#include <cs_lagr.h>
◆ itsco
source term for the carbon released during heterogeneous combustion
◆ itsfp4
variance of the air scalar
◆ itske
◆ itsli
implicit source term for the continuous phase velocity and for the turbulent energy if the
model is used
◆ itsmas
◆ itsmv1
◆ itsmv2
◆ itsr11
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itsr12
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itsr13
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itsr22
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itsr23
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itsr33
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
◆ itste
explicit thermal source term for the thermal scalar of the continuous phase
◆ itsti
implicit thermal source term for the thermal scalar of the continuous phase
◆ itsvx
explicit source term for the continuous phase X velocity
◆ itsvy
explicit source term for the continuous phase Y velocity
◆ itsvz
explicit source term for the continuous phase Z velocity
◆ 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
activation (=1) or not (=0) of the two-way coupling on the mass. Useful if iilagr = 2, physical_model = 1 and impvar = 1
◆ ltsthe
◆ npts
number of time steps for source terms accumulations
◆ 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
number of cells, whose vulumetric rate DODO (concentration ?)is greather than 0.8
◆ st_val
◆ tmamax
maximum massic concentration reached
◆ vmax
maximum volumetric concentration reached
The documentation for this struct was generated from the following file: