#include <hmi.h>
hmi.h - parameters dealing with hydrogen molecules
Definition at line 13 of file hmi.h.
method used for grain formation pumping
Definition at line 171 of file hmi.h.
Referenced by diatomics::init(), ParseSet(), and zero().
the set h2 small model command tells code says which of the small model H2 to use. Default is Elwert
Definition at line 168 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), mole_h_reactions(), ParseSet(), and zero().
char t_hmi::chJura |
the set h2 jura command tells code which treatment of H2 formation to use
Definition at line 174 of file hmi.h.
Referenced by mole_h2_grain_form(), ParseSet(), and zero().
the largest fraction of total cooling anywhere in model
Definition at line 46 of file hmi.h.
Referenced by IterStart(), lines_molecules(), PrtComment(), and zero().
Definition at line 145 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
Definition at line 145 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
Definition at line 145 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
Definition at line 145 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), mole_h_fixup(), and zero().
these are derivative wrt temp for collisional processes within X
Definition at line 145 of file hmi.h.
Referenced by CoolEvaluate(), HeatSum(), IterRestart(), IterStart(), and zero().
double t_hmi::exphmi |
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
Definition at line 153 of file hmi.h.
Referenced by diatomics::mole_H2_form(), and mole_h_rate_diagnostics().
double t_hmi::H2_forms_hminus |
Definition at line 153 of file hmi.h.
Referenced by frac_H2star_hminus(), diatomics::mole_H2_form(), and mole_h_rate_diagnostics().
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
Definition at line 185 of file hmi.h.
Referenced by diatomics::H2_LevelPops(), mole_h_fixup(), mole_solve(), ParseSet(), and zero().
the Solomon process excitation, H2g -> H2*, rate for the Bertodi & Draine model
Definition at line 83 of file hmi.h.
Referenced by mole_h_reactions().
the Solomon process excitation, H2g -> H2*, rate from Burton et al. 1990
Definition at line 80 of file hmi.h.
Referenced by mole_h_reactions().
the Solomon process excitation, H2g -> H2*, rate for Elwert et al. model in prep.
Definition at line 86 of file hmi.h.
Referenced by mole_h_reactions().
the Solomon process excitation, H2g -> H2*, rate from Tielens & Hollenbach 85
Definition at line 77 of file hmi.h.
Referenced by mole_h_reactions().
the Solomon process excitation, H2g -> H2*, - actually used
Definition at line 89 of file hmi.h.
Referenced by IterRestart(), IterStart(), and mole_h_reactions().
double t_hmi::H2_photodissoc_BHT90 |
Definition at line 113 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
Definition at line 110 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
Definition at line 111 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
double t_hmi::H2_photodissoc_TH85 |
Definition at line 112 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
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
Definition at line 108 of file hmi.h.
Referenced by IterRestart(), IterStart(), mole_h_reactions(), SaveDo(), and zero().
Definition at line 109 of file hmi.h.
Referenced by IterRestart(), IterStart(), mole_h_reactions(), and zero().
double t_hmi::H2_rate_destroy |
rate ground of H2 is destroyed
Definition at line 21 of file hmi.h.
Referenced by diatomics::H2_LevelPops(), diatomics::H2_PunchDo(), mole_effects(), and mole_h_rate_diagnostics().
Definition at line 95 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), IonHydro(), mole_h_reactions(), and zero().
Definition at line 101 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), mole_h_reactions(), and zero().
Definition at line 94 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
Definition at line 100 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
Definition at line 96 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), mole_h_reactions(), and zero().
Definition at line 102 of file hmi.h.
Referenced by mole_h_reactions(), and zero().
Definition at line 93 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), IonHydro(), mole_h_reactions(), and zero().
Definition at line 99 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), mole_h_reactions(), and zero().
the Solomon process dissociate rate from Tielens & Hollenbach 85
Definition at line 92 of file hmi.h.
Referenced by IonHydro(), IterRestart(), IterStart(), mole_effects(), mole_h_rate_diagnostics(), mole_h_reactions(), SaveDo(), and zero().
Definition at line 98 of file hmi.h.
Referenced by IterRestart(), IterStart(), mole_effects(), mole_h_reactions(), and zero().
double t_hmi::H2_total |
the total H2 density [cm-3], NOT 2*n(H2), the sum of H2 and H2*
Definition at line 16 of file hmi.h.
Referenced by ConvBase(), ConvTempEdenIoniz(), CoolCarb(), CoolEvaluate(), CoolOxyg(), GrainCollHeating(), GrainMakeDiffuse(), GrnStdDpth(), diatomics::H2_X_sink_and_source(), HeatSum(), ColliderList::init(), IonHydro(), iter_end_check(), IterRestart(), t_mean::MeanInc(), mole_effects(), mole_h_fixup(), mole_h_rate_diagnostics(), oi_othercs(), OpacityAddTotal(), PrtZone(), radius_first(), radius_increment(), radius_next(), SaveDo(), ScaleAllDensities(), and zero().
Definition at line 17 of file hmi.h.
Referenced by diatomics::H2_X_coll_rate_evaluate(), IterRestart(), mole_effects(), mole_h_fixup(), and zero().
double t_hmi::h2dep |
Definition at line 33 of file hmi.h.
Referenced by mole_effects(), mole_h_rate_diagnostics(), PrtZone(), and zero().
Definition at line 46 of file hmi.h.
Referenced by IterStart(), lines_molecules(), and PrtComment().
Definition at line 46 of file hmi.h.
Referenced by IterStart(), lines_molecules(), and PrtComment().
fraqction of cooling carried by H2 lines
Definition at line 46 of file hmi.h.
Referenced by IterStart(), lines_molecules(), and PrtComment().
mean cross section (cm-2) for H2 Lyman absorption
Definition at line 29 of file hmi.h.
Referenced by mole_h_fixup(), mole_h_reactions(), radius_first(), and zero().
double t_hmi::h2pdep |
Definition at line 33 of file hmi.h.
Referenced by mole_effects(), mole_h_rate_diagnostics(), PrtZone(), and zero().
double t_hmi::h2plus_heat |
heating due to photo dissoc of H2+
Definition at line 39 of file hmi.h.
Referenced by CoolEvaluate(), IterRestart(), IterStart(), lines_molecules(), mole_effects(), mole_h_fixup(), and zero().
largest local fraction heating due to dissoc of H2+
Definition at line 120 of file hmi.h.
Referenced by IterStart(), lines_molecules(), and PrtComment().
double t_hmi::H2star_forms_grains |
Definition at line 153 of file hmi.h.
Referenced by diatomics::mole_H2_form(), and mole_h_rate_diagnostics().
double t_hmi::H2star_forms_hminus |
Definition at line 153 of file hmi.h.
Referenced by frac_H2star_hminus(), diatomics::mole_H2_form(), and mole_h_rate_diagnostics().
double t_hmi::h3pdep |
Definition at line 33 of file hmi.h.
Referenced by mole_effects(), PrtZone(), and zero().
double t_hmi::HD_total |
Definition at line 18 of file hmi.h.
Referenced by IterRestart(), mole_effects(), and zero().
double t_hmi::HeatH2Dexc_BD96 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dexc_BHT90 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dexc_ELWERT |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dexc_TH85 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), diatomics::H2_PunchDo(), mole_effects(), mole_h_fixup(), and zero().
double t_hmi::HeatH2Dexc_used |
HeatH2Dexc_used is heating due to collisional deexcitation of vib-excited H2 actually used
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), CoolSave(), HeatSum(), IterRestart(), IterStart(), lines_molecules(), radius_next(), SaveDo(), and zero().
the largest fraction of total heat anywhere in model
Definition at line 46 of file hmi.h.
Referenced by IterStart(), lines_molecules(), PrtComment(), and zero().
double t_hmi::HeatH2Dish_BD96 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dish_BHT90 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dish_ELWERT |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), mole_effects(), and zero().
double t_hmi::HeatH2Dish_TH85 |
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), diatomics::H2_PunchDo(), mole_effects(), mole_h_fixup(), and zero().
double t_hmi::HeatH2Dish_used |
HeatH2Dish_used is heating due to H2 dissociation actually used
Definition at line 129 of file hmi.h.
Referenced by CoolEvaluate(), IterRestart(), IterStart(), lines_molecules(), radius_next(), SaveDo(), and zero().
double t_hmi::hmicol |
Definition at line 24 of file hmi.h.
Referenced by CoolEvaluate(), CoolSave(), lines_molecules(), mole_h_fixup(), mole_h_rate_diagnostics(), and mole_h_reactions().
double t_hmi::hmidep |
these are departure coef for H-, H2, H2+, and HeH, defined in hmole
Definition at line 33 of file hmi.h.
Referenced by lgCheckMonitors(), mole_effects(), mole_h_fixup(), mole_h_rate_diagnostics(), OpacityAddTotal(), PrtZone(), RT_tau_inc(), and zero().
double t_hmi::hmihet |
hminus heating, free bound
Definition at line 24 of file hmi.h.
Referenced by CoolEvaluate(), IterRestart(), IterStart(), lines_molecules(), mole_effects(), mole_h_fixup(), mole_h_rate_diagnostics(), and zero().
Definition at line 54 of file hmi.h.
Referenced by mole_effects(), mole_h_rate_diagnostics(), and mole_h_reactions().
double t_hmi::HMinus_induc_rec_rate |
Definition at line 54 of file hmi.h.
Referenced by mole_h_rate_diagnostics(), and mole_h_reactions().
double t_hmi::HMinus_photo_heat |
Definition at line 54 of file hmi.h.
Referenced by mole_effects(), and mole_h_reactions().
double t_hmi::HMinus_photo_rate |
H- photo dissoc rate
Definition at line 42 of file hmi.h.
Referenced by CoolEvaluate(), mole_h_rate_diagnostics(), mole_h_reactions(), and RT_OTS().
double t_hmi::hmitot |
Definition at line 24 of file hmi.h.
Referenced by IterRestart(), IterStart(), lines_molecules(), PrtComment(), and zero().
long int t_hmi::iheh1 |
Definition at line 58 of file hmi.h.
Referenced by ContCreatePointers().
long int t_hmi::iheh2 |
Definition at line 58 of file hmi.h.
Referenced by ContCreatePointers().
long int t_hmi::iphmin |
continuum array index for H minus threshold
Definition at line 117 of file hmi.h.
Referenced by ContCreatePointers(), mole_h_reactions(), OpacityAddTotal(), OpacityCreateAll(), RT_diffuse(), and RT_tau_inc().
say how to do chemistry (formation and destruction), if true (default) use results of large molecule, if false use TH85 approximations
Definition at line 160 of file hmi.h.
Referenced by frac_H2star_hminus(), mole_h_reactions(), ParseAtomH2(), and zero().
say how to do thermal solution, if true (default) use results of large molecule, if false use TH85 approximations
Definition at line 160 of file hmi.h.
Referenced by CoolEvaluate(), ParseAtomH2(), and zero().
hack to kill effects of H2* in chemistry network set leiden hack h2* off
Definition at line 208 of file hmi.h.
Referenced by diatomics::H2_Calc_Average_Rates(), diatomics::H2_LevelPops(), diatomics::H2_Solomon_rate(), diatomics::H2_X_sink_and_source(), diatomics::init(), t_mole_global::make_species(), diatomics::Mol_Photo_Diss_Rates(), diatomics::mole_H2_form(), ParseSet(), and zero().
Definition at line 209 of file hmi.h.
Referenced by mole_h_reactions(), ParseSet(), diatomics::SolveExcitedElectronicLevels(), diatomics::SolveSomeGroundElectronicLevels(), and zero().
H2 formation rate as set with set h2 rate command units S^-1, actual depl
Definition at line 181 of file hmi.h.
Referenced by mole_h2_grain_form(), and ParseSet().
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
Definition at line 200 of file hmi.h.
Referenced by mole_effects(), mole_h_rate_diagnostics(), and mole_h_reactions().
double t_hmi::rel_pop_LTE_H2p |
LTE population for H2+, following is n(H2+) / [n(H) n(p) ], units cm3
Definition at line 200 of file hmi.h.
Referenced by mole_effects(), and mole_h_reactions().
double t_hmi::rel_pop_LTE_H2s |
related to the LTE population of H2s, following is n(H2s) / [n(H) n(H) ], units cm3
Definition at line 188 of file hmi.h.
Referenced by mole_h_rate_diagnostics(), and mole_h_reactions().
double t_hmi::rel_pop_LTE_H3p |
related to population of H3+
Definition at line 200 of file hmi.h.
Referenced by mole_effects(), and mole_h_reactions().
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
Definition at line 188 of file hmi.h.
Referenced by mole_effects(), mole_h_rate_diagnostics(), and mole_h_reactions().
this is a scale factor to multiply the Jura rate, default is unity, changed with the set jura scale command
Definition at line 178 of file hmi.h.
Referenced by mole_h2_grain_form(), ParseSet(), and zero().
binding energy for change in H2 population while on grain surface, set with "set h2 Tad " command
Definition at line 124 of file hmi.h.
Referenced by mole_h2_grain_form(), ParseSet(), and zero().
Definition at line 73 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), IterRestart(), IterStart(), mole_h_reactions(), SaveDo(), and zero().
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
Definition at line 73 of file hmi.h.
Referenced by IterRestart(), IterStart(), mole_effects(), mole_h_reactions(), PrtFinal(), and zero().
the special version of g0 with adjustable bounds
Definition at line 63 of file hmi.h.
Referenced by diatomics::H2_PunchDo(), and mole_h_reactions().
Definition at line 63 of file hmi.h.
Referenced by GrainDrive(), GrainTemperature(), diatomics::H2_PunchDo(), mole_h_reactions(), SaveDo(), and zero().
UV flux relative to Habing value, used for some simple molecular photodissociation rates, as defined by Tielens & Hollenbach 1985
Definition at line 63 of file hmi.h.
Referenced by ion_photo(), IterRestart(), IterStart(), mole_h_reactions(), PrtFinal(), and zero().