Class List

Here are the classes, structs, unions and interfaces with brief descriptions:

[detail level 1234]

▼NDUBeat
▼Nmodels
▼Nheat_DG
CExactSolution	Exact solution of the problem
CRightHandSide	Source term
CBCNeumann	Neumann boundary condition
CGradExactSolution	Gradient of the exact solution
▼Nlaplace_DG
CExactSolution	Exact solution
CRightHandSide	Source term
CGradExactSolution	Gradient of the exact solution
▼Nmonodomain_fhn_DG
CExactSolution	Exact solution of the trans-membrane potential
CRightHandSide	Source term: applied current
CBCNeumann	Neumann boundary condition of the trans-membrane potential
CGradExactSolution	Gradient of the trans-membrane potential
CExactSolution_w	Exact solution of the gating variable
CGradExactSolution_w	Gradient of the gating variable
CHeatDG	Class to solve the heat equation using the Discontinuous Galerkin method
CLaplaceDG	Class to solve the Laplace equation using the Discontinuous Galerkin method
CMonodomainFHNDG	Class to solve the monodomain equation with Fitzhugh-Nagumo ionic model for the cardiac electrophysiology using the discontinuous Galerkin method
CAssembleDG	Class for the assembly of the main local matrices for discontinuous Galerkin methods
CComputeErrorsDG	Class to compute the errors between the numerical solution (solution_owned) and the exact solution (solution_ex_owned)
CDoFHandlerDG	Class to work with global and local degrees of freedom and their mapping
CDUBFEMHandler	Class used to discretize analytical solutions as linear combinations of Lagrangian or Dubiner basis
CDUBValues	Class representing the Dubiner basis functions definitions
CFaceHandlerDG	Class for the main operations on the faces of a discontinuous Galerkin element
CModelDG	Class representing the resolution of problems using discontinuous Galerkin methods
CModelDG_t	Class representing the resolution of time-dependent problems using discontinuous Galerkin methods
CQGaussLegendreSimplex	Class representing the Gauss-Legendre quadrature formula on simplex elements
CVolumeHandlerDG	Class for the main operations on a discontinuous Galerkin volume element