-purpose material model for thermoelectrics
• Misc App
• ADArrheniusMaterialPropertyArbitrary material property of the sum of an arbitary number () of Arrhenius functions , where is the frequency factor, is the activation energy, and is the gas constant.
• ADDensityCreates density material property. This class is deprecated, and its functionalityis replaced by StrainAdjustedDensity for cases when the density should be adjustedto account for material deformation. If it is not desired to adjust the density fordeformation, a variety of general-purpose Materials, such as GenericConstantMaterialor ParsedMaterial can be used to define the density. A StrainAdjustedDensity can also be used with '0 0 0' for the displacements.
• ArrheniusMaterialPropertyArbitrary material property of the sum of an arbitary number () of Arrhenius functions , where is the frequency factor, is the activation energy, and is the gas constant.
• DensityCreates density material property. This class is deprecated, and its functionalityis replaced by StrainAdjustedDensity for cases when the density should be adjustedto account for material deformation. If it is not desired to adjust the density fordeformation, a variety of general-purpose Materials, such as GenericConstantMaterialor ParsedMaterial can be used to define the density. A StrainAdjustedDensity can also be used with '0 0 0' for the displacements.
• Phase Field App
• ADConstantAnisotropicMobilityProvide a constant mobility tensor value
• ADGBEvolutionComputes necessary material properties for the isotropic grain growth model
• ADInterfaceOrientationMaterial2D interfacial anisotropy
• ADMathCTDFreeEnergyMaterial that implements the math free energy using the expression builder and automatic differentiation
• ADMathFreeEnergyMaterial that implements the math free energy and its derivatives:
• ADPhaseFieldTwoPhaseMaterialMaterial that assigns properties based on the phase field variable.
• ADSwitchingFunctionMultiPhaseMaterialCalculates the switching function for a given phase for a multi-phase, multi-order parameter model
• AsymmetricCrossTermBarrierFunctionMaterialFree energy contribution asymmetric across interfaces between arbitrary pairs of phases.
• BarrierFunctionMaterialHelper material to provide and its derivative in a polynomial. SIMPLE: LOW: HIGH:
• CompositeMobilityTensorAssemble a mobility tensor from multiple tensor contributions weighted by material properties
• ComputeGBMisorientationTypeCalculate types of grain boundaries in a polycrystalline sample
• ComputePolycrystalElasticityTensorCompute an evolving elasticity tensor coupled to a grain growth phase field model.
• ConstantAnisotropicMobilityProvide a constant mobility tensor value
• CoupledValueFunctionFreeEnergyCompute a free energy from a lookup function
• CrossTermBarrierFunctionMaterialFree energy contribution symmetric across interfaces between arbitrary pairs of phases.
• DeformedGrainMaterialComputes scaled grain material properties
• DerivativeMultiPhaseMaterialTwo phase material that combines n phase materials using a switching function with and n non-conserved order parameters (to be used with SwitchingFunctionConstraint*).
• DerivativeTwoPhaseMaterialTwo phase material that combines two single phase materials using a switching function.
• DiscreteNucleationFree energy contribution for nucleating discrete particles
• ElasticEnergyMaterialFree energy material for the elastic energy contributions.
• ElectrochemicalDefectMaterialCalculates density, susceptibility, and derivatives for a defect species in the grand potential sintering model coupled with electrochemistry
• ElectrochemicalSinteringMaterialIncludes switching and thermodynamic properties for the grand potential sintering model coupled with electrochemistry
• ExternalForceDensityMaterialProviding external applied force density to grains
• ForceDensityMaterialCalculating the force density acting on a grain
• GBAnisotropyA material to compute anisotropic grain boundary energies and mobilities.
• GBDependentAnisotropicTensorCompute anisotropic rank two tensor based on GB phase variable
• GBDependentDiffusivityCompute diffusivity rank two tensor based on GB phase variable
• GBEvolutionComputes necessary material properties for the isotropic grain growth model
• GBWidthAnisotropyA material to compute anisotropic grain boundary energies and mobilities with user-specified grain boundary widths, independently for each interface between grains
• GrainAdvectionVelocityCalculation the advection velocity of grain due to rigid body translation and rotation
• GrandPotentialInterfaceCalculate Grand Potential interface parameters for a specified interfacial free energy and width
• GrandPotentialSinteringMaterialIncludes switching and thermodynamic properties for the grand potential sintering model
• GrandPotentialTensorMaterialDiffusion and mobility parameters for grand potential model governing equations. Uses a tensor diffusivity
• IdealGasFreeEnergyFree energy of an ideal gas.
• InterfaceNormalCurvaturesComputes the two normal curvatures kappa_1 and kappa_2 of a diffuse interface from an order parameter eta.
• InterfaceOrientationMaterial2D interfacial anisotropy
• InterfaceOrientationMultiphaseMaterialThis Material accounts for the the orientation dependence of interfacial energy for multi-phase multi-order parameter phase-field model.
• KKSPhaseConcentrationDerivativesComputes the KKS phase concentration derivatives wrt global concentrations and order parameters, which are used in the chain rules in the KKS kernels. This class is intended to be used with KKSPhaseConcentrationMaterial.
• KKSPhaseConcentrationMaterialComputes the KKS phase concentrations by using nested Newton iteration to solve the equal chemical potential and concentration conservation equations. This class is intended to be used with KKSPhaseConcentrationDerivatives.
• KKSPhaseConcentrationMultiPhaseDerivativesComputes the KKS phase concentration derivatives wrt global concentrations and order parameters, which are used for the chain rule in the KKS kernels. This class is intended to be used with KKSPhaseConcentrationMultiPhaseMaterial.
• KKSPhaseConcentrationMultiPhaseMaterialComputes the KKS phase concentrations by using a nested Newton iteration to solve the equal chemical potential and concentration conservation equations for multiphase systems. This class is intented to be used with KKSPhaseConcentrationMultiPhaseDerivatives.
• KKSXeVacSolidMaterialKKS Solid phase free energy for Xe,Vac in UO2. Fm(cmg,cmv)
• LinearizedInterfaceFunctionDefines the order parameter substitution for linearized interface phase field models
• MathCTDFreeEnergyMaterial that implements the math free energy using the expression builder and automatic differentiation
• MathEBFreeEnergyMaterial that implements the math free energy using the expression builder and automatic differentiation
• MathFreeEnergyMaterial that implements the math free energy and its derivatives:
• MixedSwitchingFunctionMaterialHelper material to provide h(eta) and its derivative in one of two polynomial forms. MIX234 and MIX246
• MultiBarrierFunctionMaterialDouble well phase transformation barrier free energy contribution.
• PFCRFFMaterialDefined the mobility, alpha and A constants for the RFF form of the phase field crystal model
• PFCTradMaterialPolynomial coefficients for a phase field crystal correlation function
• PFParamsPolyFreeEnergyPhase field parameters for polynomial free energy for single component systems
• PhaseNormalTensorCalculate normal tensor of a phase based on gradient
• PolycrystalDiffusivityGenerates a diffusion coefficient to distinguish between the bulk, pore, grain boundaries, and surfaces
• PolycrystalDiffusivityTensorBaseGenerates a diffusion tensor to distinguish between the bulk, grain boundaries, and surfaces
• PolynomialFreeEnergyPolynomial free energy for single component systems
• RegularSolutionFreeEnergyMaterial that implements the free energy of a regular solution
• StrainGradDispDerivativesProvide the constant derivatives of strain w.r.t. the displacement gradient components.
• SwitchingFunction3PhaseMaterialMaterial for switching function that prevents formation of a third phase at a two-phase interface:
• SwitchingFunctionMaterialHelper material to provide and its derivative in one of two polynomial forms. SIMPLE: HIGH:
• SwitchingFunctionMultiPhaseMaterialCalculates the switching function for a given phase for a multi-phase, multi-order parameter model
• ThirdPhaseSuppressionMaterialFree Energy contribution that penalizes more than two order parameters being non-zero
• TimeStepMaterialProvide various time stepping quantities as material properties.
• VanDerWaalsFreeEnergyFree energy of a Van der Waals gas.
• VariableGradientMaterialCompute the norm of the gradient of a variable
• Solid Mechanics App
• ADAbruptSofteningSoftening model with an abrupt stress release upon cracking. This class relies on automatic differentiation and is intended to be used with ADComputeSmearedCrackingStress.
• ADCZMComputeDisplacementJumpSmallStrainCompute the total displacement jump across a czm interface in local coordinates for the Small Strain kinematic formulation
• ADCZMComputeDisplacementJumpTotalLagrangianCompute the displacement jump increment across a czm interface in local coordinates for the Total Lagrangian kinematic formulation
• ADCZMComputeGlobalTractionSmallStrainComputes the czm traction in global coordinates for a small strain kinematic formulation
• ADCZMComputeGlobalTractionTotalLagrangianCompute the equilibrium traction (PK1) and its derivatives for the Total Lagrangian formulation.
• ADCombinedNonlinearHardeningPlasticityCombined isotropic and kinematic plasticity model with nonlinear hardening rules, including a Voce model for isotropic hardening and an Armstrong-Fredrick model for kinematic hardening.
• ADCombinedScalarDamageScalar damage model which is computed as a function of multiple scalar damage models
• ADCompositePowerLawCreepStressUpdateThis class uses the stress update material in a radial return isotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations. This class is an extension to include multi-phase capability.
• ADComputeAxisymmetric1DFiniteStrainCompute a strain increment and rotation increment for finite strains in an axisymmetric 1D problem
• ADComputeAxisymmetric1DIncrementalStrainCompute strain increment for small strains in an axisymmetric 1D problem
• ADComputeAxisymmetric1DSmallStrainCompute a small strain in an Axisymmetric 1D problem
• ADComputeAxisymmetricRZFiniteStrainCompute a strain increment for finite strains under axisymmetric assumptions.
• ADComputeAxisymmetricRZIncrementalStrainCompute a strain increment and rotation increment for finite strains under axisymmetric assumptions.
• ADComputeAxisymmetricRZSmallStrainCompute a small strain in an Axisymmetric geometry
• ADComputeDamageStressCompute stress for damaged elastic materials in conjunction with a damage model.
• ADComputeDilatationThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the total dilatation as a function of temperature
• ADComputeEigenstrainComputes a constant Eigenstrain
• ADComputeElasticityTensorCompute an elasticity tensor.
• ADComputeFiniteShellStrainCompute a large strain increment for the shell.
• ADComputeFiniteStrainCompute a strain increment and rotation increment for finite strains.
• ADComputeFiniteStrainElasticStressCompute stress using elasticity for finite strains
• ADComputeGreenLagrangeStrainCompute a Green-Lagrange strain.
• ADComputeIncrementalShellStrainCompute a small strain increment for the shell.
• ADComputeIncrementalSmallStrainCompute a strain increment and rotation increment for small strains.
• ADComputeIncrementalStrainCompute a strain increment and rotation increment for small strains.
• ADComputeInstantaneousThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the instantaneous thermal expansion as a function of temperature
• ADComputeIsotropicElasticityTensorCompute a constant isotropic elasticity tensor.
• ADComputeIsotropicElasticityTensorShellCompute a plane stress isotropic elasticity tensor.
• ADComputeLinearElasticStressCompute stress using elasticity for small strains
• ADComputeMeanThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the mean thermal expansion as a function of temperature
• ADComputeMultipleInelasticStressCompute state (stress and internal parameters such as plastic strains and internal parameters) using an iterative process. Combinations of creep models and plastic models may be used.
• ADComputeMultiplePorousInelasticStressCompute state (stress and internal parameters such as plastic strains and internal parameters) using an iterative process. A porosity material property is defined and is calculated from the trace of inelastic strain increment.
• ADComputePlaneFiniteStrainCompute strain increment and rotation increment for finite strain under 2D planar assumptions.
• ADComputePlaneIncrementalStrainCompute strain increment for small strain under 2D planar assumptions.
• ADComputePlaneSmallStrainCompute a small strain under generalized plane strain assumptions where the out of plane strain is generally nonzero.
• ADComputeRSphericalFiniteStrainCompute a strain increment and rotation increment for finite strains in 1D spherical symmetry problems.
• ADComputeRSphericalIncrementalStrainCompute a strain increment for incremental strains in 1D spherical symmetry problems.
• ADComputeRSphericalSmallStrainCompute a small strain 1D spherical symmetry case.
• ADComputeShellStressCompute in-plane stress using elasticity for shell
• ADComputeSmallStrainCompute a small strain.
• ADComputeSmearedCrackingStressCompute stress using a fixed smeared cracking model. Uses automatic differentiation
• ADComputeStrainIncrementBasedStressCompute stress after subtracting inelastic strain increments
• ADComputeThermalExpansionEigenstrainComputes eigenstrain due to thermal expansion with a constant coefficient
• ADComputeVariableIsotropicElasticityTensorCompute an isotropic elasticity tensor for elastic constants that change as a function of material properties
• ADComputeVolumetricEigenstrainComputes an eigenstrain that is defined by a set of scalar material properties that summed together define the volumetric change.
• ADConstantsFromElasticityTensorCalculate elastic constants from an isotropic elasticity tensor
• ADEigenDecompositionMaterialEmits material properties for the eigenvalues and eigenvectors of a symmetric rank two tensor.
• ADEshelbyTensorComputes the Eshelby tensor as a function of strain energy density and the first Piola-Kirchhoff stress
• ADExponentialEnergyBasedSofteningSoftening model with an exponential softening response upon cracking. This class is intended to be used with ADComputeSmearedCrackingStress and relies on automatic differentiation.
• ADExponentialSofteningSoftening model with an exponential softening response upon cracking. This class is intended to be used with ADComputeSmearedCrackingStress and relies on automatic differentiation.
• ADHillConstantsBuild and rotate the Hill Tensor. It can be used with other Hill plasticity and creep materials.
• ADHillCreepStressUpdateThis class uses the stress update material in a generalized radial return anisotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADHillElastoPlasticityStressUpdateThis class uses the generalized radial return for anisotropic elasto-plasticity model.This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADHillPlasticityStressUpdateThis class uses the generalized radial return for anisotropic plasticity model.This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADIsotropicPlasticityStressUpdateThis class uses the discrete material in a radial return isotropic plasticity model. This class is one of the basic radial return constitutive models, yet it can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADIsotropicPowerLawHardeningStressUpdateThis class uses the discrete material in a radial return isotropic plasticity power law hardening model, solving for the yield stress as the intersection of the power law relation curve and Hooke's law. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADLAROMANCEPartitionStressUpdateLAROMANCE base class for partitioned reduced order models
• ADLAROMANCEStressUpdateBase class to calculate the effective creep strain based on the rates predicted by a material specific Los Alamos Reduced Order Model derived from a Visco-Plastic Self Consistent calculations.
• ADMultiplePowerLawCreepStressUpdateThis class uses the stress update material in a radial return isotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADNonlocalDamageNonlocal damage model. Given an RadialAverage UO this creates a new damage index that can be used as for ComputeDamageStress without havign to change existing local damage models.
• ADPorosityFromStrainPorosity calculation from the inelastic strain.
• ADPowerLawCreepStressUpdateThis class uses the stress update material in a radial return isotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• ADPowerLawSofteningSoftening model with an abrupt stress release upon cracking. This class is intended to be used with ADComputeSmearedCrackingStress and relies on automatic differentiation.
• ADPureElasticTractionSeparationPure elastic traction separation law.
• ADRankTwoCartesianComponentAccess a component of a RankTwoTensor
• ADRankTwoCylindricalComponentCompute components of a rank-2 tensor in a cylindrical coordinate system
• ADRankTwoDirectionalComponentCompute a Direction scalar property of a RankTwoTensor
• ADRankTwoInvariantCompute a invariant property of a RankTwoTensor
• ADRankTwoSphericalComponentCompute components of a rank-2 tensor in a spherical coordinate system
• ADScalarMaterialDamageScalar damage model for which the damage is prescribed by another material
• ADStrainAdjustedDensityCreates density material property
• ADStrainEnergyDensityComputes the strain energy density using a combination of the elastic and inelastic components of the strain increment, which is a valid assumption for monotonic behavior.
• ADStrainEnergyRateDensityComputes the strain energy density rate using a combination of the elastic and inelastic components of the strain increment, which is a valid assumption for monotonic behavior.
• ADSymmetricFiniteStrainCompute a strain increment and rotation increment for finite strains.
• ADSymmetricFiniteStrainElasticStressCompute stress using elasticity for finite strains
• ADSymmetricIsotropicElasticityTensorCompute a constant isotropic elasticity tensor.
• ADSymmetricLinearElasticStressCompute stress using elasticity for small strains
• ADSymmetricSmallStrainCompute a small strain.
• ADTemperatureDependentHardeningStressUpdateComputes the stress as a function of temperature and plastic strain from user-supplied hardening functions. This class can be used in conjunction with other creep and plasticity materials for more complex simulations
• ADViscoplasticityStressUpdateThis material computes the non-linear homogenized gauge stress in order to compute the viscoplastic responce due to creep in porous materials. This material must be used in conjunction with ADComputeMultiplePorousInelasticStress
• AbaqusUMATStressCoupling material to use Abaqus UMAT models in MOOSE
• AbruptSofteningSoftening model with an abrupt stress release upon cracking. This class is intended to be used with ComputeSmearedCrackingStress.
• BiLinearMixedModeTractionMixed mode bilinear traction separation law.
• CZMComputeDisplacementJumpSmallStrainCompute the total displacement jump across a czm interface in local coordinates for the Small Strain kinematic formulation
• CZMComputeDisplacementJumpTotalLagrangianCompute the displacement jump increment across a czm interface in local coordinates for the Total Lagrangian kinematic formulation
• CZMComputeGlobalTractionSmallStrainComputes the czm traction in global coordinates for a small strain kinematic formulation
• CZMComputeGlobalTractionTotalLagrangianCompute the equilibrium traction (PK1) and its derivatives for the Total Lagrangian formulation.
• CZMRealVectorCartesianComponentAccess a component of a RealVectorValue defined on a cohesive zone
• CZMRealVectorScalarCompute the normal or tangent component of a vector quantity defined on a cohesive interface.
• CappedDruckerPragerCosseratStressUpdateCapped Drucker-Prager plasticity stress calculator for the Cosserat situation where the host medium (ie, the limit where all Cosserat effects are zero) is isotropic. Note that the return-map flow rule uses an isotropic elasticity tensor built with the 'host' properties defined by the user.
• CappedDruckerPragerStressUpdateCapped Drucker-Prager plasticity stress calculator
• CappedMohrCoulombCosseratStressUpdateCapped Mohr-Coulomb plasticity stress calculator for the Cosserat situation where the host medium (ie, the limit where all Cosserat effects are zero) is isotropic. Note that the return-map flow rule uses an isotropic elasticity tensor built with the 'host' properties defined by the user.
• CappedMohrCoulombStressUpdateNonassociative, smoothed, Mohr-Coulomb plasticity capped with tensile (Rankine) and compressive caps, with hardening/softening
• CappedWeakInclinedPlaneStressUpdateCapped weak inclined plane plasticity stress calculator
• CappedWeakPlaneCosseratStressUpdateCapped weak-plane plasticity Cosserat stress calculator
• CappedWeakPlaneStressUpdateCapped weak-plane plasticity stress calculator
• CombinedNonlinearHardeningPlasticityCombined isotropic and kinematic plasticity model with nonlinear hardening rules, including a Voce model for isotropic hardening and an Armstrong-Fredrick model for kinematic hardening.
• CombinedScalarDamageScalar damage model which is computed as a function of multiple scalar damage models
• ComplianceSensitivityComputes compliance sensitivity needed for SIMP method.
• CompositeEigenstrainAssemble an Eigenstrain tensor from multiple tensor contributions weighted by material properties
• CompositeElasticityTensorAssemble an elasticity tensor from multiple tensor contributions weighted by material properties
• CompositePowerLawCreepStressUpdateThis class uses the stress update material in a radial return isotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations. This class is an extension to include multi-phase capability.
• ComputeAxisymmetric1DFiniteStrainCompute a strain increment and rotation increment for finite strains in an axisymmetric 1D problem
• ComputeAxisymmetric1DIncrementalStrainCompute strain increment for small strains in an axisymmetric 1D problem
• ComputeAxisymmetric1DSmallStrainCompute a small strain in an Axisymmetric 1D problem
• ComputeAxisymmetricRZFiniteStrainCompute a strain increment for finite strains under axisymmetric assumptions.
• ComputeAxisymmetricRZIncrementalStrainCompute a strain increment and rotation increment for small strains under axisymmetric assumptions.
• ComputeAxisymmetricRZSmallStrainCompute a small strain in an Axisymmetric geometry
• ComputeBeamResultantsCompute forces and moments using elasticity
• ComputeConcentrationDependentElasticityTensorCompute concentration dependent elasticity tensor.
• ComputeCosseratElasticityTensorCompute Cosserat elasticity and flexural bending rigidity tensors
• ComputeCosseratIncrementalSmallStrainCompute incremental small Cosserat strains
• ComputeCosseratLinearElasticStressCompute Cosserat stress and couple-stress elasticity for small strains
• ComputeCosseratSmallStrainCompute small Cosserat strains
• ComputeCrackedStressComputes energy and modifies the stress for phase field fracture
• ComputeCreepPlasticityStressCompute state (stress and internal parameters such as inelastic strains and internal parameters) using an Newton process for one creep and one plasticity model
• ComputeCrystalPlasticityThermalEigenstrainComputes the deformation gradient associated with the linear thermal expansion in a crystal plasticity simulation
• ComputeCrystalPlasticityVolumetricEigenstrainComputes the deformation gradient from the volumetric eigenstrain due to spherical voids in a crystal plasticity simulation
• ComputeDamageStressCompute stress for damaged elastic materials in conjunction with a damage model.
• ComputeDeformGradBasedStressComputes stress based on Lagrangian strain
• ComputeDilatationThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the total dilatation as a function of temperature
• ComputeEigenstrainComputes a constant Eigenstrain
• ComputeEigenstrainBeamFromVariableComputes an eigenstrain from a set of variables
• ComputeEigenstrainFromInitialStressComputes an eigenstrain from an initial stress
• ComputeElasticityBeamComputes the equivalent of the elasticity tensor for the beam element, which are vectors of material translational and flexural stiffness.
• ComputeElasticityTensorCompute an elasticity tensor.
• ComputeElasticityTensorCPCompute an elasticity tensor for crystal plasticity.
• ComputeExtraStressConstantComputes a constant extra stress that is added to the stress calculated by the constitutive model
• ComputeExtraStressVDWGasComputes a hydrostatic stress corresponding to the pressure of a van der Waals gas that is added as an extra_stress to the stress computed by the constitutive model
• ComputeFiniteBeamStrainCompute a rotation increment for finite rotations of the beam and computes the small/large strain increments in the current rotated configuration of the beam.
• ComputeFiniteStrainCompute a strain increment and rotation increment for finite strains.
• ComputeFiniteStrainElasticStressCompute stress using elasticity for finite strains
• ComputeGlobalStrainMaterial for storing the global strain values from the scalar variable
• ComputeHomogenizedLagrangianStrainCalculate eigenstrain-like contribution from the homogenization strain used to satisfy the homogenization constraints.
• ComputeHypoelasticStVenantKirchhoffStressCalculate a small strain elastic stress that is equivalent to the hyperelastic St. Venant-Kirchhoff model if integrated using the Truesdell rate.
• ComputeIncrementalBeamStrainCompute a infinitesimal/large strain increment for the beam.
• ComputeIncrementalSmallStrainCompute a strain increment and rotation increment for small strains.
• ComputeIncrementalStrainCompute a strain increment and rotation increment for small strains.
• ComputeInstantaneousThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the instantaneous thermal expansion as a function of temperature
• ComputeInterfaceStressStress in the plane of an interface defined by the gradient of an order parameter
• ComputeIsotropicElasticityTensorCompute a constant isotropic elasticity tensor.
• ComputeLagrangianCauchyCustomStressCustom stress update providing the Cauchy stress
• ComputeLagrangianLinearElasticStressStress update based on the small (engineering) stress
• ComputeLagrangianObjectiveCustomStressStress update based on the small (engineering) stress
• ComputeLagrangianObjectiveCustomSymmetricStressStress update based on the small (engineering) stress
• ComputeLagrangianStrainCompute strain in Cartesian coordinates.
• ComputeLagrangianStrainAxisymmetricCylindricalCompute strain in 2D axisymmetric RZ coordinates.
• ComputeLagrangianStrainCentrosymmetricSphericalCompute strain in centrosymmetric spherical coordinates.
• ComputeLagrangianStressCustomPK2Stress update based on the first Piola-Kirchhoff stress
• ComputeLagrangianWPSStrainCompute strain in Cartesian coordinates.
• ComputeLagrangianWrappedStressStress update based on the small (engineering) stress
• ComputeLayeredCosseratElasticityTensorComputes Cosserat elasticity and flexural bending rigidity tensors relevant for simulations with layered materials. The layering direction is assumed to be perpendicular to the 'z' direction.
• ComputeLinearElasticPFFractureStressComputes the stress and free energy derivatives for the phase field fracture model, with small strain
• ComputeLinearElasticStressCompute stress using elasticity for small strains
• ComputeLinearViscoelasticStressDivides total strain into elastic + creep + eigenstrains
• ComputeMeanThermalExpansionFunctionEigenstrainComputes eigenstrain due to thermal expansion using a function that describes the mean thermal expansion as a function of temperature
• ComputeMultiPlasticityStressMaterial for multi-surface finite-strain plasticity
• ComputeMultipleCrystalPlasticityStressCrystal Plasticity base class: handles the Newton iteration over the stress residual and calculates the Jacobian based on constitutive laws from multiple material classes that are inherited from CrystalPlasticityStressUpdateBase
• ComputeMultipleInelasticCosseratStressCompute state (stress and other quantities such as plastic strains and internal parameters) using an iterative process, as well as Cosserat versions of these quantities. Only elasticity is currently implemented for the Cosserat versions. Combinations of creep models and plastic models may be used
• ComputeMultipleInelasticStressCompute state (stress and internal parameters such as plastic strains and internal parameters) using an iterative process. Combinations of creep models and plastic models may be used.
• ComputeNeoHookeanStressStress update based on the first Piola-Kirchhoff stress
• ComputePlaneFiniteStrainCompute strain increment and rotation increment for finite strain under 2D planar assumptions.
• ComputePlaneIncrementalStrainCompute strain increment for small strain under 2D planar assumptions.
• ComputePlaneSmallStrainCompute a small strain under generalized plane strain assumptions where the out of plane strain is generally nonzero.
• ComputePlasticHeatEnergyPlastic heat energy density = stress * plastic_strain_rate
• ComputeRSphericalFiniteStrainCompute a strain increment and rotation increment for finite strains in 1D spherical symmetry problems.
• ComputeRSphericalIncrementalStrainCompute a strain increment for incremental strains in 1D spherical symmetry problems.
• ComputeRSphericalSmallStrainCompute a small strain 1D spherical symmetry case.
• ComputeReducedOrderEigenstrainaccepts eigenstrains and computes a reduced order eigenstrain for consistency in the order of strain and eigenstrains.
• ComputeSimoHughesJ2PlasticityStressThe Simo-Hughes style J2 plasticity.
• ComputeSmallStrainCompute a small strain.
• ComputeSmearedCrackingStressCompute stress using a fixed smeared cracking model
• ComputeStVenantKirchhoffStressStress update based on the first Piola-Kirchhoff stress
• ComputeStrainIncrementBasedStressCompute stress after subtracting inelastic strain increments
• ComputeSurfaceTensionKKSSurface tension of an interface defined by the gradient of an order parameter
• ComputeThermalExpansionEigenstrainComputes eigenstrain due to thermal expansion with a constant coefficient
• ComputeThermalExpansionEigenstrainBeamComputes eigenstrain due to thermal expansion with a constant coefficient
• ComputeUpdatedEulerAngleThis class computes the updated Euler angle for crystal plasticity simulations. This needs to be used together with the ComputeMultipleCrystalPlasticityStress class, where the updated rotation material property is computed.
• ComputeVariableBaseEigenStrainComputes Eigenstrain based on material property tensor base
• ComputeVariableEigenstrainComputes an Eigenstrain and its derivatives that is a function of multiple variables, where the prefactor is defined in a derivative material
• ComputeVariableIsotropicElasticityTensorCompute an isotropic elasticity tensor for elastic constants that change as a function of material properties
• ComputeVolumetricDeformGradComputes volumetric deformation gradient and adjusts the total deformation gradient
• ComputeVolumetricEigenstrainComputes an eigenstrain that is defined by a set of scalar material properties that summed together define the volumetric change. This also computes the derivatives of that eigenstrain with respect to a supplied set of variable dependencies.
• ConstantsFromElasticityTensorCalculate elastic constants from an isotropic elasticity tensor
• CrystalPlasticityHCPDislocationSlipBeyerleinUpdateTwo-term dislocation slip model for hexagonal close packed crystals from Beyerline and Tome
• CrystalPlasticityKalidindiUpdateKalidindi version of homogeneous crystal plasticity.
• CrystalPlasticityTwinningKalidindiUpdateTwinning propagation model based on Kalidindi's treatment of twinning in a FCC material
• DensityScalingComputes the scaled inertial density needed to enable stable explicit time-stepping using the desired_time_step in solid-mechanics problems. Note that if this inertial density is used in input files (for instance, in the mass matrix) it will impact the dynamics of the system, largely eliminating high-frequency oscillations, and impacting low-frequency dynamics. Hence, use with caution.
• EigenDecompositionMaterialEmits material properties for the eigenvalues and eigenvectors of a symmetric rank two tensor.
• EshelbyTensorComputes the Eshelby tensor as a function of strain energy density and the first Piola-Kirchhoff stress
• ExponentialEnergyBasedSofteningSoftening model with an exponential softening response upon cracking. This class is intended to be used with ComputeSmearedCrackingStress.
• ExponentialSofteningSoftening model with an exponential softening response upon cracking. This class is intended to be used with ComputeSmearedCrackingStress.
• FiniteStrainCPSlipRateResDeprecated class: please use CrystalPlasticityKalidindiUpdate and ComputeMultipleCrystalPlasticityStress instead.
• FiniteStrainCrystalPlasticityDeprecated class: please use CrystalPlasticityKalidindiUpdate and ComputeMultipleCrystalPlasticityStress instead. Crystal Plasticity base class: FCC system with power law flow rule implemented
• FiniteStrainHyperElasticViscoPlasticMaterial class for hyper-elastic viscoplatic flow: Can handle multiple flow models defined by flowratemodel type user objects
• FiniteStrainPlasticMaterialAssociative J2 plasticity with isotropic hardening.
• FiniteStrainUObasedCPUserObject based Crystal Plasticity system.
• FluxBasedStrainIncrementCompute strain increment based on flux
• GBRelaxationStrainIncrementCompute strain increment based on lattice relaxation at grain boundaries
• GeneralizedKelvinVoigtModelGeneralized Kelvin-Voigt model composed of a serial assembly of unit Kelvin-Voigt modules
• GeneralizedMaxwellModelGeneralized Maxwell model composed of a parallel assembly of unit Maxwell modules
• HillConstantsBuild and rotate the Hill Tensor. It can be used with other Hill plasticity and creep materials.
• HillCreepStressUpdateThis class uses the stress update material in a generalized radial return anisotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• HillElastoPlasticityStressUpdateThis class uses the generalized radial return for anisotropic elasto-plasticity model.This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• HillPlasticityStressUpdateThis class uses the generalized radial return for anisotropic plasticity model.This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• HyperElasticPhaseFieldIsoDamageComputes damaged stress and energy in the intermediate configuration assuming isotropy
• HyperbolicViscoplasticityStressUpdateThis class uses the discrete material for a hyperbolic sine viscoplasticity model in which the effective plastic strain is solved for using a creep approach.
• InclusionPropertiesCalculate quantities used to define the analytical elasticity solution to the inclusion problem.
• IsotropicPlasticityStressUpdateThis class uses the discrete material in a radial return isotropic plasticity model. This class is one of the basic radial return constitutive models, yet it can be used in conjunction with other creep and plasticity materials for more complex simulations.
• IsotropicPowerLawHardeningStressUpdateThis class uses the discrete material in a radial return isotropic plasticity power law hardening model, solving for the yield stress as the intersection of the power law relation curve and Hooke's law. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• LAROMANCEPartitionStressUpdateLAROMANCE base class for partitioned reduced order models
• LAROMANCEStressUpdateBase class to calculate the effective creep strain based on the rates predicted by a material specific Los Alamos Reduced Order Model derived from a Visco-Plastic Self Consistent calculations.
• LinearElasticTrussComputes the linear elastic strain for a truss element
• LinearViscoelasticStressUpdateCalculates an admissible state (stress that lies on or within the yield surface, plastic strains, internal parameters, etc). This class is intended to be a parent class for classes with specific constitutive models.
• MultiPhaseStressMaterialCompute a global stress from multiple phase stresses
• NonlocalDamageNonlocal damage model. Given an RadialAverage UO this creates a new damage index that can be used as for ComputeDamageStress without havign to change existing local damage models.
• PlasticTrussComputes the stress and strain for a truss element with plastic behavior defined by either linear hardening or a user-defined hardening function.
• PorosityFromStrainPorosity calculation from the inelastic strain.
• PowerLawCreepStressUpdateThis class uses the stress update material in a radial return isotropic power law creep model. This class can be used in conjunction with other creep and plasticity materials for more complex simulations.
• PowerLawSofteningSoftening model with an abrupt stress release upon cracking. This class is intended to be used with ComputeSmearedCrackingStress.
• PureElasticTractionSeparationPure elastic traction separation law.
• RankFourTensorToSymmetricRankFourTensorConverts material property of type RankFourTensorTempl<double> to type SymmetricRankFourTensorTempl<double>
• RankTwoCartesianComponentAccess a component of a RankTwoTensor
• RankTwoCylindricalComponentCompute components of a rank-2 tensor in a cylindrical coordinate system
• RankTwoDirectionalComponentCompute a Direction scalar property of a RankTwoTensor
• RankTwoInvariantCompute a invariant property of a RankTwoTensor
• RankTwoSphericalComponentCompute components of a rank-2 tensor in a spherical coordinate system
• RankTwoTensorToSymmetricRankTwoTensorConverts material property of type RankTwoTensorTempl<double> to type SymmetricRankTwoTensorTempl<double>
• SalehaniIrani3DCTraction3D Coupled (3DC) cohesive law of Salehani and Irani with no damage
• ScalarMaterialDamageScalar damage model for which the damage is prescribed by another material
• StrainAdjustedDensityCreates density material property
• StrainEnergyDensityComputes the strain energy density using a combination of the elastic and inelastic components of the strain increment, which is a valid assumption for monotonic behavior.
• StrainEnergyRateDensityComputes the strain energy density rate using a combination of the elastic and inelastic components of the strain increment, which is a valid assumption for monotonic behavior.
• StressBasedChemicalPotentialChemical potential from stress
• SumTensorIncrementsCompute tensor property by summing tensor increments
• SymmetricIsotropicElasticityTensorCompute a constant isotropic elasticity tensor.
• SymmetricRankFourTensorToRankFourTensorConverts material property of type SymmetricRankFourTensorTempl<double> to type RankFourTensorTempl<double>
• SymmetricRankTwoTensorToRankTwoTensorConverts material property of type SymmetricRankTwoTensorTempl<double> to type RankTwoTensorTempl<double>
• TemperatureDependentHardeningStressUpdateComputes the stress as a function of temperature and plastic strain from user-supplied hardening functions. This class can be used in conjunction with other creep and plasticity materials for more complex simulations
• TensileStressUpdateAssociative, smoothed, tensile (Rankine) plasticity with hardening/softening
• ThermalFractureIntegralCalculates summation of the derivative of the eigenstrains with respect to temperature.
• TwoPhaseStressMaterialCompute a global stress in a two phase model
• VolumeDeformGradCorrectedStressTransforms stress with volumetric term from previous configuration to this configuration
• WaveSpeedCalculate the wave speed as where is the effective stiffness, and is the material density.

Mesh

• Moose App
• CreateDisplacedProblemActionCreate a Problem object that utilizes displacements.
• DisplayGhostingActionAction to setup AuxVariables and AuxKernels to display ghosting when running in parallel
• ElementIDOutputActionAction for copying extra element IDs into auxiliary variables for output.
• SetupMeshActionAdd or create Mesh object to the simulation.
• SetupMeshCompleteActionPerform operations on the mesh in preparation for a simulation.
• AddMeshGeneratorActionAdd a MeshGenerator object to the simulation.
• AddMetaDataGeneratorThis mesh generator assigns extraneous mesh metadata to the input mesh
• AdvancedExtruderGeneratorExtrudes a 1D mesh into 2D, or a 2D mesh into 3D, and supports a variable height for each elevation, variable number of layers within each elevation, variable growth factors of axial element sizes within each elevation and remap subdomain_ids, boundary_ids and element extra integers within each elevation as well as interface boundaries between neighboring elevation layers, as well as following a 1D curve and modifying the radial (normal to the extrusion axis) extent of the geometry.
• AllSideSetsByNormalsGeneratorAdds sidesets to the entire mesh based on unique normals.
• AnnularMeshGeneratorFor rmin>0: creates an annular mesh of QUAD4 elements. For rmin=0: creates a disc mesh of QUAD4 and TRI3 elements. Boundary sidesets are created at rmax and rmin, and given these names. If dmin!0 and dmax!360, a sector of an annulus or disc is created. In this case boundary sidesets are also created at dmin and dmax, and given these names
• BSplineCurveGeneratorThis BSplineMeshGenerator object is designed to generate a mesh of a curve that consists of EDGE2, EDGE3, or EDGE4 elements drawn using an open uniform B-Spline.
• BlockDeletionGeneratorMesh generator which removes elements from the specified subdomains
• BlockToMeshConverterGeneratorConverts one or more blocks (subdomains) from a mesh into a stand-alone mesh with a single block in it.
• Boundary2DDelaunayGeneratorMesh generator that convert a 2D surface given as one or a few boundaries of a 3D mesh into a 2D mesh using Delaunay triangulation.
• BoundaryDeletionGeneratorMesh generator which removes side sets
• BoundaryElementConversionGeneratorConvert the elements involved in a set of external boundaries to ensure that the boundary set only contains TRI3 elements
• BoundaryLayerSubdomainGeneratorChanges the subdomain ID of elements near the specified boundary(ies).
• BoundingBoxNodeSetGeneratorAssigns all of the nodes either inside or outside of a bounding box to a new nodeset.
• BreakBoundaryOnSubdomainGeneratorBreak boundaries based on the subdomains to which their sides are attached. Naming convention for the new boundaries will be the old boundary name plus "_to_" plus the subdomain name
• BreakMeshByBlockGeneratorBreak the mesh at interfaces between blocks. New nodes will be generated so elements on each side of the break are no longer connected.
• BreakMeshByElementGeneratorBreak all element-element interfaces in the specified subdomains.
• CartesianMeshGeneratorThis CartesianMeshGenerator creates a non-uniform Cartesian mesh.
• CircularBoundaryCorrectionGeneratorThis CircularBoundaryCorrectionGenerator object is designed to correct full or partial circular boundaries in a 2D mesh to preserve areas.
• CoarsenBlockGeneratorMesh generator which coarsens one or more blocks in an existing mesh. The coarsening algorithm works best for regular meshes.
• CombinerGeneratorCombine multiple meshes (or copies of one mesh) together into one (disjoint) mesh. Can optionally translate those meshes before combining them.
• ConcentricCircleMeshGeneratorThis ConcentricCircleMeshGenerator source code is to generate concentric circle meshes.
• CutMeshByLevelSetGeneratorThis CutMeshByLevelSetGenerator object is designed to trim the input mesh by removing all the elements on outside the give level set with special processing on the elements crossed by the cutting surface to ensure a smooth cross-section. The output mesh only consists of TET4 elements.
• CutMeshByPlaneGeneratorThis CutMeshByPlaneGenerator object is designed to trim the input mesh by removing all the elements on one side of a given plane with special processing on the elements crossed by the cutting plane to ensure a smooth cross-section. The output mesh only consists of TET4 elements.
• DeleteElementsNearMeshGeneratorRemoves elements lying "near" another mesh. The proximity is examined by the distance from the element's centroid to the faces of elements of the "proximity_mesh"
• DistributedRectilinearMeshGeneratorCreate a line, square, or cube mesh with uniformly spaced or biased elements.
• ElementGeneratorGenerates individual elements given a list of nodal positions.
• ElementOrderConversionGeneratorMesh generator which converts orders of elements
• ElementSubdomainIDGeneratorAllows the user to assign each element the subdomain ID of their choice
• ElementsToSimplicesConverterSplits all non-simplex elements in a mesh into simplices.
• ElementsToTetrahedronsConverterThis ElementsToTetrahedronsConverter object is designed to convert all the elements in a 3D mesh consisting only linear elements into TET4 elements.
• ExamplePatchMeshGeneratorCreates 2D or 3D patch meshes.
• ExplodeMeshGeneratorBreak all element-element interfaces in the specified subdomains.
• ExtraNodesetGeneratorCreates a new node set and a new boundary made with the nodes the user provides.
• FancyExtruderGeneratorExtrudes a 1D mesh into 2D, or a 2D mesh into 3D, and supports a variable height for each elevation, variable number of layers within each elevation, variable growth factors of axial element sizes within each elevation and remap subdomain_ids, boundary_ids and element extra integers within each elevation as well as interface boundaries between neighboring elevation layers, as well as following a 1D curve and modifying the radial (normal to the extrusion axis) extent of the geometry.
• FileMeshGeneratorRead a mesh from a file.
• FillBetweenCurvesGeneratorThis FillBetweenCurvesGenerator object is designed to generate a transition layer to connect two boundaries of two input meshes.
• FillBetweenPointVectorsGeneratorThis FillBetweenPointVectorsGenerator object is designed to generate a transition layer with two sides containing different numbers of nodes.
• FillBetweenSidesetsGeneratorThis FillBetweenSidesetsGenerator object is designed to generate a transition layer to connect two boundaries of two input meshes.
• FlipSidesetGeneratorA Mesh Generator which flips a given sideset
• GeneratedMeshGeneratorCreate a line, square, or cube mesh with uniformly spaced or biased elements.
• ImageMeshGeneratorGenerated mesh with the aspect ratio of a given image stack.
• ImageSubdomainGeneratorSamples an image at the coordinates of each element centroid, using the resulting pixel color value as each element's subdomain ID
• LowerDBlockFromSidesetGeneratorAdds lower dimensional elements on the specified sidesets.
• ManifoldSubdomainGeneratorChanges the subdomain ID of elements whose vertex-average point lies inside or outside a closed manifold defined by surface mesh.
• MeshCollectionGeneratorCollects multiple meshes into a single (unconnected) mesh.
• MeshDiagnosticsGeneratorRuns a series of diagnostics on the mesh to detect potential issues such as unsupported features
• MeshExtruderGeneratorTakes a 1D or 2D mesh and extrudes the entire structure along the specified axis increasing the dimensionality of the mesh.
• MeshRepairGeneratorMesh generator to perform various improvement / fixing operations on an input mesh
• MoveNodeGeneratorModifies the position of one or more nodes
• NodeSetsFromSideSetsGeneratorMesh generator which constructs node sets from side sets
• OrientSurfaceMeshGeneratorChange the orientation of (part of) the surface mesh.
• OrientedSubdomainBoundingBoxGeneratorDefines a subdomain inside or outside of a bounding box with arbitrary orientation.
• OverlayMeshGeneratorCreates a Cartesian mesh overlaying the input mesh region.
• ParsedCurveGeneratorThis ParsedCurveGenerator object is designed to generate a mesh of a curve that consists of EDGE2, EDGE3, or EDGE4 elements.
• ParsedElementDeletionGeneratorRemoves elements such that the parsed expression is evaluated as strictly positive. The parameters of the parsed expression can be the X,Y,Z coordinates of the element vertex average (must be 'x','y','z' in the expression), the element volume (must be 'volume' in the expression) and the element id ('id' in the expression).
• ParsedExtraElementIDGeneratorUses a parsed expression to set an extra element id for elements (via their centroids).
• ParsedGenerateNodesetA MeshGenerator that adds nodes to a nodeset if the node satisfies the expression expression.
• ParsedGenerateSidesetA MeshGenerator that adds element sides to a sideset if the centroid of the side satisfies the combinatorial_geometry expression.
• ParsedNodeTransformGeneratorApplies a transform to a the x,y,z coordinates of a Mesh
• ParsedSubdomainIDsGeneratorUses a parsed expression to determine the subdomain ids of included elements.
• ParsedSubdomainMeshGeneratorUses a parsed expression (combinatorial_geometry) to determine if an element (via its centroid) is inside the region defined by the expression and assigns a new block ID.
• PatchMeshGeneratorCreates 2D or 3D patch meshes.
• PatternedMeshGeneratorCreates a 2D mesh from a specified set of unique 'tiles' meshes and a two-dimensional pattern.
• PlaneDeletionGeneratorRemoves elements lying 'above' the plane (in the direction of the normal).
• PlaneIDMeshGeneratorAdds an extra element integer that identifies planes in a mesh.
• PolyLineMeshFollowingNodeSetGeneratorGenerates a polyline (open ended or looped) of Edge elements by marching along a nodeeset and trying to be as close as possible to the nodes of the nodeset
• PolyLineMeshGeneratorGenerates meshes from edges connecting a list of points.
• ProjectSideSetOntoLevelSetGeneratorProjects a sideset onto a surface defined by a level set and creates a surface mesh.
• RBBMappingConverterReinterpolates all elements in a mesh to use Rational Bernstein-Bezier mappings
• RefineBlockGeneratorMesh generator which refines one or more blocks in an existing mesh
• RefineSidesetGeneratorMesh generator which refines one or more sidesets
• RenameBlockGeneratorChanges the block IDs and/or block names for a given set of blocks defined by either block ID or block name. The changes are independent of ordering. The merging of blocks is supported.
• RenameBoundaryGeneratorChanges the boundary IDs and/or boundary names for a given set of boundaries defined by either boundary ID or boundary name. The changes are independent of ordering. The merging of boundaries is supported.
• RenumberBySubdomainGeneratorChanges the element and node IDs so that elements and nodes are contiguous within a subdomain. Note that DoF ordering may be affected as well, and that the mesh renumbering will be turned off.
• RinglebMeshGeneratorCreates a mesh for the Ringleb problem.
• SideSetExtruderGeneratorTakes a 1D or 2D mesh and extrudes a selected sideset along the specified axis.
• SideSetsAroundSubdomainGeneratorAdds element faces that are on the exterior of the given block to the sidesets specified
• SideSetsBetweenSubdomainsGeneratorMeshGenerator that creates a sideset composed of the nodes located between two or more subdomains.
• SideSetsFromAllNormalsGeneratorAdds sidesets to the entire mesh based on unique normals.
• SideSetsFromBoundingBoxGeneratorDefines new sidesets using currently-defined sideset IDs inside or outside of a bounding box.
• SideSetsFromNodeSetsGeneratorMesh generator which constructs side sets from node sets
• SideSetsFromNormalsGeneratorAdds a new named sideset to the mesh for all faces matching the specified normal.
• SideSetsFromPointsGeneratorAdds a new sideset starting at the specified point containing all connected element faces with the same normal.
• SmoothMeshGeneratorUtilizes the specified smoothing algorithm to attempt to improve mesh quality.
• SphereMeshGeneratorGenerate a sphere (ball) mesh centered on the origin
• SpiralAnnularMeshGeneratorCreates an annular mesh based on TRI3 or TRI6 elements on several rings.
• StackGeneratorUse the supplied meshes and stitch them on top of each other
• StitchBoundaryMeshGeneratorAllows a pair of boundaries to be stitched together.
• StitchMeshGeneratorAllows multiple mesh files to be stitched together to form a single mesh.
• StitchedMeshGeneratorAllows multiple mesh files to be stitched together to form a single mesh.
• SubdomainBoundingBoxGeneratorChanges the subdomain ID of elements either (XOR) inside or outside the specified box to the specified ID.
• SubdomainIDGeneratorSets all the elements of the input mesh to a unique subdomain ID.
• SubdomainPerElementGeneratorAllows the user to assign each element the subdomain ID of their choice
• SubdomainsFromPartitionerGeneratorChanges the subdomain ID of elements based on the output of the partitioner
• SurfaceSubdomainsDelaunayRemesherMesh generator that re-meshes a 2D surface mesh given as one or more subdomains into a 2D surface mesh using Delaunay triangulation.
• SurfaceSubdomainsFromAllNormalsGeneratorAdds subdomains to surface (2D) elements in the (3D) mesh based on unique normals.
• SymmetryTransformGeneratorApplies a symmetry transformation to the entire mesh.
• TiledMeshGeneratorUse the supplied mesh and create a tiled grid by repeating this mesh in the x, y, and z directions.
• TransfiniteMeshGeneratorCreates a QUAD4 mesh given a set of corner vertices and edge types. The edge type can be either LINE, CIRCARC, DISCRETE or PARSED, with LINE as the default option. For the non-default options the user needs to specify additional parameters via the edge_parameter option as follows: for CIRCARC the deviation of the midpoint from an arccircle, for DISCRETE a set of points, or a paramterization via the PARSED option. Opposite edges may have different distributions s long as the number of points is identical. Along opposite edges a different point distribution can be prescribed via the options bias_x or bias_y for opposing edges.
• TransformGeneratorApplies a linear transform to the entire mesh.
• UniqueExtraIDMeshGeneratorAdd a new extra element integer ID by finding unique combinations of the existing extra element integer ID values
• XYDelaunayGeneratorTriangulates meshes within boundaries defined by input meshes.
• XYMeshLineCutterThis XYMeshLineCutter object is designed to trim the input mesh by removing all the elements on one side of a given straight line with special processing on the elements crossed by the cutting line to ensure a smooth cross-section.
• XYTriangleBoundaryLayerGeneratorGenerate a 2D layered mesh that represents a conformal boundary layer along the boundary of an input 2D mesh or a 1D loop mesh.
• XYZDelaunayGeneratorCreates tetrahedral 3D meshes within boundaries defined by input meshes.
• AnnularMeshFor rmin>0: creates an annular mesh of QUAD4 elements. For rmin=0: creates a disc mesh of QUAD4 and TRI3 elements. Boundary sidesets are created at rmax and rmin, and given these names. If dmin!0 and dmax!360, a sector of an annulus or disc is created. In this case boundary sidesets are also created a dmin and dmax, and given these names
• ConcentricCircleMeshThis ConcentricCircleMesh source code is to generate concentric circle meshes.
• FileMeshRead a mesh from a file.
• GeneratedMeshCreate a line, square, or cube mesh with uniformly spaced or biased elements.
• ImageMeshGenerated mesh with the aspect ratio of a given image stack.
• MeshGeneratorMeshMesh generated using mesh generators
• PatternedMeshCreates a 2D mesh from a specified set of unique 'tiles' meshes and a two-dimensional pattern.
• RinglebMeshCreates a mesh for the Ringleb problem.
• SpiralAnnularMeshCreates an annual mesh based on TRI3 elements (it can also be TRI6 elements) on several rings.
• StitchedMeshReads in all of the given meshes and stitches them all together into one mesh.
• TiledMeshUse the supplied mesh and create a tiled grid by repeating this mesh in the x,y, and z directions.
• BatchMeshGeneratorAction
• Partitioner
• Phase Field App
• EBSDMeshGeneratorMesh generated from a specified DREAM.3D EBSD data file.
• SphereSurfaceMeshGeneratorGenerated sphere mesh - a two dimensional manifold embedded in three dimensional space
• EBSDMeshMesh generated from a specified DREAM.3D EBSD data file.

MeshDivisions

• Moose App
• AddMeshDivisionActionAdd a MeshDivision object to the simulation.
• CartesianGridDivisionDivide the mesh along a Cartesian grid. Numbering increases from bottom to top and from left to right and from back to front. The inner ordering is X, then Y, then Z
• CylindricalGridDivisionDivide the mesh along a cylindrical grid. The innermost numbering of divisions is the radial bins, then comes the azimuthal bins, then the axial bins
• ExtraElementIntegerDivisionDivide the mesh by increasing extra element IDs. The division will be contiguously numbered even if the extra element ids are not
• FunctorBinnedValuesDivisionDivide the mesh along based on uniformly binned values of a functor.
• NearestPositionsDivisionDivide the mesh using a nearest-point / voronoi algorithm, with the points coming from a Positions object
• NestedDivisionDivide the mesh using nested divisions objects
• SphericalGridDivisionDivide the mesh along a spherical grid.
• SubdomainsDivisionDivide the mesh by increasing subdomain ids. The division will be contiguously numbered even if the subdomain ids are not

MeshModifiers

• Moose App
• AddMeshModifiersActionAdd a MeshModifier object to the simulation.
• ActivateElementsByPathDetermine activated elements.
• ActivateElementsCoupledDetermine activated elements.
• CoupledVarThresholdElementSubdomainModifierModify the element subdomain ID if a coupled variable satisfies the criterion for the threshold (above, equal, or below)
• SidesetAroundSubdomainUpdaterSets up a boundary between inner_subdomains and outer_subdomains
• TimedSubdomainModifierModify element subdomain ID of entire subdomains for given points in time. This mesh modifier only runs on the undisplaced mesh, and it will modify both the undisplaced and the displaced mesh.
• VariableValueElementSubdomainModifierModify the element subdomain ID based on the provided variable value.

Modules