#include <hmi.h>
Public Member Functions | |
| const char * | chName () const |
| void | zero () |
| void | comment (t_warnings &) |
 Public Member Functions inherited from module | |
| module () | |
| virtual | ~module () |
Detailed Description
hmi.h - parameters dealing with hydrogen molecules
Member Function Documentation
◆ chName()
|
inlinevirtual |
Implements module.
◆ comment()
|
inlinevirtual |
Implements module.
◆ zero()
|
virtual |
HeatH2Dexc_used is heating due to collisional deexcitation of vib-excited H2 actually used
these are derivative wrt temp for collisional processes within X
the Solomon process rate H2 dissociates into X continuum - actually used
set_NaN( H2_Solomon_dissoc_rate_used );
H2 + hnu => 2H from TH85
H2 + hnu => 2H actually used
Implements module.
References chGrainFormPump, chH2_small_model_type, chJura, CoolH2DexcMax, DEBUG_ENTRY, deriv_HeatH2Dexc_BD96, deriv_HeatH2Dexc_BHT90, deriv_HeatH2Dexc_ELWERT, deriv_HeatH2Dexc_TH85, deriv_HeatH2Dexc_used, H2_frac_abund_set, H2_photodissoc_BHT90, H2_photodissoc_ELWERT_H2g, H2_photodissoc_ELWERT_H2s, H2_photodissoc_TH85, H2_photodissoc_used_H2g, H2_photodissoc_used_H2s, H2_Solomon_dissoc_rate_BD96_H2g, H2_Solomon_dissoc_rate_BD96_H2s, H2_Solomon_dissoc_rate_BHT90_H2g, H2_Solomon_dissoc_rate_BHT90_H2s, H2_Solomon_dissoc_rate_ELWERT_H2g, H2_Solomon_dissoc_rate_ELWERT_H2s, H2_Solomon_dissoc_rate_TH85_H2g, H2_Solomon_dissoc_rate_TH85_H2s, H2_Solomon_dissoc_rate_used_H2g, H2_Solomon_dissoc_rate_used_H2s, H2_total, H2_total_f, h2dep, H2Opacity, h2pdep, h2plus_exc_frac, h2plus_heat, h2plus_heatcoef, h3pdep, HD_total, HeatH2Dexc_BD96, HeatH2Dexc_BHT90, HeatH2Dexc_ELWERT, HeatH2Dexc_TH85, HeatH2Dexc_used, HeatH2DexcMax, HeatH2Dish_BD96, HeatH2Dish_BHT90, HeatH2Dish_ELWERT, HeatH2Dish_TH85, HeatH2Dish_used, hmidep, hmihet, hmitot, lgH2_Chemistry_BigH2, lgH2_Thermal_BigH2, lgLeiden_Keep_ipMH2s, lgLeidenCRHack, ScaleJura, set_NaN(), Tad, UV_Cont_rel2_Draine_DB96_depth, UV_Cont_rel2_Draine_DB96_face, UV_Cont_rel2_Habing_TH85_depth, and UV_Cont_rel2_Habing_TH85_face.
Member Data Documentation
◆ chGrainFormPump
| char t_hmi::chGrainFormPump |
method used for grain formation pumping
Referenced by zero().
◆ chH2_small_model_type
| char t_hmi::chH2_small_model_type |
the set h2 small model command tells code says which of the small model H2 to use. Default is Elwert
Referenced by zero().
◆ chJura
| char t_hmi::chJura |
the set h2 jura command tells code which treatment of H2 formation to use
Referenced by zero().
◆ CoolH2DexcMax
| realnum t_hmi::CoolH2DexcMax |
the largest fraction of total cooling anywhere in model
Referenced by zero().
◆ deriv_HeatH2Dexc_BD96
◆ deriv_HeatH2Dexc_BHT90
◆ deriv_HeatH2Dexc_ELWERT
◆ deriv_HeatH2Dexc_TH85
◆ deriv_HeatH2Dexc_used
| realnum t_hmi::deriv_HeatH2Dexc_used |
these are derivative wrt temp for collisional processes within X
Referenced by zero().
◆ exphmi
| double t_hmi::exphmi |
Boltzmann factor for hmi
◆ H2_forms_grains
| double t_hmi::H2_forms_grains |
these are the H- and grain formation rates, added above and below a certain energy (2.6 eV) for production of H2 or H2* in small network
◆ H2_forms_hminus
| double t_hmi::H2_forms_hminus |
◆ H2_frac_abund_set
| double t_hmi::H2_frac_abund_set |
this is set to zero, but to positive number with atom h2 fraction command this sets the H2 density by multiplying the hydrogen density to become the H2 density
Referenced by zero().
◆ H2_H2g_to_H2s_rate_BD96
| double t_hmi::H2_H2g_to_H2s_rate_BD96 |
the Solomon process excitation, H2g -> H2*, rate for the Bertodi & Draine model
◆ H2_H2g_to_H2s_rate_BHT90
| double t_hmi::H2_H2g_to_H2s_rate_BHT90 |
the Solomon process excitation, H2g -> H2*, rate from Burton et al. 1990
◆ H2_H2g_to_H2s_rate_ELWERT
| double t_hmi::H2_H2g_to_H2s_rate_ELWERT |
the Solomon process excitation, H2g -> H2*, rate for Elwert et al. model in prep.
◆ H2_H2g_to_H2s_rate_TH85
| double t_hmi::H2_H2g_to_H2s_rate_TH85 |
the Solomon process excitation, H2g -> H2*, rate from Tielens & Hollenbach 85
◆ H2_H2g_to_H2s_rate_used
| double t_hmi::H2_H2g_to_H2s_rate_used |
the Solomon process excitation, H2g -> H2*, - actually used
◆ H2_photodissoc_BHT90
| double t_hmi::H2_photodissoc_BHT90 |
Referenced by zero().
◆ H2_photodissoc_ELWERT_H2g
| double t_hmi::H2_photodissoc_ELWERT_H2g |
Referenced by zero().
◆ H2_photodissoc_ELWERT_H2s
| double t_hmi::H2_photodissoc_ELWERT_H2s |
Referenced by zero().
◆ H2_photodissoc_TH85
| double t_hmi::H2_photodissoc_TH85 |
Referenced by zero().
◆ H2_photodissoc_used_H2g
| double t_hmi::H2_photodissoc_used_H2g |
the Solomon process rate H2 dissociates into X continuum - actually used double H2_Solomon_dissoc_rate_used; H2 + hnu => 2H from TH85 H2 + hnu => 2H actually used
Referenced by zero().
◆ H2_photodissoc_used_H2s
| double t_hmi::H2_photodissoc_used_H2s |
Referenced by zero().
◆ H2_rate_destroy
| double t_hmi::H2_rate_destroy |
rate ground of H2 is destroyed
◆ H2_Solomon_dissoc_rate_BD96_H2g
| double t_hmi::H2_Solomon_dissoc_rate_BD96_H2g |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_BD96_H2s
| double t_hmi::H2_Solomon_dissoc_rate_BD96_H2s |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_BHT90_H2g
| double t_hmi::H2_Solomon_dissoc_rate_BHT90_H2g |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_BHT90_H2s
| double t_hmi::H2_Solomon_dissoc_rate_BHT90_H2s |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_ELWERT_H2g
| double t_hmi::H2_Solomon_dissoc_rate_ELWERT_H2g |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_ELWERT_H2s
| double t_hmi::H2_Solomon_dissoc_rate_ELWERT_H2s |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_TH85_H2g
| double t_hmi::H2_Solomon_dissoc_rate_TH85_H2g |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_TH85_H2s
| double t_hmi::H2_Solomon_dissoc_rate_TH85_H2s |
Referenced by zero().
◆ H2_Solomon_dissoc_rate_used_H2g
| double t_hmi::H2_Solomon_dissoc_rate_used_H2g |
the Solomon process dissociate rate from Tielens & Hollenbach 85
Referenced by zero().
◆ H2_Solomon_dissoc_rate_used_H2s
| double t_hmi::H2_Solomon_dissoc_rate_used_H2s |
Referenced by zero().
◆ H2_total
| double t_hmi::H2_total |
the total H2 density [cm-3], NOT 2*n(H2), the sum of H2 and H2*
Referenced by zero().
◆ H2_total_f
◆ h2dep
| double t_hmi::h2dep |
Referenced by zero().
◆ h2dfrc
| realnum t_hmi::h2dfrc |
◆ h2dtot
| realnum t_hmi::h2dtot |
◆ h2line_cool_frac
| realnum t_hmi::h2line_cool_frac |
fraqction of cooling carried by H2 lines
◆ H2Opacity
◆ h2pdep
| double t_hmi::h2pdep |
Referenced by zero().
◆ h2plus_exc_frac
| double t_hmi::h2plus_exc_frac |
fraction of H2+ in excited states
Referenced by zero().
◆ h2plus_heat
| double t_hmi::h2plus_heat |
Referenced by zero().
◆ h2plus_heatcoef
| double t_hmi::h2plus_heatcoef |
heating due to photo dissoc of H2+
Referenced by zero().
◆ h2pmax
| realnum t_hmi::h2pmax |
largest local fraction heating due to dissoc of H2+
◆ H2star_forms_grains
| double t_hmi::H2star_forms_grains |
◆ H2star_forms_hminus
| double t_hmi::H2star_forms_hminus |
◆ h3pdep
| double t_hmi::h3pdep |
Referenced by zero().
◆ HD_total
| double t_hmi::HD_total |
Referenced by zero().
◆ HeatH2Dexc_BD96
| double t_hmi::HeatH2Dexc_BD96 |
Referenced by zero().
◆ HeatH2Dexc_BHT90
| double t_hmi::HeatH2Dexc_BHT90 |
Referenced by zero().
◆ HeatH2Dexc_ELWERT
| double t_hmi::HeatH2Dexc_ELWERT |
Referenced by zero().
◆ HeatH2Dexc_TH85
| double t_hmi::HeatH2Dexc_TH85 |
Referenced by zero().
◆ HeatH2Dexc_used
| double t_hmi::HeatH2Dexc_used |
HeatH2Dexc_used is heating due to collisional deexcitation of vib-excited H2 actually used
Referenced by zero().
◆ HeatH2DexcMax
| realnum t_hmi::HeatH2DexcMax |
the largest fraction of total heat anywhere in model
Referenced by zero().
◆ HeatH2Dish_BD96
| double t_hmi::HeatH2Dish_BD96 |
Referenced by zero().
◆ HeatH2Dish_BHT90
| double t_hmi::HeatH2Dish_BHT90 |
Referenced by zero().
◆ HeatH2Dish_ELWERT
| double t_hmi::HeatH2Dish_ELWERT |
Referenced by zero().
◆ HeatH2Dish_TH85
| double t_hmi::HeatH2Dish_TH85 |
Referenced by zero().
◆ HeatH2Dish_used
| double t_hmi::HeatH2Dish_used |
HeatH2Dish_used is heating due to H2 dissociation actually used
Referenced by zero().
◆ hmicol
| double t_hmi::hmicol |
◆ hmidep
| double t_hmi::hmidep |
these are departure coef for H-, H2, H2+, and HeH, defined in hmole
Referenced by zero().
◆ hmihet
| double t_hmi::hmihet |
hminus heating, free bound
Referenced by zero().
◆ HMinus_induc_rec_cooling
| double t_hmi::HMinus_induc_rec_cooling |
◆ HMinus_induc_rec_rate
| double t_hmi::HMinus_induc_rec_rate |
◆ HMinus_photo_heat
| double t_hmi::HMinus_photo_heat |
◆ HMinus_photo_rate
| double t_hmi::HMinus_photo_rate |
H- photo dissoc rate
◆ hmitot
| double t_hmi::hmitot |
Referenced by zero().
◆ iheh1
| long int t_hmi::iheh1 |
◆ iheh2
| long int t_hmi::iheh2 |
◆ iphmin
| long int t_hmi::iphmin |
continuum array index for H minus threshold
◆ lgH2_Chemistry_BigH2
| bool t_hmi::lgH2_Chemistry_BigH2 |
say how to do chemistry (formation and destruction), if true (default) use results of large molecule, if false use TH85 approximations
Referenced by zero().
◆ lgH2_Thermal_BigH2
| bool t_hmi::lgH2_Thermal_BigH2 |
say how to do thermal solution, if true (default) use results of large molecule, if false use TH85 approximations
Referenced by zero().
◆ lgLeiden_Keep_ipMH2s
| bool t_hmi::lgLeiden_Keep_ipMH2s |
hack to kill effects of H2* in chemistry network "set leiden hack h2* off
Referenced by zero().
◆ lgLeidenCRHack
| bool t_hmi::lgLeidenCRHack |
Referenced by zero().
◆ rate_h2_form_grains_set
| double t_hmi::rate_h2_form_grains_set |
H2 formation rate as set with set h2 rate command units S^-1, actual depl
◆ rel_pop_LTE_H2g
| double t_hmi::rel_pop_LTE_H2g |
related to the LTE population of H2 in ground, following is
n(H2) / [n(H) n(H) ], units cm3
◆ rel_pop_LTE_H2p
| double t_hmi::rel_pop_LTE_H2p |
LTE population for H2+, following is n(H2+) / [n(H) n(p) ], units cm3
◆ rel_pop_LTE_H2s
| double t_hmi::rel_pop_LTE_H2s |
related to the LTE population of H2s, following is
n(H2s) / [n(H) n(H) ], units cm3
◆ rel_pop_LTE_H3p
| double t_hmi::rel_pop_LTE_H3p |
related to population of H3+
◆ rel_pop_LTE_Hmin
| double t_hmi::rel_pop_LTE_Hmin |
related to the LTE populations of H-, H2, and H2+ each is a constant with temperature dependence, and needs to be multiplied by the densities of the separated components to become the LTE density.
following is n(H-) / [ n(e) n(H) ], units cm3
◆ ScaleJura
| realnum t_hmi::ScaleJura |
this is a scale factor to multiply the Jura rate, default is unity, changed with the set jura scale command
Referenced by zero().
◆ Tad
| realnum t_hmi::Tad |
binding energy for change in H2 population while on grain surface, set with "set h2 Tad " command
Referenced by zero().
◆ UV_Cont_rel2_Draine_DB96_depth
◆ UV_Cont_rel2_Draine_DB96_face
| realnum t_hmi::UV_Cont_rel2_Draine_DB96_face |
UV flux relative to Habing value, used for some simple molecular photodissociation rates, as defined by Draine & Bertoldi 1996 -0 we try to do this the way they describe, since they say that this will agree with their large H2 molecule, first define field at the illuminated face, then get value at depth using their form of the extinction and shielding, rather than our exact calculation
Referenced by zero().
◆ UV_Cont_rel2_Habing_spec_depth
| realnum t_hmi::UV_Cont_rel2_Habing_spec_depth |
the special version of g0 with adjustable bounds
◆ UV_Cont_rel2_Habing_TH85_depth
◆ UV_Cont_rel2_Habing_TH85_face
| realnum t_hmi::UV_Cont_rel2_Habing_TH85_face |
UV flux relative to Habing value, used for some simple molecular photodissociation rates, as defined by Tielens & Hollenbach 1985
Referenced by zero().
The documentation for this struct was generated from the following files:
