Kernels System

A "Kernel" is a piece of physics. It can represent one or more operators or terms in the weak form of a partial differential equation. With all terms on the left-hand-side, their sum is referred to as the "residual". The residual is evaluated at several integration quadrature points over the problem domain. To implement your own physics in MOOSE, you create your own kernel by subclassing the MOOSE Kernel class.

The Kernel system supports the use of automatic differentiation (AD) for residual calculations, as such there are two options for creating Kernel objects: Kernel and ADKernel. To further understand automatic differentiation, please refer to the Automatic Differentiation page for more information.

In a Kernel subclass the computeQpResidual() function must be overridden. This is where you implement your PDE weak form terms. For non-AD objects the following member functions can optionally be overridden:

  • computeQpJacobian()

  • computeQpOffDiagJacobian()

These two functions provide extra information that can help the numerical solver(s) converge faster and better.

Inside your Kernel class, you have access to several member variables for computing the residual and Jacobian values in the above mentioned functions:

  • _i, _j: indices for the current test and trial shape functions respectively.

  • _qp: current quadrature point index.

  • _u, _grad_u: value and gradient of the variable this Kernel operates on; indexed by _qp (i.e. _u[_qp]).

  • _test, _grad_test: value () and gradient () of the test functions at the q-points; indexed by _i and then _qp (i.e., _test[_i][_qp]).

  • _phi, _grad_phi: value () and gradient () of the trial functions at the q-points; indexed by _j and then _qp (i.e., _phi[_j][_qp]).

  • _q_point: XYZ coordinates of the current quadrature point.

  • _current_elem: pointer to the current element being operated on.

Optimized Kernel Objects

Depending on the residual calculation being performed it is sometimes possible to optimize the calculation of the residual by precomputing values during the finite element assembly of the residual vector. The following table details the various Kernel base classes that can be used for as base classes to improve performance.

BaseOverrideUse
Kernel
ADKernel		computeQpResidualUse when the term in the partial differential equation (PDE) is multiplied by both the test function and the gradient of the test function (_test and _grad_test must be applied)
KernelValue
ADKernelValue		precomputeQpResidualUse when the term computed in the PDE is only multiplied by the test function (do not use _test in the override, it is applied automatically)
KernelGrad
ADKernelGrad		precomputeQpResidualUse when the term computed in the PDE is only multiplied by the gradient of the test function (do not use _grad_test in the override, it is applied automatically)

Custom Kernel Creation

To create a custom kernel, you can follow the pattern of the Diffusion or ADDiffusion objects implemented and included in the MOOSE framework. Additionally, Example 2 in MOOSE provides a step-by-step overview of creating your own custom kernel. The following describes that calculation of the diffusion term of a PDE.

The strong-form of the diffusion equation is defined on a 3-D domain as: find such that

(1)

where is defined as the boundary on which the value of is fixed to a known constant , is defined as the boundary on which the flux across the boundary is fixed to a known constant , and is the boundary outward normal.

The weak form is generated by multiplying by a test function () and integrating over the domain (using inner-product notation):

and then integrating by parts which gives the weak form:

(2)

where is known as the trial function that defines the finite element discretization, , with being the basis functions.

The Jacobian, which is the derivative of Eq. (2) with respect to , is defined as:

(3)

As mentioned, the computeQpResidual method must be overridden for both flavors of kernels non-AD and AD. The computeQpResidual method for the non-AD version, Diffusion, is provided in Listing 1.

Listing 1: The C++ weak-form residual statement of Eq. (2) as implemented in the Diffusion kernel.

Real
Diffusion::computeQpResidual()
{
  return _grad_u[_qp] * _grad_test[_i][_qp];
}
(moose/framework/src/kernels/Diffusion.C)

This object also overrides the computeQpJacobian method to define Jacobian term of (moose/test/tests/test_harness/duplicate_outputs_analyzejacobian) as shown in Listing 2.

Listing 2: The C++ weak-form Jacobian statement of (moose/test/tests/test_harness/duplicate_outputs_analyzejacobian) as implemented in the Diffusion kernel.

Real
Diffusion::computeQpJacobian()
{
  return _grad_phi[_j][_qp] * _grad_test[_i][_qp];
}
(moose/framework/src/kernels/Diffusion.C)

The AD version of this object, ADDiffusion, relies on an optimized kernel object (see Optimized Kernel Objects), as such it overrides precomputeQpResidual as follows.

Listing 3: The C++ pre-computed portions of the weak-form residual statement of Eq. (2) as implemented in the ADDiffusion kernel.

ADDiffusion::precomputeQpResidual()
{
  return _grad_u[_qp];
}
(moose/framework/src/kernels/ADDiffusion.C)

Time Derivative Kernels

You can create a time-derivative term/kernel by subclassing TimeKernel instead of Kernel. For example, the residual contribution for a time derivative term is:

where is the finite element solution, and

(4)

because you can interchange the order of differentiation and summation.

In the equation above, is the time derivative of the th finite element coefficient of . While the exact form of this derivative depends on the time stepping scheme, without much loss of generality, we can assume the following form for the time derivative:

for some constants , which depend on and the timestepping method.

The derivative of equation Eq. (4) with respect to is then:

So that the Jacobian term for equation Eq. (4) is

where is what we call du_dot_du in MOOSE.

Therefore the computeQpResidual() function for our time-derivative term kernel looks like:


return _test[_i][_qp] * _u_dot[_qp];

And the corresponding computeQpJacobian() is:


return _test[_i][_qp] * _phi[_j][_qp] * _du_dot_du[_qp];

Coupling with Scalar Variables

If the weak form has contributions from scalar variables, then this contribution can be treated similarly as coupling from other spatial variables. See the Coupleable interface for how to obtain the variable values. Residual contributions are simply added to the computeQpResidual() function. Jacobian terms from the test spatial variable and incremental scalar variable are added by overriding the function computeQpOffDiagJacobianScalar().

Contributions to the scalar variable weak equation (test scalar variable terms) are not natively treated by the Kernel class. Inclusion of these residual and Jacobian contributions are discussed within ScalarKernels and specifically KernelScalarBase.

Further Kernel Documentation

Several specialized kernel types exist in MOOSE each with useful functionality. Details for each are in the sections below.

Available Objects

  • Moose App
  • 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: .
  • 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
  • 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 representing the contribution of the PDE term , where is a reaction rate material property, is a scalar variable (nonlinear or coupled), and whose Jacobian contribution is calculated using automatic differentiation.
  • 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.
  • 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.
  • 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: .
  • 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 .
  • DivFieldThe divergence operator optionally scaled by a constant scalar coefficient. Weak form: .
  • FunctionDiffusionDiffusion with a function coefficient.
  • 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 .
  • 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
  • ADMatAnisoDiffusionDiffusion equation kernel that takes an anisotropic diffusivity from a material property
  • 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
  • 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.
  • MaskedBodyForceKernel that defines a body force modified by a material mask
  • 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.
  • 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.
  • Heat Transfer App
  • ADHeatConductionSame as Diffusion in terms of physics/residual, but the Jacobian is computed using forward automatic differentiation
  • ADHeatConductionTimeDerivativeAD Time derivative term of the heat equation for quasi-constant specific heat and the density .
  • ADJouleHeatingSourceCalculates the heat source term corresponding to electrostatic Joule heating, with Jacobian contributions calculated using the automatic differentiation system.
  • ADMatHeatSourceForce term in thermal transport to represent a heat source
  • AnisoHeatConductionAnisotropic HeatConduction kernel with weak form given by .
  • AnisoHomogenizedHeatConductionKernel for asymptotic expansion homogenization for thermal conductivity when anisotropic thermal conductivities are used
  • HeatCapacityConductionTimeDerivativeTime derivative term of the heat equation with the heat capacity as an argument.
  • HeatConductionComputes residual/Jacobian contribution for term.
  • HeatConductionTimeDerivativeTime derivative term of the heat equation for quasi-constant specific heat and the density .
  • HeatSourceDemonstrates the multiple ways that scalar values can be introduced into kernels, e.g. (controllable) constants, functions, and postprocessors. Implements the weak form .
  • HomogenizedHeatConductionKernel for asymptotic expansion homogenization for thermal conductivity
  • JouleHeatingSourceCalculates the heat source term corresponding to electrostatic Joule heating.
  • SpecificHeatConductionTimeDerivativeTime derivative term of the heat equation with the specific heat and the density as arguments.
  • TrussHeatConductionComputes conduction term in heat equation for truss elements, taking cross-sectional area into account
  • TrussHeatConductionTimeDerivativeComputes time derivative term in heat equation for truss elements, taking cross-sectional area into account
  • Solid Mechanics App
  • ADDynamicStressDivergenceTensorsResidual due to stress related Rayleigh damping and HHT time integration terms
  • 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.
  • MomentBalancingAdditional term for moment balance of the in-plane components in the 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.
  • raccoon App
  • ADCoefMatDiffusionDiffsuion term optionally multiplied with a coefficient and material properties. The weak form is , where is the product of all multipliers.
  • ADCoefMatReactionReaction term optionally multiplied with a coefficient and material properties. The weak form is , where is the product of all multipliers.
  • ADCoefMatSourceSource term defined by the product of a coefficient and material properties
  • ADPFFDiffusionThe diffusion term in the phase-field evolution equation. The weak form is .
  • ADPFFPressureThis class computes the pressure term in the phase-field evolution equation for pressurized crack. The weak form is .
  • ADPFFSourceThe source term in the phase-field evolution equation. The weak form is .
  • ADPressurizedCrackThis class computes the body force term from pressurized phase-field fracture. The weak form is .