Declaration of scalar variables associated to the Energy equation. More...
Data Types | |
| type | t_energy_ibc_initializer_item |
Variables | |
| logical | energy_has_linearized_enthalpy_conservative_advection = .false. |
| Has explicit advection term for the linearized enthalpy method? | |
| logical | energy_has_linearized_enthalpy_compressible_gas_only = .false. |
| Has compressible gas around PCM for the linearized enthalpy method? | |
Variables associated to the time discretization | |
| double precision | energy_time_step = 0d0 |
| Current Time step. | |
| double precision | energy_time_step_n = 0d0 |
| Previous time step. | |
| double precision | energy_time_step_nm1 = 0d0 |
| Previous -1 time step. | |
| integer | energy_time_order_discretization = time_order_1 |
| Time order discretization. | |
| integer | energy_explicit_time_order_discretization = time_order_nssp32 |
| Explicit time order discretization. | |
| logical | energy_use_explicit_terms_accumulator = .false. |
| A switch for when to use explicit accumulator. | |
Boundary condition variables | |
| type(t_boundary_condition) | energy_boundary_condition |
| Boundary condition. | |
Initializer | |
| class(t_scalar_initializer), pointer | energy_initializer => null() |
| Initial condition initializer. | |
| class(t_cell_bc_initializer), pointer | energy_bc_initializer => null() |
| Boundary conditions initializer. | |
| class(t_energy_ibc_initializer_item), dimension(:), allocatable | energy_ibc_initializer |
| Immersed boundary conditions initializers. | |
| class(t_scalar_initializer), pointer | energy_source_term_initializer => null() |
| Source term initializer. | |
| class(t_scalar_initializer), pointer | energy_linear_term_initializer => null() |
| Linear term initializer. | |
Logical list to activate terms of the equation | |
| integer | energy_equation_formulation = energy_equation_formulation_cp |
| Has source term? | |
| logical | energy_has_source_term = .false. |
| Has source term? | |
| logical | energy_has_advection_term = .true. |
| Has advection term? | |
| logical | energy_has_diffusion_term = .true. |
| Has diffusion term? | |
| logical | energy_has_viscous_dissipation_rate_term = .false. |
| Has viscous dissipation term? | |
| logical | energy_has_div_u_advection_term = .true. |
| Has \( div(\mathbf{u}) \) advection term? | |
| logical | energy_has_temporal_term = .true. |
| Has temporal term? | |
| logical | energy_has_linear_term = .false. |
| Has linear term? | |
| logical | energy_has_phase_change = .false. |
| Has phase change? | |
| logical | energy_has_phase_thermal_resistance = .false. |
| Has phase resistance? | |
| logical | energy_has_immersed_boundaries = .false. |
| Flag to enable immersed boundaries for the energy equation. | |
Variables related to immersed boundaries | |
| integer, dimension(:), allocatable | energy_isd_target |
| List of enabled immersed boundaries for the energy equation. | |
| integer | n_ibc_temperature = 0 |
| Number of immersed boundaries enabled for the energy equation. | |
| logical | energy_ib_has_one_sided_inner_discretization |
| One sided discretization close to immersed boundaries. | |
| integer, dimension(:), allocatable | energy_ib_inner_discretization_order |
Variables associated to the discretization of the advection term | |
| integer | energy_diffusion_term_discretization_type = implicit_discretization |
| Diffusion term discretization type (implicit or explicit) | |
| integer | energy_diffusion_term_scheme = cell_centered_o2_diffusion_scheme |
| Diffusion term scheme. | |
| integer | energy_diffusion_explicit_time_order_discretization = time_order_1 |
| Diffusion term discretization (temporal discretization) | |
| integer | energy_advection_term_discretization_type = implicit_discretization |
| Advection term discretization type (implicit or explicit) | |
| integer | energy_advection_term_scheme = cell_centered_o2_advection_scheme |
| Advection term scheme. | |
| integer | energy_advection_term_splitting_scheme = lie_trotter_splitting |
| Advection term: Splitting Method for Lax-Wendroff TVD Superbee. | |
| double precision, dimension(3) | energy_splitting_time_coeff =1d0 |
| logical | energy_advection_term_dir_split = .false. |
| Advection term: directional splitting option. | |
| logical | is_energy_specify_advection_scheme_stability_factor = .false. |
| Specify a CFL factor for explicit sub iterations. | |
| double precision | energy_advection_scheme_stability_factor = -1d0 |
CFL used for explicit sub iterations (if is_energy_specify_advection_scheme_stability_factor, otherwize, using default values) | |
| type(t_fv_flux), parameter | default_energy_advection_explicit_flux = default_flux_godunov |
| Fluxes type The default explicit cell advection flux. | |
| type(t_fv_flux) | energy_advection_explicit_flux = default_energy_advection_explicit_flux |
| Fluxes type The effective explicit cell advection flux. | |
| logical | is_energy_fully_explicit = .false. |
| Energy Equations Fully Explicit. | |
Miscellaneous variables | |
| logical | energy_has_ghost_boundary_cells = .false. |
| Ghost boudary cell choice. | |
| type(t_cell_stencil) | energy_stencil |
| Stencil of the energy equation. | |
| integer | energy_enforced_stencil = -1 |
| Enforced stencil. | |
| logical | energy_has_imposed_value = .false. |
| Has imposed value (temperature)? | |
| double precision, dimension(3) | temperature_imposed_point = [0d0, 0d0, COORD_Z_2D] |
| Imposed value. | |
| double precision | temperature_imposed_value = huge(0d0) |
Linear system solver variables | |
| type(t_ls_map) | energy_ls_map |
| Mapping variables. | |
| class(t_linear_solver), allocatable | energy_solver |
| Linear system solver. | |
Phase thermal resistance variables | |
| integer, dimension(:,:), allocatable | energy_phase_thermal_resistance_index |
| Interface index. | |
| double precision, dimension(:), allocatable | energy_phase_thermal_resistance |
| Resistance values. | |
Phase field variables | |
| double precision | phase_field_mobility |
| Mobility parameter in Allen-Cahn equation. | |
| double precision | phase_field_energy_wall |
| Energy wall parameter in Allen-Cahn equation. | |
| double precision | phase_field_thickness |
| Thickness parameter in Allen-Cahn equation. | |
| logical | phase_field_is_isothermal = .false. |
| Activate manual setting of the undercooling energy. | |
Phase field linear system solver | |
| type(t_ls_map) | phase_field_ls_map |
| Mapping variables. | |
| class(t_linear_solver), allocatable | phase_field_solver |
| Linear system solver. | |
| class(t_scalar_initializer), allocatable | phase_field_initializer |
| Phase field initializer. | |
Phase change variables | |
| enum | { phase_change_iterative , phase_change_mof , phase_change_apparent_heat_capacity , phase_change_linearized_enthalpy , phase_change_phase_field } |
| integer | energy_phase_change_method = phase_change_iterative |
| Phase change method. | |
| integer | energy_phase_change_liquid_phase = 1 |
| Phase number of the liquid. | |
| integer | energy_phase_change_solid_phase = 2 |
| Phase number of the solid. | |
| integer | energy_phase_change_inert = 0 |
| Phase number of the inert phase (do not modify this value) | |
| integer | energy_phase_change_max_iter = 1 |
| Phase change max iteration. | |
| double precision | energy_melting_temperature = 0d0 |
| Melting temperature. | |
| double precision | energy_latent_heat = 0d0 |
| Latent heat. | |
| double precision | energy_phase_change_relaxation = 1d0 |
| Phase change relaxation factor (> 0.0) | |
| double precision | energy_phase_change_tolerance = epsilon(energy_phase_change_tolerance) |
| Phase change tolerance value. | |
| double precision | energy_phase_change_smoother = 1d0 |
| Phase change tolerance value. | |
Declaration of scalar variables associated to the Energy equation.
| anonymous enum |
| type(t_fv_flux), parameter variables_energy::default_energy_advection_explicit_flux = default_flux_godunov |
Fluxes type The default explicit cell advection flux.
| type(t_fv_flux) variables_energy::energy_advection_explicit_flux = default_energy_advection_explicit_flux |
Fluxes type The effective explicit cell advection flux.
| double precision variables_energy::energy_advection_scheme_stability_factor = -1d0 |
CFL used for explicit sub iterations (if is_energy_specify_advection_scheme_stability_factor, otherwize, using default values)
| logical variables_energy::energy_advection_term_dir_split = .false. |
Advection term: directional splitting option.
| integer variables_energy::energy_advection_term_discretization_type = implicit_discretization |
Advection term discretization type (implicit or explicit)
| integer variables_energy::energy_advection_term_scheme = cell_centered_o2_advection_scheme |
Advection term scheme.
| integer variables_energy::energy_advection_term_splitting_scheme = lie_trotter_splitting |
Advection term: Splitting Method for Lax-Wendroff TVD Superbee.
| class(t_cell_bc_initializer), pointer variables_energy::energy_bc_initializer => null() |
Boundary conditions initializer.
| type(t_boundary_condition) variables_energy::energy_boundary_condition |
Boundary condition.
| integer variables_energy::energy_diffusion_explicit_time_order_discretization = time_order_1 |
Diffusion term discretization (temporal discretization)
| integer variables_energy::energy_diffusion_term_discretization_type = implicit_discretization |
Diffusion term discretization type (implicit or explicit)
| integer variables_energy::energy_diffusion_term_scheme = cell_centered_o2_diffusion_scheme |
Diffusion term scheme.
| integer variables_energy::energy_enforced_stencil = -1 |
Enforced stencil.
| integer variables_energy::energy_equation_formulation = energy_equation_formulation_cp |
Has source term?
| integer variables_energy::energy_explicit_time_order_discretization = time_order_nssp32 |
Explicit time order discretization.
| logical variables_energy::energy_has_advection_term = .true. |
Has advection term?
| logical variables_energy::energy_has_diffusion_term = .true. |
Has diffusion term?
| logical variables_energy::energy_has_div_u_advection_term = .true. |
Has \( div(\mathbf{u}) \) advection term?
| logical variables_energy::energy_has_ghost_boundary_cells = .false. |
Ghost boudary cell choice.
| logical variables_energy::energy_has_immersed_boundaries = .false. |
Flag to enable immersed boundaries for the energy equation.
| logical variables_energy::energy_has_imposed_value = .false. |
Has imposed value (temperature)?
| logical variables_energy::energy_has_linear_term = .false. |
Has linear term?
| logical variables_energy::energy_has_linearized_enthalpy_compressible_gas_only = .false. |
Has compressible gas around PCM for the linearized enthalpy method?
| logical variables_energy::energy_has_linearized_enthalpy_conservative_advection = .false. |
Has explicit advection term for the linearized enthalpy method?
| logical variables_energy::energy_has_phase_change = .false. |
Has phase change?
| logical variables_energy::energy_has_phase_thermal_resistance = .false. |
Has phase resistance?
| logical variables_energy::energy_has_source_term = .false. |
Has source term?
| logical variables_energy::energy_has_temporal_term = .true. |
Has temporal term?
| logical variables_energy::energy_has_viscous_dissipation_rate_term = .false. |
Has viscous dissipation term?
| logical variables_energy::energy_ib_has_one_sided_inner_discretization |
One sided discretization close to immersed boundaries.
| integer, dimension(:), allocatable variables_energy::energy_ib_inner_discretization_order |
| class(t_energy_ibc_initializer_item), dimension(:), allocatable variables_energy::energy_ibc_initializer |
Immersed boundary conditions initializers.
| class(t_scalar_initializer), pointer variables_energy::energy_initializer => null() |
Initial condition initializer.
| integer, dimension(:), allocatable variables_energy::energy_isd_target |
List of enabled immersed boundaries for the energy equation.
| double precision variables_energy::energy_latent_heat = 0d0 |
Latent heat.
| class(t_scalar_initializer), pointer variables_energy::energy_linear_term_initializer => null() |
Linear term initializer.
| type(t_ls_map) variables_energy::energy_ls_map |
Mapping variables.
| double precision variables_energy::energy_melting_temperature = 0d0 |
Melting temperature.
| integer variables_energy::energy_phase_change_inert = 0 |
Phase number of the inert phase (do not modify this value)
| integer variables_energy::energy_phase_change_liquid_phase = 1 |
Phase number of the liquid.
| integer variables_energy::energy_phase_change_max_iter = 1 |
Phase change max iteration.
| integer variables_energy::energy_phase_change_method = phase_change_iterative |
Phase change method.
| double precision variables_energy::energy_phase_change_relaxation = 1d0 |
Phase change relaxation factor (> 0.0)
| double precision variables_energy::energy_phase_change_smoother = 1d0 |
Phase change tolerance value.
| integer variables_energy::energy_phase_change_solid_phase = 2 |
Phase number of the solid.
| double precision variables_energy::energy_phase_change_tolerance = epsilon(energy_phase_change_tolerance) |
Phase change tolerance value.
| double precision, dimension(:), allocatable variables_energy::energy_phase_thermal_resistance |
Resistance values.
| integer, dimension(:,:), allocatable variables_energy::energy_phase_thermal_resistance_index |
Interface index.
| class(t_linear_solver), allocatable variables_energy::energy_solver |
Linear system solver.
| class(t_scalar_initializer), pointer variables_energy::energy_source_term_initializer => null() |
Source term initializer.
| double precision, dimension (3) variables_energy::energy_splitting_time_coeff =1d0 |
| type(t_cell_stencil) variables_energy::energy_stencil |
Stencil of the energy equation.
| integer variables_energy::energy_time_order_discretization = time_order_1 |
Time order discretization.
| double precision variables_energy::energy_time_step = 0d0 |
Current Time step.
| double precision variables_energy::energy_time_step_n = 0d0 |
Previous time step.
| double precision variables_energy::energy_time_step_nm1 = 0d0 |
Previous -1 time step.
| logical variables_energy::energy_use_explicit_terms_accumulator = .false. |
A switch for when to use explicit accumulator.
| logical variables_energy::is_energy_fully_explicit = .false. |
Energy Equations Fully Explicit.
| logical variables_energy::is_energy_specify_advection_scheme_stability_factor = .false. |
Specify a CFL factor for explicit sub iterations.
| integer variables_energy::n_ibc_temperature = 0 |
Number of immersed boundaries enabled for the energy equation.
| double precision variables_energy::phase_field_energy_wall |
Energy wall parameter in Allen-Cahn equation.
| class(t_scalar_initializer), allocatable variables_energy::phase_field_initializer |
Phase field initializer.
| logical variables_energy::phase_field_is_isothermal = .false. |
Activate manual setting of the undercooling energy.
| type(t_ls_map) variables_energy::phase_field_ls_map |
Mapping variables.
| double precision variables_energy::phase_field_mobility |
Mobility parameter in Allen-Cahn equation.
| class(t_linear_solver), allocatable variables_energy::phase_field_solver |
Linear system solver.
| double precision variables_energy::phase_field_thickness |
Thickness parameter in Allen-Cahn equation.
| double precision, dimension(3) variables_energy::temperature_imposed_point = [0d0, 0d0, COORD_Z_2D] |
Imposed value.
| double precision variables_energy::temperature_imposed_value = huge(0d0) |