Solve the Allen-Cahn equation (experimental module, not followed anymore) More...
Enumerations | |
| enum | { allencahn_stabilisation_none = 0 , allencahn_stabilisation_simple = 1 , allencahn_stabilisation_sav = 3 } |
Functions/Subroutines | |
| subroutine | solve_allencahn_equation (phase_field, phase_field_n, phase_field_nm1, time_step, time_step_n, time_order_discretization, has_ghost_boundary_cells, allencahn_solver, mobility, thickness, energy_wall, undercooling_energy) |
| Solve the Allen-Cahn equation. | |
| subroutine | solve_allencahn_equation_simple (phase_field, phase_field_n, phase_field_nm1, time_step, time_step_n, time_order_discretization, has_ghost_boundary_cells, allencahn_solver, mobility, thickness, energy_wall, undercooling_energy) |
| subroutine | solve_allencahn_equation_sav (phase_field, phase_field_n, phase_field_nm1, time_step, time_step_n, time_order_discretization, has_ghost_boundary_cells, allencahn_solver, mobility, thickness, energy_wall, undercooling_energy) |
| elemental double precision function | free_energy_derivative (phase_field, energy_wall, undercooling_energy) |
| elemental double precision function | free_energy_function (phase_field, energy_wall, undercooling_energy) |
| elemental double precision function | double_well_derivative (phase_field) |
| elemental double precision function | interpolant_derivative (phase_field) |
| elemental double precision function | double_well_function (phase_field) |
| elemental double precision function | interpolant_function (phase_field) |
| double precision function, dimension(rhs_size) | dominance (rhs_size, stencil, matrix) |
Variables | |
| integer, parameter | allencahn_stabilisation = allencahn_stabilisation_simple |
| logical, parameter, private | use_lipschitz_continuous_base_functions = .TRUE. |
Solve the Allen-Cahn equation (experimental module, not followed anymore)
| anonymous enum |
| double precision function, dimension(rhs_size) mod_solve_cell_allencahn_equation::dominance | ( | integer, intent(in) | rhs_size, |
| type(t_cell_stencil), intent(in) | stencil, | ||
| double precision, dimension(rhs_size*stencil%size), intent(in) | matrix ) |
| elemental double precision function mod_solve_cell_allencahn_equation::double_well_derivative | ( | double precision, intent(in) | phase_field | ) |
| elemental double precision function mod_solve_cell_allencahn_equation::double_well_function | ( | double precision, intent(in) | phase_field | ) |
| elemental double precision function mod_solve_cell_allencahn_equation::free_energy_derivative | ( | double precision, intent(in) | phase_field, |
| double precision, intent(in) | energy_wall, | ||
| double precision, intent(in) | undercooling_energy ) |
| elemental double precision function mod_solve_cell_allencahn_equation::free_energy_function | ( | double precision, intent(in) | phase_field, |
| double precision, intent(in) | energy_wall, | ||
| double precision, intent(in) | undercooling_energy ) |
| elemental double precision function mod_solve_cell_allencahn_equation::interpolant_derivative | ( | double precision, intent(in) | phase_field | ) |
| elemental double precision function mod_solve_cell_allencahn_equation::interpolant_function | ( | double precision, intent(in) | phase_field | ) |
| subroutine mod_solve_cell_allencahn_equation::solve_allencahn_equation_sav | ( | double precision, dimension(:,:,:), intent(inout) | phase_field, |
| double precision, dimension(:,:,:), intent(in) | phase_field_n, | ||
| double precision, dimension(:,:,:), intent(in), allocatable | phase_field_nm1, | ||
| double precision, intent(in) | time_step, | ||
| double precision, intent(in) | time_step_n, | ||
| integer, intent(in) | time_order_discretization, | ||
| logical, intent(in) | has_ghost_boundary_cells, | ||
| class(t_linear_solver), intent(inout) | allencahn_solver, | ||
| double precision, intent(in) | mobility, | ||
| double precision, intent(in) | thickness, | ||
| double precision, intent(in) | energy_wall, | ||
| double precision, dimension(:,:,:), intent(in) | undercooling_energy ) |
| subroutine mod_solve_cell_allencahn_equation::solve_allencahn_equation_simple | ( | double precision, dimension(:,:,:), intent(inout) | phase_field, |
| double precision, dimension(:,:,:), intent(in) | phase_field_n, | ||
| double precision, dimension(:,:,:), intent(in), allocatable | phase_field_nm1, | ||
| double precision, intent(in) | time_step, | ||
| double precision, intent(in) | time_step_n, | ||
| integer, intent(in) | time_order_discretization, | ||
| logical, intent(in) | has_ghost_boundary_cells, | ||
| class(t_linear_solver), intent(inout) | allencahn_solver, | ||
| double precision, intent(in) | mobility, | ||
| double precision, intent(in) | thickness, | ||
| double precision, intent(in) | energy_wall, | ||
| double precision, dimension(:,:,:), intent(in) | undercooling_energy ) |
| integer, parameter mod_solve_cell_allencahn_equation::allencahn_stabilisation = allencahn_stabilisation_simple |
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private |