MPI-AMRVAC
3.1
The MPI - Adaptive Mesh Refinement - Versatile Advection Code (development version)
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Magneto-hydrodynamics module. More...
Data Types | |
interface | fun_kin_en |
Functions/Subroutines | |
subroutine | mhd_write_info (fh) |
Write this module's parameters to a snapsoht. More... | |
subroutine, public | mhd_phys_init () |
subroutine | mhd_te_images |
subroutine | mhd_sts_set_source_tc_mhd (ixIL, ixOL, w, x, wres, fix_conserve_at_step, my_dt, igrid, nflux) |
double precision function | mhd_get_tc_dt_mhd (w, ixIL, ixOL, dxD, x) |
subroutine | mhd_tc_handle_small_e (w, x, ixIL, ixOL, step) |
subroutine | tc_params_read_mhd (fl) |
subroutine | rc_params_read (fl) |
subroutine | set_equi_vars_grid_faces (igrid, x, ixIL, ixOL) |
sets the equilibrium variables More... | |
subroutine | set_equi_vars_grid (igrid) |
sets the equilibrium variables More... | |
double precision function, dimension(ixo^s, 1:nwc) | convert_vars_splitting (ixIL, ixOL, w, x, nwc) |
subroutine | mhd_check_params |
subroutine | mhd_physical_units () |
subroutine | mhd_check_w_semirelati (primitive, ixIL, ixOL, w, flag) |
subroutine | mhd_check_w_origin (primitive, ixIL, ixOL, w, flag) |
subroutine | mhd_check_w_inte (primitive, ixIL, ixOL, w, flag) |
subroutine | mhd_check_w_hde (primitive, ixIL, ixOL, w, flag) |
subroutine | mhd_to_conserved_origin (ixIL, ixOL, w, x) |
Transform primitive variables into conservative ones. More... | |
subroutine | mhd_to_conserved_hde (ixIL, ixOL, w, x) |
Transform primitive variables into conservative ones. More... | |
subroutine | mhd_to_conserved_inte (ixIL, ixOL, w, x) |
Transform primitive variables into conservative ones. More... | |
subroutine | mhd_to_conserved_split_rho (ixIL, ixOL, w, x) |
Transform primitive variables into conservative ones. More... | |
subroutine | mhd_to_conserved_semirelati (ixIL, ixOL, w, x) |
Transform primitive variables into conservative ones. More... | |
subroutine | mhd_to_primitive_origin (ixIL, ixOL, w, x) |
Transform conservative variables into primitive ones. More... | |
subroutine | mhd_to_primitive_hde (ixIL, ixOL, w, x) |
Transform conservative variables into primitive ones. More... | |
subroutine | mhd_to_primitive_inte (ixIL, ixOL, w, x) |
Transform conservative variables into primitive ones. More... | |
subroutine | mhd_to_primitive_split_rho (ixIL, ixOL, w, x) |
Transform conservative variables into primitive ones. More... | |
subroutine | mhd_to_primitive_semirelati (ixIL, ixOL, w, x) |
Transform conservative variables into primitive ones. More... | |
subroutine, public | mhd_ei_to_e (ixIL, ixOL, w, x) |
Transform internal energy to total energy. More... | |
subroutine | mhd_ei_to_e_hde (ixIL, ixOL, w, x) |
Transform internal energy to hydrodynamic energy. More... | |
subroutine | mhd_ei_to_e_semirelati (ixIL, ixOL, w, x) |
Transform internal energy to total energy and velocity to momentum. More... | |
subroutine, public | mhd_e_to_ei (ixIL, ixOL, w, x) |
Transform total energy to internal energy. More... | |
subroutine | mhd_e_to_ei_hde (ixIL, ixOL, w, x) |
Transform hydrodynamic energy to internal energy. More... | |
subroutine | mhd_e_to_ei_semirelati (ixIL, ixOL, w, x) |
Transform total energy to internal energy and momentum to velocity. More... | |
subroutine | mhd_handle_small_values_semirelati (primitive, w, x, ixIL, ixOL, subname) |
subroutine | mhd_handle_small_values_origin (primitive, w, x, ixIL, ixOL, subname) |
subroutine | mhd_handle_small_values_inte (primitive, w, x, ixIL, ixOL, subname) |
subroutine | mhd_handle_small_values_hde (primitive, w, x, ixIL, ixOL, subname) |
subroutine | mhd_get_v_origin (w, x, ixIL, ixOL, v) |
Calculate v vector. More... | |
subroutine | mhd_get_v_boris (w, x, ixIL, ixOL, v) |
Calculate v vector. More... | |
subroutine, public | mhd_get_v_idim (w, x, ixIL, ixOL, idim, v) |
Calculate v component. More... | |
subroutine | mhd_get_cmax_origin (w, x, ixIL, ixOL, idim, cmax) |
Calculate cmax_idim=csound+abs(v_idim) within ixO^L. More... | |
subroutine | mhd_get_cmax_semirelati (w, x, ixIL, ixOL, idim, cmax) |
Calculate cmax_idim for semirelativistic MHD. More... | |
subroutine | mhd_get_a2max (w, x, ixIL, ixOL, a2max) |
subroutine | mhd_get_tcutoff (ixIL, ixOL, w, x, Tco_local, Tmax_local) |
get adaptive cutoff temperature for TRAC (Johnston 2019 ApJL, 873, L22) More... | |
subroutine | mhd_get_h_speed (wprim, x, ixIL, ixOL, idim, Hspeed) |
get H speed for H-correction to fix the carbuncle problem at grid-aligned shock front More... | |
subroutine | mhd_get_cbounds (wLC, wRC, wLp, wRp, x, ixIL, ixOL, idim, Hspeed, cmax, cmin) |
Estimating bounds for the minimum and maximum signal velocities without split. More... | |
subroutine | mhd_get_cbounds_semirelati (wLC, wRC, wLp, wRp, x, ixIL, ixOL, idim, Hspeed, cmax, cmin) |
Estimating bounds for the minimum and maximum signal velocities without split. More... | |
subroutine | mhd_get_cbounds_split_rho (wLC, wRC, wLp, wRp, x, ixIL, ixOL, idim, Hspeed, cmax, cmin) |
Estimating bounds for the minimum and maximum signal velocities with rho split. More... | |
subroutine | mhd_get_ct_velocity (vcts, wLp, wRp, ixIL, ixOL, idim, cmax, cmin) |
prepare velocities for ct methods More... | |
subroutine | mhd_get_csound (w, x, ixIL, ixOL, idim, csound) |
Calculate fast magnetosonic wave speed. More... | |
subroutine | mhd_get_csound_prim (w, x, ixIL, ixOL, idim, csound) |
Calculate fast magnetosonic wave speed. More... | |
subroutine | mhd_get_csound_semirelati (w, x, ixIL, ixOL, idim, csound, gamma2) |
Calculate cmax_idim for semirelativistic MHD. More... | |
subroutine | mhd_get_pthermal_iso (w, x, ixIL, ixOL, pth) |
Calculate isothermal thermal pressure. More... | |
subroutine | mhd_get_pthermal_eint (w, x, ixIL, ixOL, pth) |
Calculate thermal pressure from internal energy. More... | |
subroutine | mhd_get_pthermal_origin (w, x, ixIL, ixOL, pth) |
Calculate thermal pressure=(gamma-1)*(e-0.5*m**2/rho-b**2/2) within ixO^L. More... | |
subroutine | mhd_get_pthermal_semirelati (w, x, ixIL, ixOL, pth) |
Calculate thermal pressure. More... | |
subroutine | mhd_get_pthermal_hde (w, x, ixIL, ixOL, pth) |
Calculate thermal pressure=(gamma-1)*(e-0.5*m**2/rho) within ixO^L. More... | |
subroutine | mhd_get_temperature_from_te (w, x, ixIL, ixOL, res) |
copy temperature from stored Te variable More... | |
subroutine | mhd_get_temperature_from_eint (w, x, ixIL, ixOL, res) |
Calculate temperature=p/rho when in e_ the internal energy is stored. More... | |
subroutine | mhd_get_temperature_from_etot (w, x, ixIL, ixOL, res) |
Calculate temperature=p/rho when in e_ the total energy is stored. More... | |
subroutine | mhd_get_temperature_from_etot_with_equi (w, x, ixIL, ixOL, res) |
subroutine | mhd_get_temperature_from_eint_with_equi (w, x, ixIL, ixOL, res) |
subroutine | mhd_get_temperature_equi (w, x, ixIL, ixOL, res) |
subroutine | mhd_get_rho_equi (w, x, ixIL, ixOL, res) |
subroutine | mhd_get_pe_equi (w, x, ixIL, ixOL, res) |
subroutine, public | mhd_get_csound2 (w, x, ixIL, ixOL, csound2) |
Calculate the square of the thermal sound speed csound2 within ixO^L. csound2=gamma*p/rho. More... | |
subroutine | mhd_get_p_total (w, x, ixIL, ixOL, p) |
Calculate total pressure within ixO^L including magnetic pressure. More... | |
subroutine | mhd_get_flux (wC, w, x, ixIL, ixOL, idim, f) |
Calculate fluxes within ixO^L without any splitting. More... | |
subroutine | mhd_get_flux_hde (wC, w, x, ixIL, ixOL, idim, f) |
Calculate fluxes within ixO^L without any splitting. More... | |
subroutine | mhd_get_flux_split (wC, w, x, ixIL, ixOL, idim, f) |
Calculate fluxes within ixO^L with possible splitting. More... | |
subroutine | mhd_get_flux_semirelati (wC, w, x, ixIL, ixOL, idim, f) |
Calculate semirelativistic fluxes within ixO^L without any splitting. More... | |
subroutine | add_source_ambipolar_internal_energy (qdt, ixIL, ixOL, wCT, w, x, ie) |
Source terms J.E in internal energy. For the ambipolar term E = ambiCoef * JxBxB=ambiCoef * B^2(-J_perpB) More... | |
subroutine | mhd_get_jxbxb (w, x, ixIL, ixOL, res) |
subroutine | sts_set_source_ambipolar (ixIL, ixOL, w, x, wres, fix_conserve_at_step, my_dt, igrid, nflux) |
Sets the sources for the ambipolar this is used for the STS method. More... | |
subroutine | update_faces_ambipolar (ixIL, ixOL, w, x, ECC, fE, circ) |
get ambipolar electric field and the integrals around cell faces More... | |
subroutine | get_flux_on_cell_face (ixIL, ixOL, ff, src) |
use cell-center flux to get cell-face flux and get the source term as the divergence of the flux More... | |
double precision function | get_ambipolar_dt (w, ixIL, ixOL, dxD, x) |
Calculates the explicit dt for the ambipokar term This function is used by both explicit scheme and STS method. More... | |
subroutine, public | multiplyambicoef (ixIL, ixOL, res, w, x) |
multiply res by the ambipolar coefficient The ambipolar coefficient is calculated as -mhd_eta_ambi/rho^2 The user may mask its value in the user file by implemneting usr_mask_ambipolar subroutine More... | |
subroutine | mhd_add_source (qdt, dtfactor, ixIL, ixOL, wCT, wCTprim, w, x, qsourcesplit, active) |
w[iws]=w[iws]+qdt*S[iws,wCT] where S is the source based on wCT within ixO More... | |
subroutine | add_pe0_divv (qdt, dtfactor, ixIL, ixOL, wCT, w, x) |
subroutine | get_lorentz_force (ixIL, ixOL, w, JxB) |
Compute the Lorentz force (JxB) More... | |
subroutine | mhd_gamma2_alfven (ixIL, ixOL, w, gamma_A2) |
Compute 1/(1+v_A^2/c^2) for semirelativistic MHD, where v_A is the Alfven velocity. More... | |
double precision function, dimension(ixo^s) | mhd_gamma_alfven (w, ixIL, ixOL) |
Compute 1/sqrt(1+v_A^2/c^2) for semirelativisitic MHD, where v_A is the Alfven velocity. More... | |
subroutine, public | mhd_get_rho (w, x, ixIL, ixOL, rho) |
subroutine | mhd_handle_small_ei (w, x, ixIL, ixOL, ie, subname) |
handle small or negative internal energy More... | |
subroutine | mhd_update_temperature (ixIL, ixOL, wCT, w, x) |
subroutine | add_source_b0split (qdt, dtfactor, ixIL, ixOL, wCT, w, x) |
Source terms after split off time-independent magnetic field. More... | |
subroutine | add_source_semirelativistic (qdt, ixIL, ixOL, wCT, w, x, wCTprim) |
Source terms for semirelativistic MHD Gombosi 2002 JCP 177, 176. More... | |
subroutine | add_source_internal_e (qdt, ixIL, ixOL, wCT, w, x, wCTprim) |
Source terms for internal energy version of MHD. More... | |
subroutine | add_source_hydrodynamic_e (qdt, ixIL, ixOL, wCT, w, x, wCTprim) |
Source terms for hydrodynamic energy version of MHD. More... | |
subroutine | add_source_res1 (qdt, ixIL, ixOL, wCT, w, x) |
Add resistive source to w within ixO Uses 3 point stencil (1 neighbour) in each direction, non-conservative. If the fourthorder precompiler flag is set, uses fourth order central difference for the laplacian. Then the stencil is 5 (2 neighbours). More... | |
subroutine | add_source_res2 (qdt, ixIL, ixOL, wCT, w, x) |
Add resistive source to w within ixO Uses 5 point stencil (2 neighbours) in each direction, conservative. More... | |
subroutine | add_source_hyperres (qdt, ixIL, ixOL, wCT, w, x) |
Add Hyper-resistive source to w within ixO Uses 9 point stencil (4 neighbours) in each direction. More... | |
subroutine | add_source_glm (qdt, ixIL, ixOL, wCT, w, x) |
subroutine | add_source_powel (qdt, ixIL, ixOL, wCT, w, x) |
Add divB related sources to w within ixO corresponding to Powel. More... | |
subroutine | add_source_janhunen (qdt, ixIL, ixOL, wCT, w, x) |
subroutine | add_source_linde (qdt, ixIL, ixOL, wCT, w, x) |
subroutine, public | get_divb (w, ixIL, ixOL, divb, fourthorder) |
Calculate div B within ixO. More... | |
subroutine, public | get_normalized_divb (w, ixIL, ixOL, divb) |
get dimensionless div B = |divB| * volume / area / |B| More... | |
subroutine, public | get_current (w, ixIL, ixOL, idirmin, current) |
Calculate idirmin and the idirmin:3 components of the common current array make sure that dxlevel(^D) is set correctly. More... | |
subroutine | mhd_get_dt (w, ixIL, ixOL, dtnew, dxD, x) |
If resistivity is not zero, check diffusion time limit for dt. More... | |
subroutine | mhd_add_source_geom (qdt, dtfactor, ixIL, ixOL, wCT, w, x) |
subroutine | mhd_add_source_geom_split (qdt, dtfactor, ixIL, ixOL, wCT, w, x) |
double precision function, dimension(ixo^s), public | mhd_mag_en_all (w, ixIL, ixOL) |
Compute 2 times total magnetic energy. More... | |
double precision function, dimension(ixo^s) | mhd_mag_i_all (w, ixIL, ixOL, idir) |
Compute full magnetic field by direction. More... | |
double precision function, dimension(ixo^s) | mhd_mag_en (w, ixIL, ixOL) |
Compute evolving magnetic energy. More... | |
double precision function, dimension(ixo^s) | mhd_kin_en_origin (w, ixIL, ixOL, inv_rho) |
compute kinetic energy More... | |
double precision function, dimension(ixo^s) | mhd_kin_en_boris (w, ixIL, ixOL, inv_rho) |
compute kinetic energy More... | |
subroutine | mhd_getv_hall (w, x, ixIL, ixOL, vHall) |
subroutine | mhd_get_jambi (w, x, ixIL, ixOL, res) |
subroutine | mhd_modify_wlr (ixIL, ixOL, qt, wLC, wRC, wLp, wRp, s, idir) |
subroutine | mhd_boundary_adjust (igrid, psb) |
subroutine | fixdivb_boundary (ixGL, ixOL, w, x, iB) |
subroutine, public | mhd_clean_divb_multigrid (qdt, qt, active) |
subroutine | mhd_update_faces (ixIL, ixOL, qt, qdt, wprim, fC, fE, sCT, s, vcts) |
subroutine | update_faces_average (ixIL, ixOL, qt, qdt, fC, fE, sCT, s) |
get electric field though averaging neighors to update faces in CT More... | |
subroutine | update_faces_contact (ixIL, ixOL, qt, qdt, wp, fC, fE, sCT, s, vcts) |
update faces using UCT contact mode by Gardiner and Stone 2005 JCP 205, 509 More... | |
subroutine | update_faces_hll (ixIL, ixOL, qt, qdt, fE, sCT, s, vcts) |
update faces More... | |
subroutine | get_resistive_electric_field (ixIL, ixOL, sCT, s, jce) |
calculate eta J at cell edges More... | |
subroutine | get_ambipolar_electric_field (ixIL, ixOL, w, x, fE) |
get ambipolar electric field on cell edges More... | |
subroutine, public | mhd_face_to_center (ixOL, s) |
calculate cell-center values from face-center values More... | |
subroutine, public | b_from_vector_potential (ixIsL, ixIL, ixOL, ws, x) |
calculate magnetic field from vector potential More... | |
subroutine | rfactor_from_temperature_ionization (w, x, ixIL, ixOL, Rfactor) |
subroutine | rfactor_from_constant_ionization (w, x, ixIL, ixOL, Rfactor) |
Variables | |
logical, public, protected | mhd_energy = .true. |
Whether an energy equation is used. More... | |
logical, public, protected | mhd_thermal_conduction = .false. |
Whether thermal conduction is used. More... | |
type(tc_fluid), allocatable, public | tc_fl |
type of fluid for thermal conduction More... | |
type(te_fluid), allocatable, public | te_fl_mhd |
type of fluid for thermal emission synthesis More... | |
logical, public, protected | mhd_radiative_cooling = .false. |
Whether radiative cooling is added. More... | |
type(rc_fluid), allocatable, public | rc_fl |
type of fluid for radiative cooling More... | |
logical, public, protected | mhd_viscosity = .false. |
Whether viscosity is added. More... | |
logical, public, protected | mhd_gravity = .false. |
Whether gravity is added. More... | |
logical, public, protected | mhd_rotating_frame = .false. |
Whether rotating frame is activated. More... | |
logical, public, protected | mhd_hall = .false. |
Whether Hall-MHD is used. More... | |
logical, public, protected | mhd_ambipolar = .false. |
Whether Ambipolar term is used. More... | |
logical, public, protected | mhd_ambipolar_sts = .false. |
Whether Ambipolar term is implemented using supertimestepping. More... | |
logical, public, protected | mhd_ambipolar_exp = .false. |
Whether Ambipolar term is implemented explicitly. More... | |
logical, public, protected | mhd_particles = .false. |
Whether particles module is added. More... | |
logical, public, protected | mhd_magnetofriction = .false. |
Whether magnetofriction is added. More... | |
logical, public, protected | mhd_glm = .false. |
Whether GLM-MHD is used to control div B. More... | |
logical, public, protected | mhd_glm_extended = .true. |
Whether extended GLM-MHD is used with additional sources. More... | |
logical, public, protected | mhd_trac = .false. |
Whether TRAC method is used. More... | |
integer, public, protected | mhd_trac_type =1 |
Which TRAC method is used. More... | |
double precision, public, protected | mhd_trac_mask = 0.d0 |
Height of the mask used in the TRAC method. More... | |
integer, public, protected | mhd_trac_finegrid =4 |
Distance between two adjacent traced magnetic field lines (in finest cell size) More... | |
logical, public, protected | mhd_internal_e = .false. |
Whether internal energy is solved instead of total energy. More... | |
logical, public, protected | mhd_hydrodynamic_e = .false. |
Whether hydrodynamic energy is solved instead of total energy. More... | |
logical, public, protected | source_split_divb = .false. |
Whether divB cleaning sources are added splitting from fluid solver. More... | |
double precision, public | mhd_glm_alpha = 0.5d0 |
GLM-MHD parameter: ratio of the diffusive and advective time scales for div b taking values within [0, 1]. More... | |
logical, public, protected | mhd_semirelativistic = .false. |
Whether semirelativistic MHD equations (Gombosi 2002 JCP) are solved. More... | |
logical, public, protected | mhd_boris_simplification = .false. |
Whether boris simplified semirelativistic MHD equations (Gombosi 2002 JCP) are solved. More... | |
double precision, public, protected | mhd_reduced_c = 0.02d0*const_c |
Reduced speed of light for semirelativistic MHD: 2% of light speed. More... | |
logical, public, protected | mhd_partial_ionization = .false. |
Whether plasma is partially ionized. More... | |
logical, public, protected | mhd_cak_force = .false. |
Whether CAK radiation line force is activated. More... | |
logical, public, protected | mhd_4th_order = .false. |
MHD fourth order. More... | |
logical, public | has_equi_rho0 = .false. |
whether split off equilibrium density More... | |
logical, public | has_equi_pe0 = .false. |
whether split off equilibrium thermal pressure More... | |
logical, public | mhd_equi_thermal = .false. |
integer, public | equi_rho0_ = -1 |
equi vars indices in the stateequi_vars array More... | |
integer, public | equi_pe0_ = -1 |
logical, public, protected | mhd_dump_full_vars = .false. |
whether dump full variables (when splitting is used) in a separate dat file More... | |
integer, public, protected | mhd_n_tracer = 0 |
Number of tracer species. More... | |
integer, public, protected | rho_ |
Index of the density (in the w array) More... | |
integer, dimension(:), allocatable, public, protected | mom |
Indices of the momentum density. More... | |
integer, public, protected | e_ |
Index of the energy density (-1 if not present) More... | |
integer, public, protected | p_ |
Index of the gas pressure (-1 if not present) should equal e_. More... | |
integer, dimension(:), allocatable, public, protected | mag |
Indices of the magnetic field. More... | |
integer, public, protected | psi_ |
Indices of the GLM psi. More... | |
integer, public, protected | te_ |
Indices of temperature. More... | |
integer, public, protected | tcoff_ |
Index of the cutoff temperature for the TRAC method. More... | |
integer, public, protected | tweight_ |
integer, dimension(:), allocatable, public, protected | tracer |
Indices of the tracers. More... | |
double precision, public | mhd_gamma = 5.d0/3.0d0 |
The adiabatic index. More... | |
double precision, public | mhd_adiab = 1.0d0 |
The adiabatic constant. More... | |
double precision, public | mhd_eta = 0.0d0 |
The MHD resistivity. More... | |
double precision, public | mhd_eta_hyper = 0.0d0 |
The MHD hyper-resistivity. More... | |
double precision, public | mhd_etah = 0.0d0 |
TODO: what is this? More... | |
double precision, public | mhd_eta_ambi = 0.0d0 |
The MHD ambipolar coefficient. More... | |
character(len=std_len), public, protected | typedivbfix = 'linde' |
Method type to clean divergence of B. More... | |
character(len=std_len), public, protected | type_ct = 'uct_contact' |
Method type of constrained transport. More... | |
logical, public, protected | mhd_divb_4thorder = .false. |
Whether divB is computed with a fourth order approximation. More... | |
logical, public | divbwave = .true. |
Add divB wave in Roe solver. More... | |
logical, public | clean_initial_divb = .false. |
clean initial divB More... | |
double precision, public, protected | he_abundance =0.1d0 |
Helium abundance over Hydrogen. More... | |
double precision, public, protected | h_ion_fr =1d0 |
Ionization fraction of H H_ion_fr = H+/(H+ + H) More... | |
double precision, public, protected | he_ion_fr =1d0 |
Ionization fraction of He He_ion_fr = (He2+ + He+)/(He2+ + He+ + He) More... | |
double precision, public, protected | he_ion_fr2 =1d0 |
Ratio of number He2+ / number He+ + He2+ He_ion_fr2 = He2+/(He2+ + He+) More... | |
double precision, public, protected | rr =1d0 |
logical, public, protected | eq_state_units = .true. |
logical, dimension(2 *^nd), public, protected | boundary_divbfix =.true. |
To control divB=0 fix for boundary. More... | |
integer, dimension(2 *^nd), public, protected | boundary_divbfix_skip =0 |
To skip * layer of ghost cells during divB=0 fix for boundary. More... | |
logical, public, protected | b0field_forcefree =.true. |
B0 field is force-free. More... | |
procedure(mask_subroutine), pointer, public | usr_mask_ambipolar => null() |
procedure(sub_convert), pointer, public | mhd_to_primitive => null() |
procedure(sub_convert), pointer, public | mhd_to_conserved => null() |
procedure(sub_get_pthermal), pointer, public | mhd_get_pthermal => null() |
procedure(sub_get_pthermal), pointer, public | mhd_get_temperature => null() |
procedure(sub_get_v), pointer, public | mhd_get_v => null() |
procedure(fun_kin_en), pointer, public | mhd_kin_en => null() |
Magneto-hydrodynamics module.
subroutine mod_mhd_phys::add_pe0_divv | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | dtfactor, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::add_source_ambipolar_internal_energy | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ie | ||
) |
Source terms J.E in internal energy. For the ambipolar term E = ambiCoef * JxBxB=ambiCoef * B^2(-J_perpB)
ambiCoef is calculated as mhd_ambi_coef/rho^2, see also the subroutine mhd_get_Jambi
Definition at line 3968 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_b0split | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | dtfactor, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Source terms after split off time-independent magnetic field.
Definition at line 4620 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_glm | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::add_source_hydrodynamic_e | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:nw), intent(in), optional | wCTprim | ||
) |
Source terms for hydrodynamic energy version of MHD.
Definition at line 4765 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_hyperres | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Add Hyper-resistive source to w within ixO Uses 9 point stencil (4 neighbours) in each direction.
Definition at line 5053 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_internal_e | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:nw), intent(in) | wCTprim | ||
) |
Source terms for internal energy version of MHD.
Definition at line 4733 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_janhunen | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::add_source_linde | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::add_source_powel | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Add divB related sources to w within ixO corresponding to Powel.
Definition at line 5166 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_res1 | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Add resistive source to w within ixO Uses 3 point stencil (1 neighbour) in each direction, non-conservative. If the fourthorder precompiler flag is set, uses fourth order central difference for the laplacian. Then the stencil is 5 (2 neighbours).
Definition at line 4875 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_res2 | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Add resistive source to w within ixO Uses 5 point stencil (2 neighbours) in each direction, conservative.
Definition at line 4983 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::add_source_semirelativistic | ( | double precision, intent(in) | qdt, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:nw), intent(in), optional | wCTprim | ||
) |
Source terms for semirelativistic MHD Gombosi 2002 JCP 177, 176.
Definition at line 4690 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::b_from_vector_potential | ( | integer, intent(in) | ixIs, |
integer, intent(in) | L, | ||
integer, intent(in) | ixI, | ||
L, | |||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixis^s,1:nws), intent(inout) | ws, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
calculate magnetic field from vector potential
Definition at line 7168 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s, 1:nwc) mod_mhd_phys::convert_vars_splitting | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, 1:nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | nwc | ||
) |
subroutine mod_mhd_phys::fixdivb_boundary | ( | integer, intent(in) | ixG, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixg^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixg^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | iB | ||
) |
double precision function mod_mhd_phys::get_ambipolar_dt | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | dx, | ||
double precision, intent(in) | D, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
Calculates the explicit dt for the ambipokar term This function is used by both explicit scheme and STS method.
Definition at line 4239 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::get_ambipolar_electric_field | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(out) | fE | ||
) |
get ambipolar electric field on cell edges
Definition at line 7075 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::get_current | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(out) | idirmin, | ||
double precision, dimension(ixi^s,7-2*ndir:3) | current | ||
) |
Calculate idirmin and the idirmin:3 components of the common current array make sure that dxlevel(^D) is set correctly.
Definition at line 5365 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::get_divb | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(inout) | divb, | ||
logical, intent(in), optional | fourthorder | ||
) |
Calculate div B within ixO.
Definition at line 5300 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::get_flux_on_cell_face | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(:^d&,:), intent(inout) | ff, | ||
double precision, dimension(ixi^s), intent(out) | src | ||
) |
use cell-center flux to get cell-face flux and get the source term as the divergence of the flux
Definition at line 4184 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::get_lorentz_force | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | w, | ||
double precision, dimension(ixi^s,3), intent(inout) | JxB | ||
) |
Compute the Lorentz force (JxB)
Definition at line 4485 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::get_normalized_divb | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s) | divb | ||
) |
get dimensionless div B = |divB| * volume / area / |B|
Definition at line 5331 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::get_resistive_electric_field | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
type(state), intent(in) | sCT, | ||
type(state), intent(in) | s, | ||
double precision, dimension(ixi^s,7-2*ndim:3) | jce | ||
) |
calculate eta J at cell edges
Definition at line 7006 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_add_source | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | dtfactor, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(in) | wCTprim, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
logical, intent(in) | qsourcesplit, | ||
logical, intent(inout) | active | ||
) |
w[iws]=w[iws]+qdt*S[iws,wCT] where S is the source based on wCT within ixO
Definition at line 4291 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_add_source_geom | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | dtfactor, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(inout) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::mhd_add_source_geom_split | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | dtfactor, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(inout) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::mhd_boundary_adjust | ( | integer, intent(in) | igrid, |
type(state), dimension(max_blocks), target | psb | ||
) |
subroutine mod_mhd_phys::mhd_check_params |
subroutine mod_mhd_phys::mhd_check_w_hde | ( | logical, intent(in) | primitive, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
logical, dimension(ixi^s,1:nw), intent(inout) | flag | ||
) |
Definition at line 1434 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_check_w_inte | ( | logical, intent(in) | primitive, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
logical, dimension(ixi^s,1:nw), intent(inout) | flag | ||
) |
Definition at line 1397 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_check_w_origin | ( | logical, intent(in) | primitive, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
logical, dimension(ixi^s,1:nw), intent(inout) | flag | ||
) |
subroutine mod_mhd_phys::mhd_check_w_semirelati | ( | logical, intent(in) | primitive, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
logical, dimension(ixi^s,1:nw), intent(inout) | flag | ||
) |
Definition at line 1292 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_clean_divb_multigrid | ( | double precision, intent(in) | qdt, |
double precision, intent(in) | qt, | ||
logical, intent(inout) | active | ||
) |
[in] | qdt | Current time step |
[in] | qt | Current time |
[in,out] | active | Output if the source is active |
Definition at line 6349 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_e_to_ei | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform total energy to internal energy.
Definition at line 1909 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_e_to_ei_hde | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform hydrodynamic energy to internal energy.
Definition at line 1927 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_e_to_ei_semirelati | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform total energy to internal energy and momentum to velocity.
Definition at line 1943 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_ei_to_e | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform internal energy to total energy.
Definition at line 1871 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_ei_to_e_hde | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform internal energy to hydrodynamic energy.
Definition at line 1885 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_ei_to_e_semirelati | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform internal energy to total energy and velocity to momentum.
Definition at line 1897 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_face_to_center | ( | integer, intent(in) | ixO, |
integer, intent(in) | L, | ||
type(state) | s | ||
) |
calculate cell-center values from face-center values
Definition at line 7108 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_gamma2_alfven | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(in) | w, | ||
double precision, dimension(ixo^s), intent(out) | gamma_A2 | ||
) |
Compute 1/(1+v_A^2/c^2) for semirelativistic MHD, where v_A is the Alfven velocity.
Definition at line 4513 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s) mod_mhd_phys::mhd_gamma_alfven | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L | |||
) |
Compute 1/sqrt(1+v_A^2/c^2) for semirelativisitic MHD, where v_A is the Alfven velocity.
Definition at line 4532 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_a2max | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ndim), intent(inout) | a2max | ||
) |
4th order
Definition at line 2467 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_cbounds | ( | double precision, dimension(ixi^s, nw), intent(in) | wLC, |
double precision, dimension(ixi^s, nw), intent(in) | wRC, | ||
double precision, dimension(ixi^s, nw), intent(in) | wLp, | ||
double precision, dimension(ixi^s, nw), intent(in) | wRp, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,1:number_species), intent(in) | Hspeed, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout) | cmax, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout), optional | cmin | ||
) |
Estimating bounds for the minimum and maximum signal velocities without split.
Definition at line 2709 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_cbounds_semirelati | ( | double precision, dimension(ixi^s, nw), intent(in) | wLC, |
double precision, dimension(ixi^s, nw), intent(in) | wRC, | ||
double precision, dimension(ixi^s, nw), intent(in) | wLp, | ||
double precision, dimension(ixi^s, nw), intent(in) | wRp, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,1:number_species), intent(in) | Hspeed, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout) | cmax, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout), optional | cmin | ||
) |
Estimating bounds for the minimum and maximum signal velocities without split.
Definition at line 2788 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_cbounds_split_rho | ( | double precision, dimension(ixi^s, nw), intent(in) | wLC, |
double precision, dimension(ixi^s, nw), intent(in) | wRC, | ||
double precision, dimension(ixi^s, nw), intent(in) | wLp, | ||
double precision, dimension(ixi^s, nw), intent(in) | wRp, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,1:number_species), intent(in) | Hspeed, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout) | cmax, | ||
double precision, dimension(ixi^s,1:number_species), intent(inout), optional | cmin | ||
) |
Estimating bounds for the minimum and maximum signal velocities with rho split.
Definition at line 2815 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_cmax_origin | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(inout) | cmax | ||
) |
Calculate cmax_idim=csound+abs(v_idim) within ixO^L.
Definition at line 2401 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_cmax_semirelati | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(inout) | cmax | ||
) |
Calculate cmax_idim for semirelativistic MHD.
Definition at line 2417 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_csound | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(out) | csound | ||
) |
Calculate fast magnetosonic wave speed.
Definition at line 2948 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_get_csound2 | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | csound2 | ||
) |
Calculate the square of the thermal sound speed csound2 within ixO^L. csound2=gamma*p/rho.
Definition at line 3393 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_csound_prim | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(out) | csound | ||
) |
Calculate fast magnetosonic wave speed.
Definition at line 2996 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_csound_semirelati | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixo^s), intent(out) | csound, | ||
double precision, dimension(ixo^s), intent(out) | gamma2 | ||
) |
Calculate cmax_idim for semirelativistic MHD.
Definition at line 3051 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_ct_velocity | ( | type(ct_velocity), intent(inout) | vcts, |
double precision, dimension(ixi^s, nw), intent(in) | wLp, | ||
double precision, dimension(ixi^s, nw), intent(in) | wRp, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(in) | cmax, | ||
double precision, dimension(ixi^s), intent(in), optional | cmin | ||
) |
prepare velocities for ct methods
Definition at line 2895 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_dt | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(inout) | dtnew, | ||
double precision, intent(in) | dx, | ||
double precision, intent(in) | D, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
If resistivity is not zero, check diffusion time limit for dt.
Definition at line 5386 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_flux | ( | double precision, dimension(ixi^s,nw), intent(in) | wC, |
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,nwflux), intent(out) | f | ||
) |
Calculate fluxes within ixO^L without any splitting.
Definition at line 3426 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_flux_hde | ( | double precision, dimension(ixi^s,nw), intent(in) | wC, |
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,nwflux), intent(out) | f | ||
) |
Calculate fluxes within ixO^L without any splitting.
Definition at line 3558 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_flux_semirelati | ( | double precision, dimension(ixi^s,nw), intent(in) | wC, |
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,nwflux), intent(out) | f | ||
) |
Calculate semirelativistic fluxes within ixO^L without any splitting.
Definition at line 3851 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_flux_split | ( | double precision, dimension(ixi^s,nw), intent(in) | wC, |
double precision, dimension(ixi^s,nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,nwflux), intent(out) | f | ||
) |
Calculate fluxes within ixO^L with possible splitting.
Definition at line 3669 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_h_speed | ( | double precision, dimension(ixi^s, nw), intent(in) | wprim, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s,1:number_species), intent(out) | Hspeed | ||
) |
get H speed for H-correction to fix the carbuncle problem at grid-aligned shock front
Definition at line 2663 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_jambi | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(:^d&,:), intent(inout), allocatable | res | ||
) |
subroutine mod_mhd_phys::mhd_get_jxbxb | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(:^d&,:), intent(out) | res | ||
) |
subroutine mod_mhd_phys::mhd_get_p_total | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | p | ||
) |
Calculate total pressure within ixO^L including magnetic pressure.
Definition at line 3411 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pe_equi | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Definition at line 3382 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pthermal_eint | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | pth | ||
) |
Calculate thermal pressure from internal energy.
Definition at line 3116 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pthermal_hde | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | pth | ||
) |
Calculate thermal pressure=(gamma-1)*(e-0.5*m**2/rho) within ixO^L.
Definition at line 3248 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pthermal_iso | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | pth | ||
) |
Calculate isothermal thermal pressure.
Definition at line 3102 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pthermal_origin | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | pth | ||
) |
Calculate thermal pressure=(gamma-1)*(e-0.5*m**2/rho-b**2/2) within ixO^L.
Definition at line 3162 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_pthermal_semirelati | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | pth | ||
) |
Calculate thermal pressure.
Definition at line 3210 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_get_rho | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | rho | ||
) |
Definition at line 4542 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_rho_equi | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Definition at line 3373 of file mod_mhd_phys.t.
double precision function mod_mhd_phys::mhd_get_tc_dt_mhd | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | dx, | ||
double precision, intent(in) | D, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::mhd_get_tcutoff | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, intent(out) | Tco_local, | ||
double precision, intent(out) | Tmax_local | ||
) |
get adaptive cutoff temperature for TRAC (Johnston 2019 ApJL, 873, L22)
test case, fixed cutoff temperature
iijima et al. 2021, LTRAC method
test case, fixed cutoff temperature
iijima et al. 2021, LTRAC method
do nothing here
Definition at line 2490 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_equi | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Definition at line 3359 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_from_eint | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Calculate temperature=p/rho when in e_ the internal energy is stored.
Definition at line 3300 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_from_eint_with_equi | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Definition at line 3344 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_from_etot | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Calculate temperature=p/rho when in e_ the total energy is stored.
Definition at line 3314 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_from_etot_with_equi | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
Definition at line 3329 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_temperature_from_te | ( | double precision, dimension(ixi^s, 1:nw), intent(in) | w, |
double precision, dimension(ixi^s, 1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | res | ||
) |
copy temperature from stored Te variable
Definition at line 3290 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_v_boris | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,ndir), intent(out) | v | ||
) |
Calculate v vector.
Definition at line 2358 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_get_v_idim | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idim, | ||
double precision, dimension(ixi^s), intent(out) | v | ||
) |
Calculate v component.
Definition at line 2380 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_get_v_origin | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,ndir), intent(out) | v | ||
) |
Calculate v vector.
Definition at line 2337 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_getv_hall | ( | double precision, dimension(ixi^s,nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:3), intent(inout) | vHall | ||
) |
subroutine mod_mhd_phys::mhd_handle_small_ei | ( | double precision, dimension(ixi^s,1:nw), intent(inout) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | ie, | ||
character(len=*), intent(in) | subname | ||
) |
handle small or negative internal energy
Definition at line 4557 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_handle_small_values_hde | ( | logical, intent(in) | primitive, |
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
character(len=*), intent(in) | subname | ||
) |
subroutine mod_mhd_phys::mhd_handle_small_values_inte | ( | logical, intent(in) | primitive, |
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
character(len=*), intent(in) | subname | ||
) |
subroutine mod_mhd_phys::mhd_handle_small_values_origin | ( | logical, intent(in) | primitive, |
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
character(len=*), intent(in) | subname | ||
) |
subroutine mod_mhd_phys::mhd_handle_small_values_semirelati | ( | logical, intent(in) | primitive, |
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
character(len=*), intent(in) | subname | ||
) |
Definition at line 1954 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s) mod_mhd_phys::mhd_kin_en_boris | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixo^s), intent(in), optional | inv_rho | ||
) |
compute kinetic energy
Definition at line 5784 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s) mod_mhd_phys::mhd_kin_en_origin | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixo^s), intent(in), optional | inv_rho | ||
) |
compute kinetic energy
Definition at line 5765 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s) mod_mhd_phys::mhd_mag_en | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L | |||
) |
Compute evolving magnetic energy.
Definition at line 5755 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s), public mod_mhd_phys::mhd_mag_en_all | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L | |||
) |
Compute 2 times total magnetic energy.
Definition at line 5727 of file mod_mhd_phys.t.
double precision function, dimension(ixo^s) mod_mhd_phys::mhd_mag_i_all | ( | double precision, dimension(ixi^s, nw), intent(in) | w, |
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | idir | ||
) |
Compute full magnetic field by direction.
Definition at line 5741 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_modify_wlr | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | qt, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wLC, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wRC, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wLp, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wRp, | ||
type(state) | s, | ||
integer, intent(in) | idir | ||
) |
Definition at line 5879 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::mhd_phys_init |
Definition at line 365 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_physical_units |
Definition at line 1214 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_sts_set_source_tc_mhd | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wres, | ||
logical, intent(in) | fix_conserve_at_step, | ||
double precision, intent(in) | my_dt, | ||
integer, intent(in) | igrid, | ||
integer, intent(in) | nflux | ||
) |
subroutine mod_mhd_phys::mhd_tc_handle_small_e | ( | double precision, dimension(ixi^s,1:nw), intent(inout) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
integer, intent(in) | step | ||
) |
subroutine mod_mhd_phys::mhd_te_images |
subroutine mod_mhd_phys::mhd_to_conserved_hde | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform primitive variables into conservative ones.
Definition at line 1494 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_conserved_inte | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform primitive variables into conservative ones.
Definition at line 1525 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_conserved_origin | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform primitive variables into conservative ones.
Definition at line 1458 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_conserved_semirelati | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform primitive variables into conservative ones.
Definition at line 1596 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_conserved_split_rho | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform primitive variables into conservative ones.
Definition at line 1555 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_primitive_hde | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform conservative variables into primitive ones.
Definition at line 1690 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_primitive_inte | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform conservative variables into primitive ones.
Definition at line 1727 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_primitive_origin | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform conservative variables into primitive ones.
Definition at line 1651 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_primitive_semirelati | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform conservative variables into primitive ones.
Definition at line 1804 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_to_primitive_split_rho | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s, nw), intent(inout) | w, | ||
double precision, dimension(ixi^s, 1:ndim), intent(in) | x | ||
) |
Transform conservative variables into primitive ones.
Definition at line 1764 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::mhd_update_faces | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | qt, | ||
double precision, intent(in) | qdt, | ||
double precision, dimension(ixi^s,1:nw), intent(in) | wprim, | ||
double precision, dimension(ixi^s,1:nwflux,1:ndim), intent(in) | fC, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(inout) | fE, | ||
type(state) | sCT, | ||
type(state) | s, | ||
type(ct_velocity) | vcts | ||
) |
subroutine mod_mhd_phys::mhd_update_temperature | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | wCT, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
subroutine mod_mhd_phys::mhd_write_info | ( | integer, intent(in) | fh | ) |
Write this module's parameters to a snapsoht.
Definition at line 348 of file mod_mhd_phys.t.
subroutine, public mod_mhd_phys::multiplyambicoef | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(inout) | res, | ||
double precision, dimension(ixi^s,1:nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x | ||
) |
multiply res by the ambipolar coefficient The ambipolar coefficient is calculated as -mhd_eta_ambi/rho^2 The user may mask its value in the user file by implemneting usr_mask_ambipolar subroutine
Definition at line 4272 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::rc_params_read | ( | type(rc_fluid), intent(inout) | fl | ) |
Name of cooling curve
Name of cooling method
Fixed temperature not lower than tlow
Lower limit of temperature
Add cooling source in a split way (.true.) or un-split way (.false.)
Definition at line 1047 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::rfactor_from_constant_ionization | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | Rfactor | ||
) |
Definition at line 7198 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::rfactor_from_temperature_ionization | ( | double precision, dimension(ixi^s,1:nw), intent(in) | w, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s), intent(out) | Rfactor | ||
) |
subroutine mod_mhd_phys::set_equi_vars_grid | ( | integer, intent(in) | igrid | ) |
sets the equilibrium variables
Definition at line 1136 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::set_equi_vars_grid_faces | ( | integer, intent(in) | igrid, |
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
integer, intent(in) | ixI, | ||
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L | |||
) |
sets the equilibrium variables
Definition at line 1092 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::sts_set_source_ambipolar | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(inout) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:nw), intent(inout) | wres, | ||
logical, intent(in) | fix_conserve_at_step, | ||
double precision, intent(in) | my_dt, | ||
integer, intent(in) | igrid, | ||
integer, intent(in) | nflux | ||
) |
Sets the sources for the ambipolar this is used for the STS method.
at the corresponding indices store_flux_var is explicitly called for each of the fluxes one by one
Definition at line 4025 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::tc_params_read_mhd | ( | type(tc_fluid), intent(inout) | fl | ) |
Definition at line 1017 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::update_faces_ambipolar | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, dimension(ixi^s,1:nw), intent(in) | w, | ||
double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
double precision, dimension(ixi^s,1:3), intent(in) | ECC, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(out) | fE, | ||
double precision, dimension(ixi^s,1:ndim), intent(out) | circ | ||
) |
get ambipolar electric field and the integrals around cell faces
Definition at line 4130 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::update_faces_average | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | qt, | ||
double precision, intent(in) | qdt, | ||
double precision, dimension(ixi^s,1:nwflux,1:ndim), intent(in) | fC, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(inout) | fE, | ||
type(state) | sCT, | ||
type(state) | s | ||
) |
get electric field though averaging neighors to update faces in CT
Definition at line 6526 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::update_faces_contact | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | qt, | ||
double precision, intent(in) | qdt, | ||
double precision, dimension(ixi^s,1:nw), intent(in) | wp, | ||
double precision, dimension(ixi^s,1:nwflux,1:ndim), intent(in) | fC, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(inout) | fE, | ||
type(state) | sCT, | ||
type(state) | s, | ||
type(ct_velocity) | vcts | ||
) |
update faces using UCT contact mode by Gardiner and Stone 2005 JCP 205, 509
Definition at line 6625 of file mod_mhd_phys.t.
subroutine mod_mhd_phys::update_faces_hll | ( | integer, intent(in) | ixI, |
integer, intent(in) | L, | ||
integer, intent(in) | ixO, | ||
L, | |||
double precision, intent(in) | qt, | ||
double precision, intent(in) | qdt, | ||
double precision, dimension(ixi^s,7-2*ndim:3), intent(inout) | fE, | ||
type(state) | sCT, | ||
type(state) | s, | ||
type(ct_velocity) | vcts | ||
) |
update faces
Definition at line 6849 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::b0field_forcefree =.true. |
B0 field is force-free.
Definition at line 230 of file mod_mhd_phys.t.
logical, dimension(2*^nd), public, protected mod_mhd_phys::boundary_divbfix =.true. |
To control divB=0 fix for boundary.
Definition at line 224 of file mod_mhd_phys.t.
integer, dimension(2*^nd), public, protected mod_mhd_phys::boundary_divbfix_skip =0 |
To skip * layer of ghost cells during divB=0 fix for boundary.
Definition at line 227 of file mod_mhd_phys.t.
logical, public mod_mhd_phys::clean_initial_divb = .false. |
clean initial divB
Definition at line 201 of file mod_mhd_phys.t.
logical, public mod_mhd_phys::divbwave = .true. |
Add divB wave in Roe solver.
Definition at line 198 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::e_ |
Index of the energy density (-1 if not present)
Definition at line 131 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::eq_state_units = .true. |
Definition at line 221 of file mod_mhd_phys.t.
integer, public mod_mhd_phys::equi_pe0_ = -1 |
Definition at line 116 of file mod_mhd_phys.t.
integer, public mod_mhd_phys::equi_rho0_ = -1 |
equi vars indices in the stateequi_vars array
Definition at line 115 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::h_ion_fr =1d0 |
Ionization fraction of H H_ion_fr = H+/(H+ + H)
Definition at line 207 of file mod_mhd_phys.t.
logical, public mod_mhd_phys::has_equi_pe0 = .false. |
whether split off equilibrium thermal pressure
Definition at line 111 of file mod_mhd_phys.t.
logical, public mod_mhd_phys::has_equi_rho0 = .false. |
whether split off equilibrium density
Definition at line 109 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::he_abundance =0.1d0 |
Helium abundance over Hydrogen.
Definition at line 204 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::he_ion_fr =1d0 |
Ionization fraction of He He_ion_fr = (He2+ + He+)/(He2+ + He+ + He)
Definition at line 210 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::he_ion_fr2 =1d0 |
Ratio of number He2+ / number He+ + He2+ He_ion_fr2 = He2+/(He2+ + He+)
Definition at line 213 of file mod_mhd_phys.t.
integer, dimension(:), allocatable, public, protected mod_mhd_phys::mag |
Indices of the magnetic field.
Definition at line 137 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_4th_order = .false. |
MHD fourth order.
Definition at line 106 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_adiab = 1.0d0 |
The adiabatic constant.
Definition at line 156 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_ambipolar = .false. |
Whether Ambipolar term is used.
Definition at line 43 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_ambipolar_exp = .false. |
Whether Ambipolar term is implemented explicitly.
Definition at line 49 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_ambipolar_sts = .false. |
Whether Ambipolar term is implemented using supertimestepping.
Definition at line 46 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_boris_simplification = .false. |
Whether boris simplified semirelativistic MHD equations (Gombosi 2002 JCP) are solved.
Definition at line 94 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_cak_force = .false. |
Whether CAK radiation line force is activated.
Definition at line 103 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_divb_4thorder = .false. |
Whether divB is computed with a fourth order approximation.
Definition at line 183 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_dump_full_vars = .false. |
whether dump full variables (when splitting is used) in a separate dat file
Definition at line 119 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_energy = .true. |
Whether an energy equation is used.
Definition at line 16 of file mod_mhd_phys.t.
logical, public mod_mhd_phys::mhd_equi_thermal = .false. |
Definition at line 112 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_eta = 0.0d0 |
The MHD resistivity.
Definition at line 159 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_eta_ambi = 0.0d0 |
The MHD ambipolar coefficient.
Definition at line 168 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_eta_hyper = 0.0d0 |
The MHD hyper-resistivity.
Definition at line 162 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_etah = 0.0d0 |
TODO: what is this?
Definition at line 165 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_gamma = 5.d0/3.0d0 |
The adiabatic index.
Definition at line 153 of file mod_mhd_phys.t.
procedure(sub_get_pthermal), pointer, public mod_mhd_phys::mhd_get_pthermal => null() |
Definition at line 287 of file mod_mhd_phys.t.
procedure(sub_get_pthermal), pointer, public mod_mhd_phys::mhd_get_temperature => null() |
Definition at line 289 of file mod_mhd_phys.t.
procedure(sub_get_v), pointer, public mod_mhd_phys::mhd_get_v => null() |
Definition at line 290 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_glm = .false. |
Whether GLM-MHD is used to control div B.
Definition at line 58 of file mod_mhd_phys.t.
double precision, public mod_mhd_phys::mhd_glm_alpha = 0.5d0 |
GLM-MHD parameter: ratio of the diffusive and advective time scales for div b taking values within [0, 1].
Definition at line 87 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_glm_extended = .true. |
Whether extended GLM-MHD is used with additional sources.
Definition at line 61 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_gravity = .false. |
Whether gravity is added.
Definition at line 34 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_hall = .false. |
Whether Hall-MHD is used.
Definition at line 40 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_hydrodynamic_e = .false. |
Whether hydrodynamic energy is solved instead of total energy.
Definition at line 80 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_internal_e = .false. |
Whether internal energy is solved instead of total energy.
Definition at line 76 of file mod_mhd_phys.t.
procedure(fun_kin_en), pointer, public mod_mhd_phys::mhd_kin_en => null() |
Definition at line 291 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_magnetofriction = .false. |
Whether magnetofriction is added.
Definition at line 55 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::mhd_n_tracer = 0 |
Number of tracer species.
Definition at line 122 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_partial_ionization = .false. |
Whether plasma is partially ionized.
Definition at line 100 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_particles = .false. |
Whether particles module is added.
Definition at line 52 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_radiative_cooling = .false. |
Whether radiative cooling is added.
Definition at line 26 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::mhd_reduced_c = 0.02d0*const_c |
Reduced speed of light for semirelativistic MHD: 2% of light speed.
Definition at line 97 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_rotating_frame = .false. |
Whether rotating frame is activated.
Definition at line 37 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_semirelativistic = .false. |
Whether semirelativistic MHD equations (Gombosi 2002 JCP) are solved.
Definition at line 91 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_thermal_conduction = .false. |
Whether thermal conduction is used.
Definition at line 19 of file mod_mhd_phys.t.
procedure(sub_convert), pointer, public mod_mhd_phys::mhd_to_conserved => null() |
Definition at line 285 of file mod_mhd_phys.t.
procedure(sub_convert), pointer, public mod_mhd_phys::mhd_to_primitive => null() |
Definition at line 284 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_trac = .false. |
Whether TRAC method is used.
Definition at line 64 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::mhd_trac_finegrid =4 |
Distance between two adjacent traced magnetic field lines (in finest cell size)
Definition at line 73 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::mhd_trac_mask = 0.d0 |
Height of the mask used in the TRAC method.
Definition at line 70 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::mhd_trac_type =1 |
Which TRAC method is used.
Definition at line 67 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::mhd_viscosity = .false. |
Whether viscosity is added.
Definition at line 31 of file mod_mhd_phys.t.
integer, dimension(:), allocatable, public, protected mod_mhd_phys::mom |
Indices of the momentum density.
Definition at line 128 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::p_ |
Index of the gas pressure (-1 if not present) should equal e_.
Definition at line 134 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::psi_ |
Indices of the GLM psi.
Definition at line 140 of file mod_mhd_phys.t.
type(rc_fluid), allocatable, public mod_mhd_phys::rc_fl |
type of fluid for radiative cooling
Definition at line 28 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::rho_ |
Index of the density (in the w array)
Definition at line 125 of file mod_mhd_phys.t.
double precision, public, protected mod_mhd_phys::rr =1d0 |
Definition at line 217 of file mod_mhd_phys.t.
logical, public, protected mod_mhd_phys::source_split_divb = .false. |
Whether divB cleaning sources are added splitting from fluid solver.
Definition at line 83 of file mod_mhd_phys.t.
type(tc_fluid), allocatable, public mod_mhd_phys::tc_fl |
type of fluid for thermal conduction
Definition at line 21 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::tcoff_ |
Index of the cutoff temperature for the TRAC method.
Definition at line 146 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::te_ |
Indices of temperature.
Definition at line 143 of file mod_mhd_phys.t.
type(te_fluid), allocatable, public mod_mhd_phys::te_fl_mhd |
type of fluid for thermal emission synthesis
Definition at line 23 of file mod_mhd_phys.t.
integer, dimension(:), allocatable, public, protected mod_mhd_phys::tracer |
Indices of the tracers.
Definition at line 150 of file mod_mhd_phys.t.
integer, public, protected mod_mhd_phys::tweight_ |
Definition at line 147 of file mod_mhd_phys.t.
character(len=std_len), public, protected mod_mhd_phys::type_ct = 'uct_contact' |
Method type of constrained transport.
Definition at line 180 of file mod_mhd_phys.t.
character(len=std_len), public, protected mod_mhd_phys::typedivbfix = 'linde' |
Method type to clean divergence of B.
Definition at line 177 of file mod_mhd_phys.t.
procedure(mask_subroutine), pointer, public mod_mhd_phys::usr_mask_ambipolar => null() |
Definition at line 283 of file mod_mhd_phys.t.