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programmer's documentation
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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 model is used More... | |
| integer, save | itske |
explicit source term for the turbulent dissipation and the turbulent energy if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr11 |
source term for the Reynolds stress and the turbulent dissipation if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr12 |
source term for the Reynolds stress and the turbulent dissipation if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr13 |
source term for the Reynolds stress and the turbulent dissipation if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr22 |
source term for the Reynolds stress and the turbulent dissipation if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr23 |
source term for the Reynolds stress and the turbulent dissipation if the turbulence model is used for the continuous phase More... | |
| integer, save | itsr33 |
source term for the Reynolds stress and the turbulent dissipation if the 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... | |
| 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
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
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
turbulence model is used for the continuous phase
| integer, save itsr12 |
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
| integer, save itsr13 |
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
| integer, save itsr22 |
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
| integer, save itsr23 |
source term for the Reynolds stress and the turbulent dissipation if the
turbulence model is used for the continuous phase
| integer, save itsr33 |
source term for the Reynolds stress and the turbulent dissipation if the
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 |
| integer, save ltsmas |
| integer, save ltsthe |
| 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 reinitialised 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
1.8.7