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Data Fields
cs_lagr_source_terms_t Struct Reference

#include <cs_lagr.h>

Collaboration diagram for cs_lagr_source_terms_t:
Collaboration graph

Data Fields

int ltsdyn
 
int ltsmas
 
int ltsthe
 
int itsvx
 
int itsvy
 
int itsvz
 
int itsli
 
int itske
 
int itsr11
 
int itsr12
 
int itsr13
 
int itsr22
 
int itsr23
 
int itsr33
 
int itste
 
int itsti
 
int itsmas
 
int * itsmv1
 
int * itsmv2
 
int itsco
 
int itsfp4
 
int nstits
 
int npts
 
int ntxerr
 
cs_real_t vmax
 
cs_real_t tmamax
 
cs_real_tst_val
 

Field Documentation

§ itsco

int itsco

source term for the carbon released during heterogeneous combustion

§ itsfp4

int itsfp4

variance of the air scalar

§ itske

int itske

§ itsli

int itsli

implicit source term for the continuous phase velocity and for the turbulent energy if the $k-\varepsilon$ model is used

§ itsmas

int itsmas

mass source term

§ itsmv1

int* itsmv1

§ itsmv2

int* itsmv2

§ itsr11

int itsr11

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itsr12

int itsr12

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itsr13

int itsr13

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itsr22

int itsr22

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itsr23

int itsr23

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itsr33

int itsr33

source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase

§ itste

int itste

explicit thermal source term for the thermal scalar of the continuous phase

§ itsti

int itsti

implicit thermal source term for the thermal scalar of the continuous phase

§ itsvx

int itsvx

explicit source term for the continuous phase X velocity

§ itsvy

int itsvy

explicit source term for the continuous phase Y velocity

§ itsvz

int itsvz

explicit source term for the continuous phase Z velocity

§ ltsdyn

int ltsdyn

activation (=1) or not (=0) of the two-way coupling on the dynamics of the continuous phase. Useful if iilagr = 2 and iccvfg = 0

§ ltsmas

int ltsmas

activation (=1) or not (=0) of the two-way coupling on the mass. Useful if iilagr = 2, physical_model = 1 and impvar = 1

§ ltsthe

int ltsthe

§ npts

int npts

number of time steps for source terms accumulations

§ nstits

int nstits

number of absolute time steps (including the restarts) after which a time-average of the two-way coupling source terms is calculated. indeed, if the flow is steady (isttio=1), the average quantities that appear in the two-way coupling source terms can be calculated over different time steps, in order to get a better precision. if the number of absolute time steps is strictly inferior to nstits, the code considers that the flow has not yet reached its steady state (transition period) and the averages appearing in the source terms are reinitialized at each time step, as it is the case for unsteady flows (isttio=0). Useful if iilagr = 2 and isttio = 1

§ ntxerr

int ntxerr

number of cells, whose vulumetric rate DODO (concentration ?)is greather than 0.8

§ st_val

cs_real_t* st_val

source term values

§ tmamax

cs_real_t tmamax

maximum massic concentration reached

§ vmax

cs_real_t vmax

maximum volumetric concentration reached


The documentation for this struct was generated from the following file: