Main mesh classes
Main finite element classes
Main linear algebra classes and sources
Main parallel classes
Main GPU classes
Example codes
- Example 0: simplest example, nodal H1 FEM for the Laplace problem
- Example 0p: simplest parallel example, nodal H1 FEM for the Laplace problem
- Example 1: nodal H1 FEM for the Laplace problem (same discretization as ex0 but with more sophisticated options)
- Example 1p: parallel nodal H1 FEM for the Laplace problem (same discretization as ex0p but with more sophisticated options)
- Example 2: vector FEM for linear elasticity
- Example 2p: parallel vector FEM for linear elasticity
- Example 3: Nedelec H(curl) FEM for the definite Maxwell problem
- Example 3p: parallel Nedelec H(curl) FEM for the definite Maxwell problem
- Example 4: Raviart-Thomas H(div) FEM for the grad-div problem
- Example 4p: parallel Raviart-Thomas H(div) FEM for the grad-div problem
- Example 5: mixed pressure-velocity FEM for the Darcy problem
- Example 5p: parallel mixed pressure-velocity FEM for the Darcy problem
- Example 6: non-conforming adaptive mesh refinement for the Laplace problem
- Example 6p: parallel non-conforming adaptive mesh refinement for the Laplace problem
- Example 7: Laplace problem on a surface (the unit sphere)
- Example 7p: parallel Laplace problem on a surface (the unit sphere)
- Example 8: Discontinuous Petrov-Galerkin (DPG) for the Laplace problem
- Example 8p: parallel Discontinuous Petrov-Galerkin (DPG) for the Laplace problem
- Example 9: Discontinuous Galerkin (DG) time-dependent advection
- Example 9p: parallel Discontinuous Galerkin (DG) time-dependent advection
- Example 10: time-dependent implicit nonlinear elasticity
- Example 10p: parallel time-dependent implicit nonlinear elasticity
- Example 11p: parallel Laplace eigensolver
- Example 12p: parallel linear elasticity eigensolver
- Example 13p: parallel Maxwell eigensolver
- Example 14: Discontinuous Galerkin (DG) for the Laplace problem
- Example 14p: parallel Discontinuous Galerkin (DG) for the Laplace problem
- Example 15: dynamic AMR for Laplace with prescribed time-dependent source
- Example 15p: parallel dynamic AMR for Laplace with prescribed time-dependent source
- Example 16: time-dependent nonlinear heat equation
- Example 16p: parallel time-dependent nonlinear heat equation
- Example 17: Discontinuous Galerkin (DG) for linear elasticity
- Example 17p: parallel Discontinuous Galerkin (DG) for linear elasticity
- Example 18: Discontinuous Galerkin (DG) for the Euler equations
- Example 18p: parallel Discontinuous Galerkin (DG) for the Euler equations
- Example 19: incompressible nonlinear elasticity
- Example 19p: parallel incompressible nonlinear elasticity
- Example 20: symplectic ODE integration
- Example 20p: parallel symplectic ODE integration
- Example 21: adaptive mesh refinement for linear elasticity
- Example 21p: parallel adaptive mesh refinement for linear elasticity
- Example 22: complex-valued linear systems for damped harmonic oscillators
- Example 22p: parallel complex-valued linear systems for damped harmonic oscillators
- Example 23: second order in time wave equation
- Example 24: mixed finite element spaces and interpolators
- Example 24p: parallel mixed finite element spaces and interpolators
- Example 25: simulation of electromagnetic wave propagation using a Perfectly Matched Layer (PML)
- Example 25p: parallel simulation of electromagnetic wave propagation using a Perfectly Matched Layer (PML)
- Example 26: multigrid preconditioner for the Laplace problem using nodal H1 FEM
- Example 26p: parallel multigrid preconditioner for the Laplace problem using nodal H1 FEM
- Example 27: boundary conditions for the Laplace problem
- Example 27p: parallel boundary conditions for the Laplace problem
- Example 28: sliding contact in elasticity
- Example 28p: parallel sliding contact in elasticity
- Example 29: Laplace solve on a 3D-embedded surface
- Example 29p: parallel Laplace solve on a 3D-embedded surface
- Example 30: mesh preprocessing to resolve problem data
- Example 30p: parallel mesh preprocessing to resolve problem data
- Example 31: Nedelec H(curl) FEM for the definite anisotropic Maxwell problem
- Example 31p: parallel Nedelec H(curl) FEM for the definite anisotropic Maxwell problem
- Example 32p: parallel anisotropic Maxwell eigensolver
- Example 33: nodal H1 FEM for the fractional Laplacian problem
- Example 33p: parallel nodal H1 FEM for the fractional Laplacian problem
AmgX Examples
Caliper Examples
HiOp Examples
PETSc Examples
PUMI Examples
SUNDIALS Examples
SuperLU Examples
Miniapps
See also the examples documentation online.