Thermal conduction for HD and MHD Adaptation of mod_thermal_conduction for the mod_supertimestepping In order to use it set use_mhd_tc=1 (for the mhd impl) or 2 (for the hd impl) in mhd_list (for the mhd module both hd and mhd impl can be used) or use_new_hd_tc in hd_list parameters to true (for the hd module, hd implementation has to be used) The TC is set by calling one tc_init_hd_for_total_energy and tc_init_mhd_for_total_energy might The second argument: ixArray has to be [rho_,e_,mag(1)] for mhd (Be aware that the other components of the mag field are assumed consecutive) and [rho_,e_] for hd additionally when internal energy equation is solved, an additional element of this array is eaux_: the index of the internal energy variable. More...
Data Types | |
| interface | get_var_subr |
| type | tc_fluid |
Functions/Subroutines | |
| subroutine | tc_init_params (phys_gamma) |
| subroutine, public | tc_get_mhd_params (fl, read_mhd_params) |
| Init TC coeffiecients: MHD case. More... | |
| subroutine, public | tc_get_hd_params (fl, read_hd_params) |
| Read tc module parameters from par file: MHD case. More... | |
| double precision function, public | get_tc_dt_mhd (w, ixIL, ixOL, dxD, x, fl) |
| Get the explicut timestep for the TC (mhd implementation) More... | |
| subroutine, public | sts_set_source_tc_mhd (ixIL, ixOL, w, x, wres, fix_conserve_at_step, my_dt, igrid, nflux, fl) |
| anisotropic thermal conduction with slope limited symmetric scheme Sharma 2007 Journal of Computational Physics 227, 123 More... | |
| subroutine | set_source_tc_mhd (ixIL, ixOL, w, x, fl, qvec, rho, Te, alpha) |
| double precision function, dimension(ixi^s) | slope_limiter (f, ixIL, ixOL, idims, pm, tc_slope_limiter) |
| subroutine | gradientc (q, ixIL, ixOL, idir, gradq) |
| Calculate gradient of a scalar q at cell interfaces in direction idir. More... | |
| double precision function, public | get_tc_dt_hd (w, ixIL, ixOL, dxD, x, fl) |
| subroutine, public | sts_set_source_tc_hd (ixIL, ixOL, w, x, wres, fix_conserve_at_step, my_dt, igrid, nflux, fl) |
| subroutine | set_source_tc_hd (ixIL, ixOL, w, x, fl, qvec, rho, Te) |
Variables | |
| double precision | tc_gamma_1 |
| The adiabatic index. More... | |
Detailed Description
Thermal conduction for HD and MHD Adaptation of mod_thermal_conduction for the mod_supertimestepping In order to use it set use_mhd_tc=1 (for the mhd impl) or 2 (for the hd impl) in mhd_list (for the mhd module both hd and mhd impl can be used) or use_new_hd_tc in hd_list parameters to true (for the hd module, hd implementation has to be used) The TC is set by calling one tc_init_hd_for_total_energy and tc_init_mhd_for_total_energy might The second argument: ixArray has to be [rho_,e_,mag(1)] for mhd (Be aware that the other components of the mag field are assumed consecutive) and [rho_,e_] for hd additionally when internal energy equation is solved, an additional element of this array is eaux_: the index of the internal energy variable.
10.07.2011 developed by Chun Xia and Rony Keppens 01.09.2012 moved to modules folder by Oliver Porth 13.10.2013 optimized further by Chun Xia 12.03.2014 implemented RKL2 super timestepping scheme to reduce iterations and improve stability and accuracy up to second order in time by Chun Xia. 23.08.2014 implemented saturation and perpendicular TC by Chun Xia 12.01.2017 modulized by Chun Xia
PURPOSE: IN MHD ADD THE HEAT CONDUCTION SOURCE TO THE ENERGY EQUATION S=DIV(KAPPA_i,j . GRAD_j T) where KAPPA_i,j = tc_k_para b_i b_j + tc_k_perp (I - b_i b_j) b_i b_j = B_i B_j / B**2, I is the unit matrix, and i, j= 1, 2, 3 for 3D IN HD ADD THE HEAT CONDUCTION SOURCE TO THE ENERGY EQUATION S=DIV(tc_k_para . GRAD T) USAGE:
- in mod_usr.t -> subroutine usr_init(), add unit_length=your length unit unit_numberdensity=your number density unit unit_velocity=your velocity unit unit_temperature=your temperature unit before call (m)hd_activate()
- to switch on thermal conduction in the (m)hd_list of amrvac.par add: (m)hd_thermal_conduction=.true.
- in the tc_list of amrvac.par : tc_perpendicular=.true. ! (default .false.) turn on thermal conduction perpendicular to magnetic field tc_saturate=.true. ! (default .false. ) turn on thermal conduction saturate effect tc_slope_limiter='MC' ! choose limiter for slope-limited anisotropic thermal conduction in MHD
Function/Subroutine Documentation
◆ get_tc_dt_hd()
| double precision function, public mod_thermal_conduction::get_tc_dt_hd | ( | 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, | ||
| type(tc_fluid), intent(in) | fl | ||
| ) |
Definition at line 689 of file mod_thermal_conduction.t.
◆ get_tc_dt_mhd()
| double precision function, public mod_thermal_conduction::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, | ||
| type(tc_fluid), intent(in) | fl | ||
| ) |
Get the explicut timestep for the TC (mhd implementation)
Definition at line 189 of file mod_thermal_conduction.t.
◆ gradientc()
| subroutine mod_thermal_conduction::gradientc | ( | double precision, dimension(ixi^s), intent(in) | q, |
| integer, intent(in) | ixI, | ||
| integer, intent(in) | L, | ||
| integer, intent(in) | ixO, | ||
| L, | |||
| integer, intent(in) | idir, | ||
| double precision, dimension(ixi^s), intent(inout) | gradq | ||
| ) |
Calculate gradient of a scalar q at cell interfaces in direction idir.
Definition at line 647 of file mod_thermal_conduction.t.
◆ set_source_tc_hd()
| subroutine mod_thermal_conduction::set_source_tc_hd | ( | 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, | ||
| type(tc_fluid), intent(in) | fl, | ||
| double precision, dimension(ixi^s,1:ndim), intent(out) | qvec, | ||
| double precision, dimension(ixi^s), intent(in) | rho, | ||
| double precision, dimension(ixi^s), intent(in) | Te | ||
| ) |
◆ set_source_tc_mhd()
| subroutine mod_thermal_conduction::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(in) | w, | ||
| double precision, dimension(ixi^s,1:ndim), intent(in) | x, | ||
| type(tc_fluid), intent(in) | fl, | ||
| double precision, dimension(ixi^s,1:ndim), intent(out) | qvec, | ||
| double precision, dimension(ixi^s), intent(in) | rho, | ||
| double precision, dimension(ixi^s), intent(in) | Te, | ||
| double precision, intent(in) | alpha | ||
| ) |
◆ slope_limiter()
| double precision function, dimension(ixi^s) mod_thermal_conduction::slope_limiter | ( | double precision, dimension(ixi^s), intent(in) | f, |
| integer, intent(in) | ixI, | ||
| integer, intent(in) | L, | ||
| integer, intent(in) | ixO, | ||
| L, | |||
| integer, intent(in) | idims, | ||
| integer, intent(in) | pm, | ||
| integer, intent(in) | tc_slope_limiter | ||
| ) |
Definition at line 609 of file mod_thermal_conduction.t.
◆ sts_set_source_tc_hd()
| subroutine, public mod_thermal_conduction::sts_set_source_tc_hd | ( | 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: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, | ||
| type(tc_fluid), intent(in) | fl | ||
| ) |
◆ sts_set_source_tc_mhd()
| subroutine, public mod_thermal_conduction::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(in) | 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, | ||
| type(tc_fluid), intent(in) | fl | ||
| ) |
anisotropic thermal conduction with slope limited symmetric scheme Sharma 2007 Journal of Computational Physics 227, 123
Definition at line 277 of file mod_thermal_conduction.t.
◆ tc_get_hd_params()
| subroutine, public mod_thermal_conduction::tc_get_hd_params | ( | type(tc_fluid), intent(inout) | fl, |
| read_hd_params | |||
| ) |
Read tc module parameters from par file: MHD case.
Read tc parameters from par file: HD case
Definition at line 160 of file mod_thermal_conduction.t.
◆ tc_get_mhd_params()
| subroutine, public mod_thermal_conduction::tc_get_mhd_params | ( | type(tc_fluid), intent(inout) | fl, |
| read_mhd_params | |||
| ) |
Init TC coeffiecients: MHD case.
Definition at line 114 of file mod_thermal_conduction.t.
◆ tc_init_params()
| subroutine mod_thermal_conduction::tc_init_params | ( | double precision, intent(in) | phys_gamma | ) |
Definition at line 106 of file mod_thermal_conduction.t.
Variable Documentation
◆ tc_gamma_1
| double precision mod_thermal_conduction::tc_gamma_1 |
The adiabatic index.
Definition at line 47 of file mod_thermal_conduction.t.
