programmer's documentation
Variables
Source terms

Variables

integer, save 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 More...
 
integer, save ltsmas
 activation (=1) or not (=0) of the two-way coupling on the mass. Useful if iilagr = 2, iphyla = 1 and impvar = 1 More...
 
integer, save ltsthe
 if iphyla = 1 and itpvar = 1, ltsthe activates (=1) or not (=0) the two-way coupling on temperature. if iphyla = 2, ltsthe activates (=1) or not (=0) the two-way coupling on the eulerian variables related to pulverised coal combustion. Useful if iilagr = 2 More...
 
integer, save itsvx
 explicit source term for the continuous phase X velocity More...
 
integer, save itsvy
 explicit source term for the continuous phase Y velocity More...
 
integer, save itsvz
 explicit source term for the continuous phase Z velocity More...
 
integer, save itsli
 implicit source term for the continuous phase velocity and for the turbulent energy if the $k-\varepsilon$ model is used More...
 
integer, save itske
 explicit source term for the turbulent dissipation and the turbulent energy if the $k-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr11
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr12
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr13
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr22
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr23
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itsr33
 source term for the Reynolds stress and the turbulent dissipation if the $R_{ij}-\varepsilon$ turbulence model is used for the continuous phase More...
 
integer, save itste
 explicit thermal source term for the thermal scalar of the continuous phase More...
 
integer, save itsti
 implicit thermal source term for the thermal scalar of the continuous phase More...
 
integer, save itsmas
 mass source term More...
 
integer, dimension(ncharm2), save itsmv1
 source term for the light volatile matters More...
 
integer, dimension(ncharm2), save itsmv2
 source term for the heavy volatile matters More...
 
integer, save itsco
 source term for the carbon released during heterogeneous combustion More...
 
integer, save itsfp4
 Variance of the air scalar. More...
 
integer, save nstits
 
integer, save npts
 number of time steps for source terms accumulations More...
 
integer, save ntxerr
 nomber of cells, whose vulumetric rate DODO (concentration ?)is greather than 0.8 More...
 
double precision, save vmax
 maximum volumetric concentration reached More...
 
double precision, save tmamax
 maximum massic concentration reached More...
 

Detailed Description

Variable Documentation

integer, save itsco

source term for the carbon released during heterogeneous combustion

integer, save itsfp4

Variance of the air scalar.

integer, save itske

explicit source term for the turbulent dissipation and the turbulent energy if the $k-\varepsilon$ turbulence model is used for the continuous phase

integer, save itsli

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

integer, save itsmas

mass source term

integer, dimension(ncharm2), save itsmv1

source term for the light volatile matters

integer, dimension(ncharm2), save itsmv2

source term for the heavy volatile matters

integer, save itsr11

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

integer, save itsr12

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

integer, save itsr13

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

integer, save itsr22

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

integer, save itsr23

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

integer, save itsr33

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

integer, save itste

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

integer, save itsti

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

integer, save itsvx

explicit source term for the continuous phase X velocity

integer, save itsvy

explicit source term for the continuous phase Y velocity

integer, save itsvz

explicit source term for the continuous phase Z velocity

integer, save 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

integer, save ltsmas

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

integer, save ltsthe

if iphyla = 1 and itpvar = 1, ltsthe activates (=1) or not (=0) the two-way coupling on temperature. if iphyla = 2, ltsthe activates (=1) or not (=0) the two-way coupling on the eulerian variables related to pulverised coal combustion. Useful if iilagr = 2

integer, save npts

number of time steps for source terms accumulations

integer, save nstits

number of absolute Lagrangian iterations (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 Lagrangian iterations 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

integer, save ntxerr

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

double precision, save tmamax

maximum massic concentration reached

double precision, save vmax

maximum volumetric concentration reached