BCs System

construction:Undocumented System

The BCs system has not been documented. The content listed below should be used as a starting point for documenting the system, which includes the typical automatic documentation associated with a system; however, what is contained is ultimately determined by what is necessary to make the documentation clear for users.


# BCs System

## Overview

!! Replace this line with information regarding the BCs system.

## Example Input File Syntax

!! Describe and include an example of how to use the BCs system.

!syntax list /BCs objects=True actions=False subsystems=False

!syntax list /BCs objects=False actions=False subsystems=True

!syntax list /BCs objects=False actions=True subsystems=False

Available Objects

Moose App
ADDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-533af818-b810-41a1-a324-2c78868e5357");katex.render("u=g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-3174e4b1-7337-4d14-92bf-ae99b93ee159");katex.render("g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
ADFunctionDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-4d5d92a9-35ea-4ef7-940c-79316453e2ae");katex.render("u=g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-bd2f95d8-2038-4457-95d3-35c7f71101b9");katex.render("g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is calculated by a function.
ADFunctionNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-f2677bbd-b4c8-4a44-9e44-98a92dbbcab7");katex.render("\\frac{\\partial u}{\\partial n}=h(t,\\vec{x})", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-40e6987f-4cda-453b-9c84-2755ec057795");katex.render("h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a (possibly) time and space-dependent MOOSE Function.
ADFunctionPenaltyDirichletBCEnforces a (possibly) time and space-dependent MOOSE Function Dirichlet boundary condition in a weak sense by penalizing differences between the current solution and the Dirichlet data.
ADNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-ba770be6-d646-4017-91a9-d6b4d5e6b1da");katex.render("\\frac{\\partial u}{\\partial n}=h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-5e91716b-cd60-4c15-bd7e-1550bee4c198");katex.render("h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
ADPenaltyDirichletBCEnforces a Dirichlet boundary condition in a weak sense by penalizing differences between the current solution and the Dirichlet data.
ADVectorFunctionDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-02429e5f-071b-41d2-9b1e-495db849aa90");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-e6cd2c24-adf8-4fdc-b434-acd25b35fe64");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ components are calculated with functions.
ADVectorMatchedValueBCImplements a ADVectorNodalBC which equates two different Variables' values on a specified boundary.
ArrayDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-cda9c0eb-fcc7-4f79-8044-23561f8253c2");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-2806a65f-4ad1-408c-8a5d-605d57de1fb9");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ are constant, controllable values.
ArrayHFEMDirichletBCImposes the Dirichlet BC with HFEM.
ArrayNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-8c7cae16-6693-4c42-90f3-675e95dd41e1");katex.render("\\frac{\\partial u}{\\partial n}=h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-a9911867-b5be-4303-998c-c6663bc55252");katex.render("h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
ArrayPenaltyDirichletBCEnforces a Dirichlet boundary condition in a weak sense with $var element = document.getElementById("moose-equation-24a840e6-1b0c-4e28-8566-bf9134bc264a");katex.render("p(\\vec{u}^\\ast, \\vec{u} - \\vec{u}_0)", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-258180b5-ec09-4645-abf3-f300ab77f1a1");katex.render("p", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is the constant scalar penalty; $var element = document.getElementById("moose-equation-20cb4f1e-e7b0-4ba3-9e35-eef5b107321e");katex.render("\\vec{u}^\\ast", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is the test functions and $var element = document.getElementById("moose-equation-284a9e03-c723-49c0-95b0-5f407b86bc68");katex.render("\\vec{u} - \\vec{u}_0", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is the differences between the current solution and the Dirichlet data.
ArrayVacuumBCImposes the Robin boundary condition $var element = document.getElementById("moose-equation-196a90dc-0b28-4e42-9cbd-8a37c4a02c7f");katex.render("\\partial_n \\vec{u}=-\\frac{\\vec{\\alpha}}{2}\\vec{u}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ .
ConvectiveFluxBCDetermines boundary values via the initial and final values, flux, and exposure duration
CoupledVarNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-93460b35-fea2-47ef-81b7-695fc2cc5e8a");katex.render("\\frac{\\partial u}{\\partial n}=v", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-332dbfdd-1413-4ec4-93f6-2e298b6ae645");katex.render("v", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a variable.
DGFunctionDiffusionDirichletBCDiffusion Dirichlet boundary condition for discontinuous Gelerkin method.
DiffusionFluxBCComputes a boundary residual contribution consistent with the Diffusion Kernel. Does not impose a boundary condition; instead computes the boundary contribution corresponding to the current value of grad(u) and accumulates it in the residual vector.
DirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-8ece5766-6722-494a-8166-d73487cd586a");katex.render("u=g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-425a4751-f22f-46ee-94a9-c4f09d244f83");katex.render("g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
EigenArrayDirichletBCArray Dirichlet BC for eigenvalue solvers
EigenDirichletBCDirichlet BC for eigenvalue solvers
FunctionDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-e2727461-f7e8-419b-abc0-e305d52aa2cc");katex.render("u=g(t,\\vec{x})", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-d5a56a63-0ce7-4ada-82f0-0e98ac5df713");katex.render("g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a (possibly) time and space-dependent MOOSE Function.
FunctionGradientNeumannBCImposes the integrated boundary condition arising from integration by parts of a diffusion/heat conduction operator, and where the exact solution can be specified.
FunctionNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-1f154097-fae0-4f0d-ae33-a57673d860c7");katex.render("\\frac{\\partial u}{\\partial n}=h(t,\\vec{x})", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-37d2954c-381e-4c60-aabb-96e4d534127b");katex.render("h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a (possibly) time and space-dependent MOOSE Function.
FunctionPenaltyDirichletBCEnforces a (possibly) time and space-dependent MOOSE Function Dirichlet boundary condition in a weak sense by penalizing differences between the current solution and the Dirichlet data.
HFEMDirichletBCImposes the Dirichlet BC with HFEM.
LagrangeVecDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-da57f795-d4e6-413b-868d-2ff3d3ac01c9");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-e2a957a7-6a3a-4fb9-9a31-c1800129afbe");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ are constant, controllable values.
LagrangeVecFunctionDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-d1b90493-e428-4fc7-9a4e-b8e16b8484e4");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-e0ec192b-feb4-4a81-9f91-7b365c274742");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ components are calculated with functions.
MatchedValueBCImplements a NodalBC which equates two different Variables' values on a specified boundary.
NeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-6c5c2900-5d37-4cc1-bb3c-daa57cb8d006");katex.render("\\frac{\\partial u}{\\partial n}=h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-79f0b70d-36d9-4970-b5bd-38cec27286d2");katex.render("h", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
OneDEqualValueConstraintBCComputes the \f$ \int \lambda dg\f$ term from the mortar method (for two 1D domains only).
PenaltyDirichletBCEnforces a Dirichlet boundary condition in a weak sense by penalizing differences between the current solution and the Dirichlet data.
PostprocessorDirichletBCDirichlet boundary condition with value prescribed by a Postprocessor value.
PostprocessorNeumannBCNeumann boundary condition with value prescribed by a Postprocessor value.
SinDirichletBCImposes a time-varying essential boundary condition $var element = document.getElementById("moose-equation-3433faeb-187b-4f60-8fbe-94fd6d03dddf");katex.render("u=g(t)", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-1490ad01-6166-4d53-baa7-8f1bc2cac086");katex.render("g(t)", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ varies from an given initial value at time $var element = document.getElementById("moose-equation-a753641f-26c7-4aec-aee0-c1276630ed8d");katex.render("t=0", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ to a given final value over a specified duration.
SinNeumannBCImposes a time-varying flux boundary condition $var element = document.getElementById("moose-equation-9e32e220-7036-4e13-9995-83972db9c686");katex.render("\\frac{\\partial u}{\\partial n}=g(t)", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-ffb1af84-bcb4-4d2c-9639-93d66863640d");katex.render("g(t)", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ varies from an given initial value at time $var element = document.getElementById("moose-equation-ceb0340d-e99a-40ad-8ae8-f11ec021a45b");katex.render("t=0", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ to a given final value over a specified duration.
VacuumBCVacuum boundary condition for neutron diffusion on the boundary.
VectorDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-95c6faa4-cf6d-4680-9cce-143224547aaa");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-65ffa3f3-6892-4621-800b-b6c3bd88dfb3");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ are constant, controllable values.
VectorFunctionDirichletBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-55712ed7-4e69-4ca5-8284-3d2e0e0c49ac");katex.render("\\vec{u}=\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-91646a09-f96f-4696-a12d-aa12e22bf500");katex.render("\\vec{g}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ components are calculated with functions.
VectorNeumannBCImposes the integrated boundary condition $var element = document.getElementById("moose-equation-d5bd018b-36b2-4ead-a695-79d2ef3e2d69");katex.render("\\frac{\\partial u}{\\partial n}=\\vec{V}\\cdot\\hat{n}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-99f4598a-c2e0-4e87-bde7-2e178f917079");katex.render("\\vec{V}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a user-defined, constant vector.
VectorPenaltyDirichletBCEnforces a Dirichlet boundary condition for vector nonlinear variables in a weak sense by applying a penalty to the difference in the current solution and the Dirichlet data.
WeakGradientBCComputes a boundary residual contribution consistent with the Diffusion Kernel. Does not impose a boundary condition; instead computes the boundary contribution corresponding to the current value of grad(u) and accumulates it in the residual vector.
XFEMApp
CrackTipEnrichmentCutOffBCImposes the essential boundary condition $var element = document.getElementById("moose-equation-d07ac69f-1004-4dc9-8228-4405c5cccf03");katex.render("u=g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ , where $var element = document.getElementById("moose-equation-e7a3aab3-232c-4fb4-abe7-b80b02199556");katex.render("g", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ is a constant, controllable value.
Heat Conduction App
ADConvectiveHeatFluxBCConvective heat transfer boundary condition with temperature and heat transfer coefficent given by material properties.
ConvectiveFluxFunctionDetermines boundary value by fluid heat transfer coefficient and far-field temperature
ConvectiveHeatFluxBCConvective heat transfer boundary condition with temperature and heat transfer coefficent given by material properties.
CoupledConvectiveFlux
CoupledConvectiveHeatFluxBCConvective heat transfer boundary condition with temperature and heat transfer coefficent given by auxiliary variables.
FunctionRadiativeBCBoundary condition for radiative heat exchange where the emissivity function is supplied by a Function.
GapHeatTransferTransfers heat across a gap between two surfaces dependent on the gap geometry specified.
GrayLambertNeumannBCThis BC imposes a heat flux density that is computed from the GrayLambertSurfaceRadiationBase userobject.
HeatConductionBC
InfiniteCylinderRadiativeBCBoundary condition for radiative heat exchange with a cylinderwhere the boundary is approximated as a cylinder as well.
Navier Stokes App
AdvectionBCBoundary conditions for outflow/outflow of advected quantities: phi * velocity * normal, where phi is the advected quantitiy
EnergyFreeBCImplements free advective flow boundary conditions for the energy equation.
INSADMomentumNoBCBCThis class implements the 'No BC' boundary condition based on the 'Laplace' form of the viscous stress tensor.
INSMomentumNoBCBCLaplaceFormThis class implements the 'No BC' boundary condition based on the 'Laplace' form of the viscous stress tensor.
INSMomentumNoBCBCTractionFormThis class implements the 'No BC' boundary condition based on the 'traction' form of the viscous stress tensor.
INSTemperatureNoBCBCThis class implements the 'No BC' boundary condition discussed by Griffiths, Papanastiou, and others.
ImplicitNeumannBCThis class implements a form of the Neumann boundary condition in which the boundary term is treated 'implicitly'.
MassFreeBCImplements free advective flow boundary conditions for the mass equation.
MomentumFreeBCImplements free flow boundary conditions for one of the momentum equations.
MomentumFreeSlipBC
NSEnergyInviscidSpecifiedBCThis class corresponds to the inviscid part of the 'natural' boundary condition for the energy equation.
NSEnergyInviscidSpecifiedDensityAndVelocityBCThis class corresponds to the inviscid part of the 'natural' boundary condition for the energy equation.
NSEnergyInviscidSpecifiedNormalFlowBCThis class corresponds to the inviscid part of the 'natural' boundary condition for the energy equation.
NSEnergyInviscidSpecifiedPressureBCThis class corresponds to the inviscid part of the 'natural' boundary condition for the energy equation.
NSEnergyInviscidUnspecifiedBCThis class corresponds to the inviscid part of the 'natural' boundary condition for the energy equation.
NSEnergyViscousBCThis class couples together all the variables for the compressible Navier-Stokes equations to allow them to be used in derived IntegratedBC classes.
NSEnergyWeakStagnationBCThe inviscid energy BC term with specified normal flow.
NSImposedVelocityBCImpose Velocity BC.
NSImposedVelocityDirectionBCThis class imposes a velocity direction component as a Dirichlet condition on the appropriate momentum equation.
NSInflowThermalBCThis class is used on a boundary where the incoming flow values (rho, u, v, T) are all completely specified.
NSMassSpecifiedNormalFlowBCThis class implements the mass equation boundary term with a specified value of rho*(u.n) imposed weakly.
NSMassUnspecifiedNormalFlowBCThis class implements the mass equation boundary term with the rho*(u.n) boundary integral computed implicitly.
NSMassWeakStagnationBCThe inviscid energy BC term with specified normal flow.
NSMomentumConvectiveWeakStagnationBCThe convective part (sans pressure term) of the momentum equation boundary integral evaluated at specified stagnation temperature, stagnation pressure, and flow direction values.
NSMomentumInviscidNoPressureImplicitFlowBCMomentum equation boundary condition used when pressure is not integrated by parts.
NSMomentumInviscidSpecifiedNormalFlowBCMomentum equation boundary condition in which pressure is specified (given) and the value of the convective part is allowed to vary (is computed implicitly).
NSMomentumInviscidSpecifiedPressureBCMomentum equation boundary condition in which pressure is specified (given) and the value of the convective part is allowed to vary (is computed implicitly).
NSMomentumPressureWeakStagnationBCThis class implements the pressure term of the momentum equation boundary integral for use in weak stagnation boundary conditions.
NSMomentumViscousBCThis class corresponds to the viscous part of the 'natural' boundary condition for the momentum equations.
NSPenalizedNormalFlowBCThis class penalizes the the value of u.n on the boundary so that it matches some desired value.
NSPressureNeumannBCThis kernel is appropriate for use with a 'zero normal flow' boundary condition in the context of the Euler equations.
NSStagnationPressureBCThis Dirichlet condition imposes the condition p_0 = p_0_desired.
NSStagnationTemperatureBCThis Dirichlet condition imposes the condition T_0 = T_0_desired.
NSThermalBCNS thermal BC.
Rdg App
AEFVBCA boundary condition kernel for the advection equation using a cell-centered finite volume method.
Chemical Reactions App
ChemicalOutFlowBCChemical flux boundary condition
Fsi App
FluidFreeSurfaceBCApplies a mixed Dirichlet-Neumann BC on the fluid surface.
Porous Flow App
PorousFlowEnthalpySinkApplies a source equal to the product of the mass flux and the fluid enthalpy. The enthalpy is computed at temperature T_in and pressure equal to the porepressure in the porous medium, if fluid_phase is given, otherwise at the supplied porepressure. Hence this adds heat energy to the porous medium at rate corresponding to a fluid being injected at (porepressure, T_in) at rate (-flux_function).
PorousFlowHalfCubicSinkApplies a flux sink to a boundary. The base flux defined by PorousFlowSink is multiplied by a cubic.
PorousFlowHalfGaussianSinkApplies a flux sink to a boundary. The base flux defined by PorousFlowSink is multiplied by a Gaussian.
PorousFlowPiecewiseLinearSinkApplies a flux sink to a boundary. The base flux defined by PorousFlowSink is multiplied by a piecewise linear function.
PorousFlowSinkApplies a flux sink to a boundary.
Peridynamics App
RBMPresetOldValuePDClass to apply a preset BC to nodes with rigid body motion (RBM).
Functional Expansion Tools App
FXFluxBCSets a flux boundary condition, evaluated using a FunctionSeries instance. This does not fix the flux, but rather 'strongly encourages' flux agreement by penalizing the differences through contributions to the residual.
FXValueBCImposes a fixed value boundary condition, evaluated using a FunctionSeries instance.
FXValuePenaltyBCSets a value boundary condition, evaluated using a FunctionSeries instance. This does not fix the value, but rather 'strongly encourages' value agreement by penalizing the differences through contributions to the residual.
Tensor Mechanics App
ADPressureApplies a pressure on a given boundary in a given direction
ADTorqueApply a moment as tractions distributed over a surface around a pivot point. This should operate on the displaced mesh for large deformations.
CoupledPressureBCApplies a pressure from a variable on a given boundary in a given direction
DashpotBC
DisplacementAboutAxisImplements a boundary condition that enforces rotationaldisplacement around an axis on a boundary
InteractionIntegralBenchmarkBCImplements a boundary condition that enforces a displacement field around a crack tip based on applied stress intensity factors.
PenaltyInclinedNoDisplacementBCPenalty Enforcement of an inclined boundary condition
PresetAccelerationPrescribe acceleration on a given boundary in a given direction
PresetDisplacementPrescribe the displacement on a given boundary in a given direction.
PresetVelocity
PressureApplies a pressure on a given boundary in a given direction
StickyBCImposes the boundary condition $var element = document.getElementById("moose-equation-47477d3b-0288-43f6-9d47-96463f77484a");katex.render("u = u_{old}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ if $var element = document.getElementById("moose-equation-67a03fab-7af0-4875-bba2-ee70a37ecaa1");katex.render("u_{old}", element, {displayMode:false,throwOnError:false,macros:{"\\pf":"\\frac{\\partial #1}{\\partial #2}"}});$ exceeds the bounds provided
TorqueApply a moment as tractions distributed over a surface around a pivot point. This should operate on the displaced mesh for large deformations.

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AddBCActionAdd a BoundaryCondition object to the simulation.

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BCs System

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