- solveTrueWhether or not to actually solve the Nonlinear system. This is handy in the case that all you want to do is execute AuxKernels, Transfers, etc. without actually solving anything
Default:True
C++ Type:bool
Controllable:Yes
Description:Whether or not to actually solve the Nonlinear system. This is handy in the case that all you want to do is execute AuxKernels, Transfers, etc. without actually solving anything
FEProblemBase
The FEProblemBase class is an intermediate base class containing all of the common logic for running the various MOOSE simulations. MOOSE has two built-in types of problems FEProblem for solving "normal" physics problems and EigenProblem for solving Eigenvalue problems. Additionally, MOOSE contains an ExternalProblem problem useful for creating "MOOSE-wrapped Apps".
A normal (default) Problem object that contains a single NonlinearSystem and a single AuxiliarySystem object.
Convenience Zeros
One of the advantages of the MOOSE framework is the ease at building up Multiphysics simulations. Coupling is a first-class feature and filling out residuals, or material properties with coupling is very natural. When coupling is optional, it is often handy to have access to valid data structures that may be used in-place of the actual coupled variables. This makes it possible to avoid branch statements inside of your residual statements and other computationally intensive areas of code. One of the ways MOOSE makes this possible is by making several different types of "zero" variables available. The following statements illustrate how optional coupling may be implemented with these zeros.
// In the constructor initialization list of a Kernel
_velocity_vector(isParamValid("velocity_vector") ? coupledGradient("velocity_vector") : _grad_zero)
// The residual statement
return _test[_i][_qp] * (_velocity_vector[_qp] * _grad_u[_qp]);
Selective Reinit
The system automatically determines which variables should be made available for use on the current element ("reinit"-ed). Each variable is tracked on calls through the coupling interface. Variables that are not needed are simply not prepared. This can save significant amounts of time on systems that have several active variables.
Finite Element Concepts
Shape Functions
While the weak form is essentially what you need for adding physics to MOOSE, in traditional finite element software more work is necessary.
We need to discretize our weak form and select a set of simple "basis functions" amenable for manipulation by a computer.
Our discretized expansion of u takes on the following form:
The here are called "basis functions"
These form the basis for the "trial function",
Analogous to the we used earlier
The gradient of can be expanded similarly:
In the Galerkin finite element method, the same basis functions are used for both the trial and test functions:
Substituting these expansions back into our weak form, we get:
The left-hand side of the equation above is what we generally refer to as the component of our "Residual Vector" and write as .
Shape Functions are the functions that get multiplied by coefficients and summed to form the solution.
Individual shape functions are restrictions of the global basis functions to individual elements.
They are analogous to the functions from polynomial fitting (in fact, you can use those as shape functions).
Typical shape function families: Lagrange, Hermite, Hierarchic, Monomial, Clough-Toucher - MOOSE has support for all of these.
Lagrange shape functions are the most common. - They are interpolary at the nodes, i.e., the coefficients correspond to the values of the functions at the nodes.
Example 1D Shape Functions
Linear Lagrange
Quadratic Lagrange
Cubic Lagrange
Cubic Hermite
2D Lagrange Shape Functions
Example bi-quadratic basis functions defined on the Quad9 element:
is associated to a "corner" node, it is zero on the opposite edges.
is associated to a "mid-edge" node, it is zero on all other edges.
is associated to the "center" node, it is symmetric and on the element.
Numerical Integration
The only remaining non-discretized parts of the weak form are the integrals.
We split the domain integral into a sum of integrals over elements:
Through a change of variables, the element integrals are mapped to integrals over the "reference" elements .
is the Jacobian of the map from the physical element to the reference element.
To approximate the reference element integrals numerically, we use quadrature (typically "Gaussian Quadrature"):
is the spatial location of the th quadrature point and is its associated weight.
MOOSE handles multiplication by the Jacobian and the weight automatically, thus your
Kernel
is only responsible for computing the part of the integrand.Under certain common situations, the quadrature approximation is exact! - For example, in 1 dimension, Gaussian Quadrature can exactly integrate polynomials of order with quadrature points.
Note that sampling at the quadrature points yields:
And our weak form becomes:
The second sum is over boundary faces, .
MOOSE
Kernels
must provide each of the terms in square brackets (evaluated at or as necessary).
Input Parameters
- allow_initial_conditions_with_restartTrueTrue to allow the user to specify initial conditions when restarting. Initial conditions can override any restarted field
Default:True
C++ Type:bool
Controllable:No
Description:True to allow the user to specify initial conditions when restarting. Initial conditions can override any restarted field
- force_restartFalseEXPERIMENTAL: If true, a sub_app may use a restart file instead of using of using the master backup file
Default:False
C++ Type:bool
Controllable:No
Description:EXPERIMENTAL: If true, a sub_app may use a restart file instead of using of using the master backup file
- restart_file_baseFile base name used for restart (e.g.
/ or /LATEST to grab the latest file available) C++ Type:FileNameNoExtension
Controllable:No
Description:File base name used for restart (e.g.
/ or /LATEST to grab the latest file available)
Restart Parameters
- allow_invalid_solutionFalseSet to true to allow convergence even though the solution has been marked as 'invalid'
Default:False
C++ Type:bool
Controllable:No
Description:Set to true to allow convergence even though the solution has been marked as 'invalid'
- immediately_print_invalid_solutionFalseWhether or not to report invalid solution warnings at the time the warning is produced instead of after the calculation
Default:False
C++ Type:bool
Controllable:No
Description:Whether or not to report invalid solution warnings at the time the warning is produced instead of after the calculation
Solution Validity Control Parameters
- boundary_restricted_elem_integrity_checkTrueSet to false to disable checking of boundary restricted elemental object variable dependencies, e.g. are the variable dependencies defined on the selected boundaries?
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable checking of boundary restricted elemental object variable dependencies, e.g. are the variable dependencies defined on the selected boundaries?
- boundary_restricted_node_integrity_checkTrueSet to false to disable checking of boundary restricted nodal object variable dependencies, e.g. are the variable dependencies defined on the selected boundaries?
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable checking of boundary restricted nodal object variable dependencies, e.g. are the variable dependencies defined on the selected boundaries?
- check_uo_aux_stateFalseTrue to turn on a check that no state presents during the evaluation of user objects and aux kernels
Default:False
C++ Type:bool
Controllable:No
Description:True to turn on a check that no state presents during the evaluation of user objects and aux kernels
- error_on_jacobian_nonzero_reallocationFalseThis causes PETSc to error if it had to reallocate memory in the Jacobian matrix due to not having enough nonzeros
Default:False
C++ Type:bool
Controllable:No
Description:This causes PETSc to error if it had to reallocate memory in the Jacobian matrix due to not having enough nonzeros
- fv_bcs_integrity_checkTrueSet to false to disable checking of overlapping Dirichlet and Flux BCs and/or multiple DirichletBCs per sideset
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable checking of overlapping Dirichlet and Flux BCs and/or multiple DirichletBCs per sideset
- kernel_coverage_checkTrueSet to false to disable kernel->subdomain coverage check
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable kernel->subdomain coverage check
- material_coverage_checkTrueSet to false to disable material->subdomain coverage check
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable material->subdomain coverage check
- material_dependency_checkTrueSet to false to disable material dependency check
Default:True
C++ Type:bool
Controllable:No
Description:Set to false to disable material dependency check
- skip_nl_system_checkFalseTrue to skip the NonlinearSystem check for work to do (e.g. Make sure that there are variables to solve for).
Default:False
C++ Type:bool
Controllable:No
Description:True to skip the NonlinearSystem check for work to do (e.g. Make sure that there are variables to solve for).
Simulation Checks Parameters
- control_tagsAdds user-defined labels for accessing object parameters via control logic.
C++ Type:std::vector<std::string>
Controllable:No
Description:Adds user-defined labels for accessing object parameters via control logic.
- default_ghostingFalseWhether or not to use libMesh's default amount of algebraic and geometric ghosting
Default:False
C++ Type:bool
Controllable:No
Description:Whether or not to use libMesh's default amount of algebraic and geometric ghosting
- enableTrueSet the enabled status of the MooseObject.
Default:True
C++ Type:bool
Controllable:No
Description:Set the enabled status of the MooseObject.
Advanced Parameters
- extra_tag_matricesExtra matrices to add to the system that can be filled by objects which compute residuals and Jacobians (Kernels, BCs, etc.) by setting tags on them. The outer index is for which nonlinear system the extra tag vectors should be added for
C++ Type:std::vector<std::vector<TagName>>
Controllable:No
Description:Extra matrices to add to the system that can be filled by objects which compute residuals and Jacobians (Kernels, BCs, etc.) by setting tags on them. The outer index is for which nonlinear system the extra tag vectors should be added for
- extra_tag_solutionsExtra solution vectors to add to the system that can be used by objects for coupling variable values stored in them.
C++ Type:std::vector<TagName>
Controllable:No
Description:Extra solution vectors to add to the system that can be used by objects for coupling variable values stored in them.
- extra_tag_vectorsExtra vectors to add to the system that can be filled by objects which compute residuals and Jacobians (Kernels, BCs, etc.) by setting tags on them. The outer index is for which nonlinear system the extra tag vectors should be added for
C++ Type:std::vector<std::vector<TagName>>
Controllable:No
Description:Extra vectors to add to the system that can be filled by objects which compute residuals and Jacobians (Kernels, BCs, etc.) by setting tags on them. The outer index is for which nonlinear system the extra tag vectors should be added for
Tagging Parameters
- ignore_zeros_in_jacobianFalseDo not explicitly store zero values in the Jacobian matrix if true
Default:False
C++ Type:bool
Controllable:No
Description:Do not explicitly store zero values in the Jacobian matrix if true
- nl_sys_namesnl0 The nonlinear system names
Default:nl0
C++ Type:std::vector<NonlinearSystemName>
Controllable:No
Description:The nonlinear system names
- previous_nl_solution_requiredFalseTrue to indicate that this calculation requires a solution vector for storing the previous nonlinear iteration.
Default:False
C++ Type:bool
Controllable:No
Description:True to indicate that this calculation requires a solution vector for storing the previous nonlinear iteration.
- use_nonlinearTrueDetermines whether to use a Nonlinear vs a Eigenvalue system (Automatically determined based on executioner)
Default:True
C++ Type:bool
Controllable:No
Description:Determines whether to use a Nonlinear vs a Eigenvalue system (Automatically determined based on executioner)
Nonlinear System(S) Parameters
- near_null_space_dimension0The dimension of the near nullspace
Default:0
C++ Type:unsigned int
Controllable:No
Description:The dimension of the near nullspace
- null_space_dimension0The dimension of the nullspace
Default:0
C++ Type:unsigned int
Controllable:No
Description:The dimension of the nullspace
- transpose_null_space_dimension0The dimension of the transpose nullspace
Default:0
C++ Type:unsigned int
Controllable:No
Description:The dimension of the transpose nullspace
Null Space Removal Parameters
- parallel_barrier_messagingFalseDisplays messaging from parallel barrier notifications when executing or transferring to/from Multiapps (default: false)
Default:False
C++ Type:bool
Controllable:No
Description:Displays messaging from parallel barrier notifications when executing or transferring to/from Multiapps (default: false)
- verbose_multiappsFalseSet to True to enable verbose screen printing related to MultiApps
Default:False
C++ Type:bool
Controllable:No
Description:Set to True to enable verbose screen printing related to MultiApps
When "check_uo_aux_state" is set to true, MOOSE will evaluate user objects (including all postprocessors and vector postprocessors) and auxiliary kernels on every execute flag except linear
twice. It then compares the results after two evaluations including the auxiliary system solutions and all the real reporter values added by user objects. When MOOSE sees a difference, it will issue an error indicating that there are unresolved dependencies during the evaluation because otherwise the results should only depend on primary solutions and should not change. MOOSE also prints the details about the difference to help users removing the states caused by these unresolved dependencies.