#include "cddefines.h"#include "physconst.h"#include "iterations.h"#include "hydrogenic.h"#include "oxy.h"#include "doppvel.h"#include "dense.h"#include "hextra.h"#include "grains.h"#include "magnetic.h"#include "state.h"#include "rt.h"#include "he.h"#include "struc.h"#include "h2.h"#include "coolheavy.h"#include "lines.h"#include "dynamics.h"#include "carb.h"#include "mean.h"#include "atomfeii.h"#include "iso.h"#include "conv.h"#include "geometry.h"#include "timesc.h"#include "peimbt.h"#include "ionbal.h"#include "continuum.h"#include "atmdat.h"#include "mole.h"#include "ca.h"#include "input.h"#include "atoms.h"#include "pressure.h"#include "numderiv.h"#include "colden.h"#include "yield.h"#include "hmi.h"#include "rfield.h"#include "abund.h"#include "radius.h"#include "opacity.h"#include "broke.h"#include "secondaries.h"#include "called.h"#include "phycon.h"#include "warnings.h"#include "thermal.h"#include "cooling.h"#include "fe.h"#include "hyperfine.h"#include "init.h"Include dependency graph for zero.cpp:
Go to the source code of this file.
Functions | |
| void | zero (void) |
| void | rfield_opac_zero (long lo, long ihi) |
| void rfield_opac_zero | ( | long | lo, | |
| long | ihi | |||
| ) |
zero out rfield arrays between certain limits, code in zero.c
Definition at line 1548 of file zero.cpp.
References t_opac::albedo, t_rfield::ConEmitOut, t_rfield::ConEmitReflec, t_rfield::ConInterOut, t_rfield::ConOTS_local_OTS_rate, t_rfield::ConOTS_local_photons, t_rfield::ConRefIncid, t_rfield::ContBoltz, t_rfield::convoc, t_opac::E2TauAbsFace, t_opac::E2TauAbsOut, t_opac::E2TauAbsTotal, t_opac::ExpmTau, t_opac::ExpZone, t_rfield::fine_opac_zone, t_rfield::fine_opt_depth, t_rfield::flux, t_rfield::flux_accum, t_rfield::flux_beam_const_save, t_rfield::flux_isotropic_save, t_rfield::flux_time_beam_save, t_opac::FreeFreeOpacity, lgRfieldMalloced, t_rfield::nfine_malloc, t_rfield::OccNumbBremsCont, t_rfield::OccNumbContEmitOut, t_rfield::OccNumbDiffCont, t_opac::OldOpacSave, opac, t_opac::opacity_abs, t_opac::opacity_sct, t_opac::OpacStatic, t_rfield::otscon, t_rfield::otsconNew, t_rfield::otslin, t_rfield::otslinNew, t_rfield::outlin, t_rfield::outlin_noplot, t_rfield::reflin, rfield, t_rfield::SummedCon, t_rfield::SummedDif, t_rfield::SummedOcc, t_opac::TauAbsGeo, t_opac::TauAbsTotal, t_opac::taumin, t_opac::TauScatGeo, t_opac::TauTotalGeo, and t_opac::tmn.
| void zero | ( | void | ) |
zero actively zero out or initialize variables needed for model calculation this is the old one and should be removed - its vars moved into those above
option to set proton elimination rates to zero >>refer CO chemistry Huntress, W. T., 1977, ApJS, 33, 495 By default, this is false - changed with set chemistry command
option to not include neutrals in the non-equilibrium scheme >> refer Federman, S. R. & Zsargo, J. 2003, ApJ, 589, 319 By default, this is false - changed with set chemistry command
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( hmi.H2_Solomon_dissoc_rate_used );
H2 + hnu => 2H from TH85
H2 + hnu => 2H actually used
Definition at line 61 of file zero.cpp.
References AbundancesZero(), t_geometry::AngleIllumRadian, t_conv::autocv, t_conv::AverEdenError, t_conv::AverHeatCoolError, t_conv::AverPressError, t_timesc::BigCOMoleForm, t_conv::BigEdenError, t_conv::BigHeatCoolError, t_conv::BigPressError, t_CoolHeavy::brems_cool_h, t_CoolHeavy::brems_cool_net, carb, t_LineSave::chNormLab, t_conv::chSolverEden, t_conv::chSolverTemp, t_iso::chTypeAtomSet, t_iso::chTypeAtomUsed, t_hydro::cintot, t_timesc::CloudAgeSet, co, t_co::COCoolBigFrac, t_co::codfrc, t_co::CODissHeat, t_co::codtot, t_CoolHeavy::colmet, continuum, conv, CoolHeavy, t_geometry::covgeo, t_geometry::covrt, DEBUG_ENTRY, t_geometry::DirectionalCosin, t_conv::EdenErrorAllowed, t_continuum::EnergyKshell, FeIIZero(), t_geometry::FillFac, t_geometry::filpow, t_geometry::fiscal, geometry, H2_Init(), t_hydro::HCollIonMax, t_conv::HeatCoolRelErrorAllowed, hmole_init(), hydro, hyperfine, t_geometry::iEmissPower, Singleton< T >::Inst(), ionbal, ipH_LIKE, ipHYDROGEN, t_LineSave::ipNormWavL, iso, t_iterations::iter_malloc, iteration, iterations, t_iterations::itermx, t_iterations::IterPrnt, lgAbort, t_conv::lgAutoIt, t_co::lgCOCoolCaped, t_continuum::lgCon0, t_conv::lgConvEden, t_iterations::lgConverge_set, t_conv::lgConvPres, t_conv::lgConvTemp, t_continuum::lgCoStarInterpolationCaution, t_geometry::lgEndDflt, lgFirstCall, t_CoolHeavy::lgFreeOn, t_state::lgGet_state, t_hydro::lgHiPop2, t_conv::lgLevel2_Cool_Imp, t_conv::lgLevel2_OTS_Imp, t_LineSave::lgLineEmergent, t_hyperfine::lgLya_pump_21cm, t_conv::lgMap, t_co::lgNoCOMole, t_LineSave::lgNormSet, t_NumDeriv::lgNumDeriv, t_state::lgPut_state, t_hydro::lgReevalRecom, t_geometry::lgSphere, t_state::lgState_print, t_geometry::lgStatic, t_geometry::lgStaticNoIt, t_ionbal::lgTrimhiOn, t_geometry::lgZoneSet, t_geometry::lgZoneTrp, LIMELM, t_conv::LimFail, LineSave, Magnetic_init(), MALLOC, t_geometry::nend, t_geometry::nEndDflt, NISO, t_conv::nPres2Ioniz, t_geometry::nprint, t_LineSave::nsum, t_conv::nTotalIoniz, NumDeriv, oxy, t_oxy::p1401, t_oxy::p1666, t_carb::p1909, t_carb::p2326, peimbt, PHFIT96, t_hydro::pop2mx, radius, t_continuum::ResolutionScaleFactor, t_radius::router, t_LineSave::ScaleNormLine, t_LineSave::sig_figs, t_timesc::sound_speed_isothermal, state, t_timesc::time_H2_Dest_here, t_timesc::time_H2_Dest_longest, t_timesc::time_H2_Form_here, t_timesc::time_H2_Form_longest, t_timesc::TimeH21cm, timesc, t_ionbal::trimhi, t_ionbal::trimlo, t_peimbt::tsqden, t_LineSave::WavLNorm, and wcnint().
Referenced by cdInit(), hypho(), and optimize_func().
Here is the call graph for this function:
1.4.7