%-------------------------------------------------------------------------------

% This file is part of Code_Saturne, a general-purpose CFD tool.
%
% Copyright (C) 1998-2015 EDF S.A.
%
% This program is free software; you can redistribute it and/or modify it under
% the terms of the GNU General Public License as published by the Free Software
% Foundation; either version 2 of the License, or (at your option) any later
% version.
%
% This program is distributed in the hope that it will be useful, but WITHOUT
% ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
% FOR A PARTICULAR PURPOSE.  See the GNU General Public License for more
% details.
%
% You should have received a copy of the GNU General Public License along with
% this program; if not, write to the Free Software Foundation, Inc., 51 Franklin
% Street, Fifth Floor, Boston, MA 02110-1301, USA.

%-------------------------------------------------------------------------------

%==================================
%==================================
\section{Keyword list}
%==================================
%==================================
\label{sec:prg_motscles}

The keywords are classified under relevant headings. For each keyword of \CS Kernel,
the following informations are given:

\noindent
\makebox[2.5cm][l]{Variable name}\makebox[1.3cm][l]{Type}%
\makebox[5cm][l]{Allowed values}%
\makebox[4.cm][l]{[Default]}O/C\hspace{1cm}Level\\
\hspace*{2.5cm}Description\\
\hspace*{2.5cm}Potential dependences


\begin{list}{$\bullet$}{}
\item \textbf{Variable name}: Name of the variable containing the keyword.

\item \textbf{Type}: a (Array), i (Integer), r (Real number), c
      (Character string).

\item \textbf{Allowed values}: list or range of allowed values.

\item \textbf{Default}: value defined by the code before any user
      modification (every keyword has one). In some cases, a
      non-allowed value is given (generally $-999$ or $-10^{12}$), forcing the
      user to specify a value. If he does not do it, the code may:
\begin{list}{-}{}
\item automatically use a recommended value (for example, automatic
      choice of the variables for which chronological records will be
      generated).

\item stop, if the keyword is essential.
\end{list}

\item \textbf{O/C}: Optional/Compulsory
\begin{list}{-}{}
\item O: optional keyword, whose default value may be enough.

\item C: keyword which must imperatively be specified.
\end{list}

\item \textbf{Level}: L1, L2 or L3
\begin{list}{-}{}
\item L1 (level 1): the users will have to modify it in the framework of
      standard applications. The L1 keywords are written in bold.

\item L2 (level 2): the users may have to modify it in the framework of
      advanced applications. The L2 keywords are all optional.

\item L3 (level 3): the developers may have to modify it; it keeps its
      default value in any other case. The L3 keywords are all optional.
\end{list}

\item \textbf{Description}:  keyword description, with its potential
      dependences.

\end{list}

The L1 keywords can be modified through the Graphical Use Interface or
in the \texttt{cs\_user\_parameters.f90} file. L2 and L3 keywords can only be modified through
the \texttt{cs\_user\_parameters.f90} file, even if they do not appear in the version proposed
as example it the \texttt{SRC/REFERENCE/base} directory.\\
It is however recommended not to modify the keywords which do not belong to the L1
level.

The alphabetical keyword list is displayed in the index, in the end of
this report.

\minititre{Notes}
$\bullet\ $The notation ``d'' refers to a double precision real. For
           instance, 1.8d-2 means 0.018. \\
$\bullet\ $The notation ``{\tt grand}'' (which can be used in the code)
corresponds to $10^{12}$.

%==================================
\subsection{Input-output}
%==================================

\minititre{Notes}
\begin{list}{$\bullet$}{}
\item Two different files can have neither the same unit number nor the
      same name.
\end{list}

%==================================
\subsubsection{''Calculation'' files}
%==================================


\minititre{General}

%\minititre{1D wall thermal module}
\minititre{Vortex method for LES}

\motcle{impmvo}{i}{strictly positive integer}{\tt impmvo}{O}{L3}
{unit of the upstream restart file for the vortex method\\
useful if and only if {\tt isuivo = 1} and {\tt ivrtex=1}}

\motcle{impvvo}{i}{strictly positive integer}{\tt impvvo}{O}{L3}
{unit of the downstream restart file for the vortex method\\
useful if and only if {\tt ivrtex=1}}

\motcle{impdvo}{i}{strictly positive integer}{\tt impdvo}{O}{L3}
{unit of the {\tt ficvor} data files for the vortex method. These
files are text files. Their number and names are specified by the user in
the \texttt{usvort} subroutine.\\
(Although it corresponds to an ``upstream'' data file, {\tt impdvo} is
initialized to 20 because, in case of multiple vortex entries,
it is opened at the same time as the {\tt ficmvo} upstream restart file,
which already uses unit 11)\\
useful if and only if {\tt ivrtex=1}}


%\minititre{Radiation}
\minititre{Thermochemistry}

\motcle{impfpp}{i}{strictly positive integer}{25}{O}{L3}
{unit of the thermochemical data file\\
useful in case of gas or pulverised coal combustion or electric arcs}

\motcle{ficfpp}{c}{string of 32 characters}{\tt dp\_tch}{O}{L3}
{name of the thermochemical data file. The launch script is designed to copy the
user specified thermochemical data file in the temporary execution directory
under the name \texttt{dp\_tch}, for \CS to open it properly. Should the value
of {\tt ficfpp} be changed, the launch script would have to be adapted.\\
useful in case of gas or pulverised coal combustion}

\motcle{impjnf}{i}{strictly positive integer}{\tt impfpp}{O}{L3}
{unit of the JANAF data file\\
useful in case of gas or pulverised coal combustion}

\motcle{ficjnf}{c}{string of 5 characters}{\tt JANAF}{O}{L3}
{name of the JANAF data file. The launch script is designed to copy the
user specified JANAF data file in the temporary execution directory
under the name \texttt{JANAF}, for \CS to open it properly. Should the value
of {\tt ficjnf} be changed, the launch script would have to be adapted.\\
useful in case of gas or pulverised coal combustion}

\minititre{Lagrangian}

\motcle{impla1}{i}{strictly positive integer}{50}{O}{L3}
{unit of a file specific to Lagrangian modelling\\
useful in case of Lagrangian modelling}

\motcle{impla2}{i}{strictly positive integer}{51}{O}{L3}
{unit of a file specific to Lagrangian modelling\\
useful in case of Lagrangian modelling}

\motcle{impla3}{i}{strictly positive integer}{52}{O}{L3}
{unit of a file specific to Lagrangian modelling\\
useful in case of Lagrangian modelling}

\motcle{impla4}{i}{strictly positive integer}{53}{O}{L3}
{unit of a file specific to Lagrangian modelling\\
useful in case of Lagrangian mode ling}

\motcle{impla5}{ia}{strictly positive integer}{54 to 68}{O}{L3}
{units of files specific Lagrangian modelling, 15-dimension array\\
useful in case of Lagrangian modelling}


%==================================
\subsubsection{Post-processing for {\em EnSight} or other tools}
%==================================

\minititre{Notes}
$\bullet\quad$The format depends on the user choices, and most options
are defined using the GUI or \\
\texttt{cs\_user\_postprocess.c}.\\
$\bullet\quad$The post-processing files can be of the following formats: {\em Ensight Gold},
{\em MED} or {\em CGNS}. The use of the two latter formats depends on
the installation of the corresponding external libraries.\\
$\bullet\quad$For each quantity (problem unknown, preselected numerical
variable or preselected physical parameter), the user specifies if a
post-processing output is wanted. The output frequency can be set.\\

\motcleb{keyvis}{ifk}{field key, 0, 1, 2, or 3}{0}{O}{L1}
{for each quantity defined at the cell centres (physical or numerical
variable), indicator of whether it should be post-processed or not \\
\hspace*{1.3cm}= -999: not initialised. By default, the post-processed
quantities are the unknowns (pressure, velocity, $k$, $\varepsilon$,
$R_{ij}$, $\omega$, $\varphi$, $\overline{f}$, scalars), density,
turbulent viscosity and the time step if is not uniform\\
\hspace*{1.3cm}= 0: not post-processed\\
\hspace*{1.3cm}= 1: post-processed on main location\\
\hspace*{1.3cm}= 2: non-reconstructed values postprocessed on boundary if main location is cells\\
\hspace*{1.3cm}= 3: both 1 and 2\\
useful if and only if the variable is defined at the cell centers or boundary faces:
calculation variable, physical property (time step, density,
viscosity, specific heat) or turbulent viscosity if {\tt iturb}
$\geqslant$ 10}

%==================================
\subsubsection{Chronological records of the variables on specific points}
%==================================

\minititre{Standard use through Interface or \texttt{cs\_user\_parameters.f90}}
For each quantity (problem unknown, preselected numerical variable or
preselected physical parameter), the user indicates whether chronological records
should be generated, the output period and the position of the
probes. The code generates chronological records at the cell centers located
closest to the geometric points defined by the user by means of their
coordinates. For each quantity, the number of probes and their
index-numbers must be specified (it is not mandatory to generate all
the variables at all the probes).


\motcleb{ncapt}{i}{positive or null integer}{0}{O}{L1}
{total number of probes (limited to {\tt ncaptm}=100)\\
always useful }

\motcleb{xyzcap}{ra}{real numbers}{0.0}{O}{L1}
{3D-coordinates of the probes\\
the coordinates are written: {\tt xyzcap(i,j)}, with $i$ = 1, 2 or 3 and $j$
$\leqslant$ {\tt ncapt}\\
useful if and only if {\tt ncapt} $>$ 0}

\motcleb{ihisvr}{ia}{-999, -1 or positive or null integer}{-999}{O}{L1}
{number {\tt ihisvr(n, 1)} and index-numbers {\tt ihisvr(n, j$>$1)} of the recording
probes to be used for each variable, {\em i.e.} calculation variable
or physical property defined at the cell centers.
With {\tt ihisvr(n, 1)}=-999 or -1, {\tt ihisvr(n, j$>$1)} is useless.\\
\hspace*{.5cm} $\bullet$ {\tt ihisvr(n, 1)}: number of recording probes to use
for the variable N\\
\hspace*{1.3cm}= -999: default value: chronological records are generated on
all the probes if N is one of the main variables (pressure, velocity,
turbulence, scalars), the local time step or the turbulent
viscosity. For the other quantities, no chronological record is generated.\\
\hspace*{1.3cm}= -1: chronological records are produced on all the probes\\
\hspace*{1.3cm}= 0: no chronological record on any probe\\
\hspace*{1.3cm}$>0$: chronological record on {\tt ihisvr(n, 1)} probes to be
specified with  {\tt ihisvr(n, j$>$1)}\\
always useful, must be less than or equal to {\tt ncapt}\\
\hspace*{.5cm} $\bullet$ {\tt ihisvr(n, j$>$1)}: index-numbers of the probes
used for the variable $n$\\
(with $j \leqslant${\tt ihisvr(n,1)+1)}\\
\hspace*{1.3cm}= -999: by default: if {\tt ihisvr(n, 1)} $\ne$
-999, the  code stops. Otherwise, refer to the description of the case
{\tt ihisvr(n, 1)}=-999\\
useful if and only if {\tt ihisvr(n, 1)} $>$ 0 \\
The condition {\tt ihisvr(n, j)} $\leqslant${\tt ncapt} must be respected.\\
For ease to use, it is recommended to simply specify {\tt ihisvr(n,1)}=-1 for
all of the interesting variables.}

\motcle{emphis}{c}{string of less than 80 characters}{\tt ./}{O}{L3}
{directory in which potential chronological record files generated by
the Kernel will be written (path related to the execution directory)\\
it is recommended to keep the default value and, if necessary, to modify the
launch script to copy the files in the alternate destination directory\\
useful if and only if chronological record files are generated ({\em
i.e.} there is {\tt n} for which {\tt ihisvr(n, 1)} $\ne$ 0)}

\motcleb{nthist}{i}{-1 or strictly positive integer}{1 or -1}{O}{L1}
{output period of the chronological record files\\
\hspace*{1.3cm}= -1: no output\\
\hspace*{1.3cm}$>$ 0: period  (every {\tt nthist} time step)\\
The default value is -1 when there is no chronological record file to
generate (if there is no probe, {\tt ncapt} = 0, or if {\tt ihisvr(n, 1)}=0 for
all the variables) and 1 otherwise\\
If chronological records are generated, it is usually best to keep the default
value {\tt nthist}=1, in order to avoid missing any high frequency evolution (unless
the total number of time steps is too large to do so)\\
useful if and only if chronological record files are generated ({\em
i.e.} there are probes ({\tt ncapt}$>$0) or  there is {\tt n} for which
{\tt ihisvr(n, 1)} $\ne$ 0)}

\motcle{nthsav}{i}{-1 or positive or null integer}{0}{O}{L3}
{saving period the chronological record files (they are first stored in a
temporary file and then saved every {\tt nthsav} time step)\\
\hspace*{1.3cm}= 0: by default (4 times during a calculation)\\
\hspace*{1.3cm}= -1: saving at the end of the calculation\\
\hspace*{1.3cm}$>$ 0: period (every {\tt nthsav} time step)\\
During the calculation, the user can read the chronological record files
in the execution directory when they have been saved, {\em i.e.} at the first
time step, at the tenth time step and when the time step number is a multiple of
{\tt nthsav} (multiple of {\tt (ntmabs-ntpabs)/4} if {\tt nthsav}=0)\\
{\em Note: using the \texttt{control\_file} file enables to update the value of
{\tt ntmabs}. Hence, if the calculation is at the time step n, a save of the
chronological record files can be forced by changing {\tt ntmabs} to
{\tt ntpabs}+4(n+1)
using \texttt{control\_file}; after the files have been saved, {\tt ntmabs} can be
reset to its original value, still using \texttt{control\_file}.}\\
useful if and only if chronological record files are generated ({\em
i.e.} there are probes ({\tt ncapt}$>$0) there is {\tt n} for which
{\tt ihisvr(n, 1)} $\ne$ 0)}

\minititre{Non-standard use through \texttt{ushist}}
(see p.~\pageref{sec:prg_ushist})

\motcle{impush}{ia}{strictly positive integer}{33 to 32+\texttt{nushmx}=49}{O}{L3}
{units of the user chronological record files\\
useful if and only if the subroutine \texttt{ushist} is used}

\motcle{ficush}{ca}{strings of 13 characters}{\texttt{ush*} or
\texttt{ush*.n\_*}}{O}{L2}
{names of the user chronological record files.
In the case of a non-parallel calculation, the suffix applied the file
name is a three digit number: \texttt{ush001}, \texttt{ush002},
\texttt{ush003}...
In the case of a parallel-running calculation, the processor
index-number is added to the suffix. For instance, for a calculation
running on two processors:  \texttt{ush001.n\_0001},
\texttt{ush002.n\_0001}, \texttt{ush003.n\_0001}... and
\texttt{ush001.n\_0002},
\texttt{ush002.n\_0002}, \texttt{ush003.n\_0002}...
The opening, closing, format and location of these files must be managed
by the user.\\
useful if and only if the subroutine \texttt{ushist} is used}

%==================================
\subsubsection{Time averages}
%==================================
See \doxygenfile{parameters.html}{the dedicated \texttt{Doxygen} documentation}.

%==================================
\subsubsection{Others}
%==================================

\motcle{impusr}{ia}{strictly positive integer}{{\tt 70} to {\tt 69+nusrmx}=79}{O}{L3}
{unit numbers for potential user specified files\\
useful if and only if the user needs files (therefore always useful, by security)}

\motcleb{ficusr}{ca}{string of 13 characters}{\tt usrf* or usrf*.n\_*}{O}{L1}
{name of the potential user specified files. In the case of a non-parallel
calculation, the suffix applied the file name is a two digit number:
from \texttt{usrf01} to \texttt{usrf10}. In the case of a
parallel-running calculation, the four digit processor index-number is
added to the suffix. For instance, for a calculation running on two
processors: from \texttt{usrf01.n\_0001} to \texttt{usrf10.n\_0001} and
from \texttt{usrf01.n\_0002} to \texttt{usrf10.n\_0002}. The opening,
closing, format and location of these files must be managed by the user.\\
useful if and only if the user needs files (therefore always useful, by security)}

\motcleb{keylog}{ifk}{1 or 0}{-1}{O}{L1}
{for every quantity (variable, physical or numerical property ...),
indicator concerning the writing in the execution report file \\
\hspace*{1.3cm}= 1: writing in the execution listing.\\
\hspace*{1.3cm}= 0: no writing.\\
always useful}

\motcleb{iwarni}{ia}{integer}{0}{O}{L1}
{{\tt iwarni(ivar)} characterises the level of detail of the outputs for the
variable {\tt ivar} (from 1 to {\tt nvar}). The quantity of information
increases with its value.\\
Impose the value 0 or 1 for a reasonable listing size. Impose the value 2
to get a maximum quantity of information, in case of problem during the
execution.\\
always useful}

\motcleb{nomvar}{ca}{string of less than 80 characters}{``''}{O}{L1}
{name of the variables (unknowns, physical properties ...): used in the
execution listing, in the post-processing files, etc.\\
{``''}: not initialised (the code chooses the manes by default)\\
It is recommended not to define variable names of more than 16
characters, to get a clear execution listing (some advanced writing
levels take into account only the first 16 characters).\\
always useful}

\motcleb{ntlist}{i}{-1 or strictly positive integer}{1}{O}{L1}
{writing period in the execution report file\\
\hspace*{1.3cm}= -1: no writing\\
\hspace*{1.3cm}$>$ 0: period (every {\tt ntlist} time step)\\
The value of {\tt ntlist} must be adapted according to the number of iterations
carried out in the calculation. Keeping {\tt ntlist} to 1 will indeed provide
a maximum volume of information, but if the number of time steps is too large,
the execution report file might become too big and unusable
(problems with disk space, memory problems while opening the file with a text
editor, problems finding the desired information in the file, ...).\\
always useful}

\motcle{ntsuit}{i}{-1, 0 or positive or null integer}{0}{O}{L3}
{saving period of the restart files\\
\hspace*{1.3cm}= -2: no restart at all\\
\hspace*{1.3cm}= -1: only at the end of the calculation\\
\hspace*{1.3cm}= 0: by default (four times during the calculation)\\
\hspace*{1.3cm}$>$ 0: period\\
always useful}


%==================================
\subsection{Numerical options}
%==================================
\subsubsection{Calculation management}
%==================================

\motcle{iecaux}{i}{0 or 1}{1}{O}{L2}
{indicates the writing (=1) or not (=0) of the auxiliary calculation
restart file\\
always useful}

\motcle{ileaux}{i}{0 or 1}{1}{O}{L2}
{indicates the reading (=1) or not (=0) of the auxiliary
calculation restart file\\
useful only in the case of a calculation restart}

\motcleb{inpdt0}{i}{0 or 1}{0}{O}{L1}
{indicates the calculation mode: 1 for a zero time step control
calculation, {\em i.e.} without solving the transport equations,
and 0 for a standard calculation.\\
In case of a calculation using the control mode ({\tt inpdt0}=1), when the
calculation is not a restart, the equations are not solved, but the
physical properties and the boundary conditions are calculated. When
the calculation is a restart, the physical properties and the boundary
conditions are those read from the restart file (note: in the case of a
second-order time scheme, the mass flow is modified as if a normal
time step was realised: the mass flow generated in an potential
post-processing is therefore not the mass flow read from the restart file).\\
In the control mode ({\tt inpdt0}=1), the variable {\tt ntmabs} is not used.\\
In the standard mode ({\tt inpdt0}=0), the code solves the equations at least
once, even if {\tt ntmabs}=0.\\
always useful}

\motcleb{isuite}{i}{0 or 1}{0}{C}{L1}
{indicator of a calculation restart (=1) or not (=0)\\
always useful. This value is set automatically by the code; depending on
whether a restart directory is present, and should not be modified by
the user}

\motcle{ntcabs}{i}{integer}{\tt ntpabs}{O}{L3}
{current time step number\\
always useful\\
{\tt ntcabs} is initialised and updated automatically by the code,
its value is not to be modified by the user}

\motcleb{ntmabs}{i}{integer $>$ {\tt ntpabs}}{10}{C}{L1}
{number of the last time step after which the calculation stops. It is
an absolute number: for the restart calculations, {\tt ntmabs} takes into
account the number of time steps of the previous calculations. For
instance, after a first calculation of 3 time steps, a restart file of 2
time steps is realised by setting {\tt ntmabs}=3+2=5\\
always useful}

\motcle{ntpabs}{i}{integer}{0, read}{O}{L3}
{number of the last time step in the previous calculation. In the case of
a restart calculation, {\tt ntpabs} is read from the restart file. Otherwise
it is initialised to 0\\
always useful\\
{\tt ntpabs} is initialised automatically by the code, its value is not to
be modified by the user}

\motcle{tmarus}{r}{-1 or strictly positive real}{-1}{O}{L3}
{margin in seconds on the remaining CPU time which is necessary to allow
the calculation to stop automatically and write all the required results
(for the machines having a queue manager)\\
\hspace*{1.3cm}= -1: calculated automatically\\
\hspace*{1.3cm}$>$ 0: margin defined by the user\\
always useful, but the default value should not be changed
unless absolutely necessary.}


\motcle{ttcabs}{r}{positive or null real number}{\tt ttpabs}{O}{L3}
{physical simulation time at the current time step. For the restart
calculations, \mbox{ttcabs} takes into account the physical time of the
previous calculations.\\
If the time step is uniform ({\tt idtvar}=0 or 1), {\tt ttcabs} increases
of {\tt dt} (value of the time step) at each iteration. If the time step is
non-uniform ({\tt idtvar}=2),
{\tt ttcabs} increases of {\tt dtref} at each time step.\\
always useful\\
{\tt ttcabs} is initialised and updated automatically by the code,
its value is not to be modified by the user}

\motcle{ttpabs}{r}{positive or null real number}{0, read}{O}{L3}
{simulation physical time at the last time step of the previous
calculation. In the case of a restart calculation, {\tt ttpabs} is read from
the restart file. Otherwise it is initialised to 0.\\
always useful\\
{\tt ttcabs} is initialised automatically by the code, its value is not to
be modified by the user}

%==================================
\subsubsection{Scalar unknowns}
%==================================

\motcleb{nscaus}{i}{0$\leqslant$ integer $\leqslant$ {\tt nscmax}}{0}{O}{L1}
{number of user scalars solutions of an advection equation\\
always useful}

\motcleb{itherm}{ia}{0, 1, 2 or 3}{0}{O}{L1}
{\hspace*{1.3cm}= 0: no thermal model\\
\hspace*{1.3cm}= 1: temperature\\
\hspace*{1.3cm}= 2: enthalpy\\
\hspace*{1.3cm}= 3: total energy (only for compressible module).\\
When a particular physics module is activated (gas combustion, pulverised coal,
electricity or compressible), the user must not modify {\tt itherm} (the choice
is made automatically: the solved variable is either the enthalpy or the total
energy). The user is also reminded that, in the case of a coupling with
\syrthes, the solved thermal variable should be the temperature
({\tt itherm}=1).
More precisely, everything is designed in the code to allow for the
running of a calculation coupled with \syrthes with the enthalpy as thermal
variable (the correspondence and conversion is then specified by the user in
the subroutine \texttt{usthht}).
However this case has never been used in practice and has therefore not been
tested. With the compressible model, it is possible to carry out calculations
coupled with \syrthes, although the thermal scalar represents the total
energy and not the temperature.}

\motcleb{iscalt}{ia}{-1 or integer $>$ 0}{-1}{O}{L1}
{{\tt iscalt} is the index-number of the scalar
representing the temperature or the enthalpy. If {\tt iscalt}=-1, neither
the temperature nor the enthalpy is represented by a scalar. When a specific
physics module is activated (gas combustion, pulverised coal,
electricity or compressible),
the user must not modify {\tt iscalt} (the choice is made
automatically)\footnote{In the case of the compressible module, {\tt iscalt}
does not correspond to the temperature nor enthalpy but to the total energy}.\\
useful if and only if {\tt nscal} $\geqslant$ 1.}

\motcleb{iscacp}{ia}{0 or 1}{0}{O}{L2}
{\hspace*{1.3cm}= 0: scalar does not behave like a temperature\\
\hspace*{1.3cm}= 1: scalar behaves like a temperature
(use $C_p$ for wall law).\\
useful if and only if {\tt nscal} $\geqslant$ 1.}

\motcleb{itpscl}{ia}{0, 1 or 2}{0}{O}{L1}
{\hspace*{1.3cm}= 0: none\\
\hspace*{1.3cm}= 1: Kelvin\\
\hspace*{1.3cm}= 2: Celsius\\
The distinction between {\tt itpscl} = 1 or 2 is useful only in case of
radiation modelling. For calculations without radiation modelling,
use {\tt itpscl}=1 for the temperature.\\
useful if and only if {\tt nscal} $\geqslant$ 1.}

\motcle{iclvfl}{ia}{-1, 0, 1 or 2}{-1}{O}{L3}
{for every scalar {\tt iscal} representing the average of the square of the
fluctuations of another scalar {\tt ii=iscavr(iscal)} (noted $f$),
indicator of the clipping method\\
\hspace*{1.3cm}= -1: no clipping because the scalar does not represent
the average of the square of the fluctuations of another scalar\\
\hspace*{1.3cm}= 0: clipping to 0 for the lower range of values\\
\hspace*{1.3cm}= 1: clipping to 0 for the lower range of values and to
\mbox{$(f-f_{min})(f_{max}-f)$} for higher values, where $f$ is
the associated scalar, $f_{min}$ and $f_{max}$ its minimum and maximum
values specified by the user ({\em i.e.} {\tt scamin(ii)} and {\tt scamax(ii)}) \\
\hspace*{1.3cm}= 2: clipping to {\tt max(0,scamin(iscal))} for lower
values and to {\tt scamax(iscal)} for higher values. {\tt scamin} and {\tt scamax}
are limits specified by the user\\
useful for the scalars {\tt iscal} for which {\tt iscavr(iscal)}$>$0.}

\motcle{itbrrb}{i}{0 or 1}{0}{O}{L3}
{Reconstruction (=1) or not (=0) of the temperature, enthalpy or total energy
value in the boundary cells. Useful in the case of coupling with \syrthes
and with radiation.}

\motcle {icpsyr}{ia}{-999,0,1}{-999}{O}{L3}
{For each scalar {\tt iscal}, {\tt icpsyr(iscal)} indicates whether it is
coupled with \syrthes (=1) or not (=0).
There can be only one coupled scalar per calculation.\\
\hspace*{1.3cm}=-999: by default\\
\hspace*{2.cm} $\bullet$ {\tt icpsyr(iscal)}=1 for the thermal scalar
{\tt iscal=(iscalt)} when a coupling with \syrthes has been specified\\
\hspace*{2.cm} $\bullet$ {\tt icpsyr(iscal)}=0 otherwise\\
\hspace*{1.3cm}= 0: the scalar {\tt iscal} is not coupled with \syrthes\\
\hspace*{1.3cm}= 1: the scalar {\tt iscal} is coupled with \syrthes\\
useful in case of coupling with \syrthes}


%==================================
\subsubsection{Definition of the equations}
%==================================

\motcle{istat}{ia}{0 or 1}{1 or 0}{O}{L2}
{for each unknown {\tt ivar} to calculate, indicates whether
unsteady terms are present ({\tt istat(ivar)}=1) or not (0) in the matrices.\\
By default, {\tt istat} is set to 0 for the pressure (variable {\tt ivar=ipr})
or $\overline{f}$ in v2f modelling (variable {\tt ivar=ifb}) and set to
1 for the other unknowns.\\
useful for all the unknowns}

\motcle{iconv}{ia}{0 or 1}{1 or 0}{O}{L2}
{for each unknown {\tt ivar} to calculate, indicates if the
convection is taken into account ({\tt iconv(ivar)}=1) or not (0).\\
By default, {\tt iconv} is set to 0 for the pressure (variable {\tt ivar=ipr})
or $\overline{f}$ in v2f modelling (variable {\tt ivar=ifb}) and set to
1 for the other unknowns.\\
useful for all the unknowns}

\motcle{idiff}{ia}{0 or 1}{1}{O}{L2}
{for each unknown {\tt ivar} to calculate, indicates whether the
diffusion is taken into account ({\tt idiff(ivar)}=1) or not (0)\\
useful for all the unknowns}

\motcle{idifft}{ia}{0 or 1}{1}{O}{L3}
{for each unknown {\tt ivar} to calculate, when diffusion is taken
into account ({\tt idiff(ivar)}=1), {\tt idifft(ivar)} indicates if the turbulent
diffusion is taken into account ({\tt idifft(ivar)}=1) or not (0)\\
useful for all the unknowns }

\motcle{idircl}{ia}{0 or 1}{1 or 0}{O}{L3}
{for each unknown {\tt ivar} to calculate, indicates whether the diagonal
of the matrix should be slightly shifted ({\tt idircl(ivar)}=1) or not (0) if there
is no Dirichlet boundary condition and if {\tt istat}=0. Indeed, in such a case,
the matrix for the general advection/diffusion equation is singular. A slight
shift in the diagonal will make it invertible again.\\
By default, {\tt idircl} is set to 1 for all the unknowns, except $\overline{f}$ in
v2f modelling, since its equation contains another diagonal term that ensures
the regularity of the matrix.\\
useful for all the unknowns}

\motcle{ivisse}{ia}{0 or 1}{1}{O}{L3}
{indicates whether the source terms in transposed gradient
and velocity divergence should be taken into account in the momentum
equation. In the compressible module, these terms also account for the volume
viscosity (cf. {\tt viscv0} and {\tt iviscv}):\\
$\partial_i \left[(\kappa -2/3\,(\mu+\mu_t))\partial_k U_k  \right]
 +     \partial_j \left[ (\mu+\mu_t)\partial_i U_j \right]$ \\
\hspace*{1.3cm}= 0: not taken into account\\
\hspace*{1.3cm}= 1: taken into account\\
always useful}


%==================================
\subsubsection{Definition of the time advancement}
%==================================

\motcleb{idtvar}{i}{-1, 0, 1, 2}{0}{O}{L1}
{type of time step\\
\hspace*{1.3cm}= 0: constant in time and spatially uniform\\
\hspace*{1.3cm}= 1: variable in time and spatially uniform\\
\hspace*{1.3cm}= 2: variable in time and in space\\
\hspace*{1.3cm}= -1: steady-state algorithm\\
If the numerical scheme is a second-order in time, only the option 0 is
allowed.\\
always useful}

\motcleb{idilat}{i}{1, 2, 3, 4}{1}{O}{L1}
{Algorithm to take into account the density variation in time\\
\hspace*{1.3cm}= 1: steady dilatable flow algorithm (default)\\
\hspace*{1.3cm}= 2: unsteady dilatable flow algorithm\\
\hspace*{1.3cm}= 3: low-Mach number algorithm\\
\hspace*{1.3cm}= 4: non conservative algorithm for fire simulation\\
always useful}

\motcle{iptlro}{i}{0 or 1}{0}{O}{L2}
{when density gradients and gravity are present, a local thermal time
step can be calculated, based on the Brunt-Vaisala frequency. In numerical
simulations, it is usually wise for the time step to be lower than this limit,
otherwise numerical instabilities may appear\\
{\tt iptlro} indicates whether the time step should be limited to the local thermal
time step (=1) or not (=0)\\
when {\tt iptlro}=1, the listing shows the number of cells where the time step has
been clipped due to the thermal criterion, as well as the maximum ratio between
the time step and the maximum thermal time step. If {\tt idtvar}=0, since the time
step is fixed and cannot be clipped, this ratio can be greater than
1\footnote{It is then the user's
choice to decide whether he should diminish DTREF or not}. When {\tt idtvar}$>$0, this
ratio will be less than 1, except if the constraint {\tt dtmin} has prevented the
code from reaching a sufficiently low value for {\tt dt}\\
useful when density gradients and gravity are present}

\motcleb{cdtvar}{ra}{strictly positive real number}{1}{O}{L1}
{multiplicative factor applied to the time step for each scalar\\
Hence, the time step used when solving the evolution equation for the
variable is the time step used for the dynamic equations (velocity/pressure)
multiplied by {\tt cdtvar}.\\
The size of the array {\tt cdtvar} is {\tt nvar}. For instance, the multiplicative
coefficient applied to the scalar 2 is {\tt cdtvar(isca(2))}). Yet, the value of
{\tt cdtvar} for the velocity components and the pressure is not used. Also,
although it is possible to change the value of {\tt cdtvar} for the turbulent
variables, it is highly not recommended\\
useful if and only if {\tt nscal} $\geqslant$ 1}


\motcle{coumax}{r}{strictly positive real number}{1}{O}{L1}
{target Courant number (local or maximum) in case of non-constant time step\\
useful if {\tt idtvar} $\ne$ 0}

\motcle{foumax}{r}{strictly positive real number}{10}{O}{L1}
{target Fourrier nmber (local or maximum) in case of non-constant time step\\
useful if {\tt idtvar} $\ne$ 0}

\motcleb{dtref}{r}{strictly positive real number}{\tt -grand*10}{C}{L1}
{reference time step value\\
always useful.\\
This is the time step value used in the case of a calculation run with a
uniform and constant time step, {\em i.e.} {\tt idtvar}=0 (restart calculation
or not). It is the value used to initialise the time step in the case of
an initial calculation run with a non-constant time step
({\tt idtvar}=1 or 2). It is also the value used to initialise the time step
in the case of a restart calculation in which the type of
time step has been changed (for instance, {\tt idtvar}=1 in the new
calculation and {\tt idtvar}=0 or 2 in the previous calculation): see
\texttt{cs\_user\_initialization}}

\motcle{dtmin}{r}{positive or null real number}{\tt 0.1*dtref}{O}{L2}
{lower limit for the calculated time step when non-constant time step is activated\\
useful if {\tt idtvar} $\ne$ 0}

\motcle{dtmax}{r}{strictly positive real number}{\tt 1000*dtref}{O}{L2}
{upper limit for the calculated time step when non-constant time step is activated\\
useful if {\tt idtvar} $\ne$ 0}

\motcle{varrdt}{r}{strictly positive real number}{0.1}{O}{L3}
{maximum allowed relative increase in the calculated time step value
between two successive time steps (to ensure stability, any decrease in the time step
is immediate and without limit)\\
useful if {\tt idtvar} $\ne$ 0}

\motcle{relxst}{r}{0 $<$ real $\leqslant$ 1}{0.9}{O}{L2}
{relaxation coefficient for the steady algorithm
 ({\tt relaxp}=1: no relaxation)\\
useful if {\tt idtvar}=-1}

\motcle{relaxv}{ra}{0 $\leqslant$ real $\leqslant$ 1}{0.7 or 1.}{O}{L3}
{for each variable {\tt ivar}, relaxation coefficient of the variable.
This relaxation parameter is only useful for the pressure with the unsteady
algorithm (so as to improve the convergence in case of meshes of insufficient
quality or and for some of the turbulent models ({\tt iturb} = 20, 21,
50 or 60 and {\tt ikecou}=0; if {\tt ikecou}=1, {\tt relaxv(ivar)}
is not used, whatever its value may be). Default values are 0.7 for turbulent
variables and 1. for pressure.\\
{\tt relaxv} also stores the value of the relaxation coefficient when using the steady
algorithm, deduced from the value of {\tt relxst} (defaulting to
 {\tt relaxv(ivar} $eq$  {1. - \tt relxst})\\
useful only for the pressure and for turbulent variables
if and only if ($k-\varepsilon$, v2f or $k-\omega$ models without coupling)
 with the unsteady algorithm\\
always useful with the steady algorithm}


\minititre{Non-constant time step}
The calculation of the time step uses a reference time step DTREF (at
the calculation beginning). Later, every time step, the time step value
is calculated by taking into account the different existing limits, in
the following order: \\
\hspace*{1.cm}$\bullet$ {\tt coumax}, {\tt foumax}: the more restrictive limit between
both is used (in the compressible module, the acoustic limitation is added),\\
\hspace*{1.cm}$\bullet$ {\tt varrdt}:  progressive increase and immediate
decrease in the time step,\\
\hspace*{1.cm}$\bullet$ {\tt iptlro}: limitation by the thermal time step,\\
\hspace*{1.cm}$\bullet$ {\tt dtmax} and {\tt dtmin}: clipping of the time step to
the maximum, then to the minimum limit.\\


%==================================
\subsubsection{Turbulence}
%==================================

\motcleb{iturb}{i}{
\begin{tabular}{l}
0, 10, 20, 21, 30, 31, 32, \\
40, 41, 42, 50, 51, 60, 70
\end{tabular}
}{-999}{O}{L1}
{indicator of the turbulence model {\tt iturb}\\
\hspace*{1.3cm}= -999: not initialised. This value is not allowed and
must be modified by the user\\
\hspace*{1.3cm}= 0: laminar\\
\hspace*{1.3cm}= 10: mixing length (not valided)\\
\hspace*{1.3cm}= 20: $k-\varepsilon$\\
\hspace*{1.3cm}= 21: $k-\varepsilon$ with linear production (Laurence \& Guimet)\\
\hspace*{1.3cm}= 30: $R_{ij}-\varepsilon$ ``standard'' LRR (Launder, Reece \& Rodi)\\
\hspace*{1.3cm}= 31: $R_{ij}-\varepsilon$ SSG (Speziale, Sarkar \& Gatski)\\
\hspace*{1.3cm}= 32: $R_{ij}-\varepsilon$ EBRSM (elliptic blending)\\
\hspace*{1.3cm}= 40: LES (Smagorinsky model) \\
\hspace*{1.3cm}= 41: LES (dynamic model) \\
\hspace*{1.3cm}= 42: LES (WALE model) \\
\hspace*{1.3cm}= 50: v2-f, $\varphi$-model version\\
\hspace*{1.3cm}= 51: v2-f, BL-v2/k version\\
\hspace*{1.3cm}= 60: $k-\omega$, SST version \\
\hspace*{1.3cm}= 70: Spalart-Allmaras \\
always useful}

The $k-\varepsilon$ (standard and linearized production) and $R_{ij}-\varepsilon$
(LRR and SSG) turbulence
models implemented in \CS are ``High-Reynolds'' models. It is therefore
necessary to make sure that the thickness of the first cell neighboring
the wall is larger than the thickness of the viscous sub-layer (at the
wall, $y^+>2.5$ is required as a minimum, and preferably between 30 and
100)\footnote{While creating the mesh, $y^+=\frac{yu*}{\nu}$ is
generally unknown. It can be roughly estimated as $\frac{yU}{10\nu}$, where
$U$ is the characteristic velocity, $\nu$ is the kinematic viscosity of the fluid
 and $y$ is the mid-height of the first cell near the wall.}. If the mesh does
 not respect this condition, the results may be biased
(particularly if thermal processes are involved). Using scalable wall-functions
(cf. keyword {\tt iwallf}) may help avoiding this problem.\\
The v2-f model is a ``Low-Reynolds'' model, it is therefore necessary to
make sure that the thickness of the first cell neighboring the wall is
smaller than the thickness of the viscous sub-layer ($y^+<1$).\\
The $k-\omega$ SST model provides correct results whatever the thickness of the first cell.
Yet, it requires the knowledge of the distance to the wall in every
cell of the calculation domain. The user may refer to the keyword
{\tt icdpar\index{icdpar}} for more details about the potential limitations.\\
The $k-\varepsilon$ model with linear production allows to correct the
known flaw of the standard $k-\varepsilon$ model which overestimates the
turbulence level in case of strong velocity gradients (stopping point).\\
With LES, the wall functions are usually not greatly adapted. It is generally more advisable
(if possible) to refine the mesh towards the wall so that the first cell is in the
viscous sub-layer, where the boundary conditions are simple natural no-slip conditions.\\
Concerning the LES model, the user may refer to the subroutine
\texttt{ussmag} for complements about the dynamic model. Its usage
and the interpretation of its results require particular attention.
In addition, the user must pay further attention when using the dynamic
model with the least squares method based on a partial extended
neighbourhood ({\tt imrgra}=3). Indeed, the results may be degraded if the user
does not implement his own way of averaging the dynamic constant in
\texttt{ussmag} (\textit{i.e.} if the user keeps the local average based
on the extended neighbourhood).\\

\motcleb{iturt}{ia}{0, 10, 20 or 30}{0}{O}{L2}
{indicator of the turbulent flux model $ \overline{\varia^\prime \vect{u}^\prime}$
for any scalar $\varia$\\
\hspace*{1.3cm}= 0: Simple Gradient Diffusion Hypothesis (SGDH) (default value)\\
\hspace*{1.3cm}= 10: Generalized Gradient Diffusion Hypothesis (GGDH)\\
\hspace*{1.3cm}= 20: Algebraic Flux Model (AFM)\\
\hspace*{1.3cm}= 30: Differential Flux Model (DFM: transport equations of the turbulent flux)\\
GGDH, AFM and DFM are only available when a second order closure is used ({\em i.e.} {\tt iturb}=30, 31, 32).
}

\motcle{iwallf}{i}{0, 1, 2, 3, 4 or 5}{3}{O}{L2}
{indicates the type of wall function is used for
 the velocity boundary conditions on a frictional wall.\\
\hspace*{1.3cm}= 0: no wall functions\\
\hspace*{1.3cm}= 1: one scale of friction velocities (power law)\\
\hspace*{1.3cm}= 2: one scale of friction velocities (log law)\\
\hspace*{1.3cm}= 3: two scales of friction velocities (log law)\\
\hspace*{1.3cm}= 4: two scales of friction velocities (log law) - scalable wall functions\\
\hspace*{1.3cm}= 5: two scales of friction velocities (mixing length based on V. Driest analysis)\\
{\tt iwallf} is initialised to 2 for {\tt iturb}=10, 40, 41 or 70
(mixing length, LES and Spalart Allmaras).\\
{\tt iwallf} is initialised to 0 for {\tt iturb}=0, 32, 50 or 51\\
{\tt iwallf} is initialised to 3 for {\tt iturb}=20, 21, 30, 31 or 60
($k-\varepsilon$, $R_{ij}-\varepsilon$ LRR, $R_{ij}-\varepsilon$ SSG and
$k-\omega$ SST models).\\
The v2f model ({\tt iturb}=50) is not designed to use wall functions
(the mesh must be ``low Reynolds'').\\
The value {\tt iwallf}=3 is not compatible with {\tt iturb}=0, 10, 40
or 41 (laminar, mixing length and LES).\\
Concerning the $k-\varepsilon$ and $R_{ij}-\varepsilon$ models, the
two-scales model is usually at least as satisfactory as the one-scale
model.\\
The scalable wall function allows to virtually ``shift'' the wall when
necessary in order to be always in a logarithmic layer.
It is used to make up for
the problems related to the use of High-Reynolds models on very refined
meshes.\\
useful if {\tt iturb} is different from 50}

\motcle{ilogpo}{i}{0 or 1}{1}{O}{L3}
{type of wall function used for the velocity: power law
({\tt ilogpo}=0, deprecated) or logarithmic law ({\tt ilogpo}=1)\\
always useful}

\motcle{ypluli}{r}{real number $>$ 0}{\tt 1/xkappa, 10.88}{O}{L3}
{limit value of $y^+$ for the viscous sub-layer\\
{\tt ypluli} depends on the chosen wall function: it is
initialised to 10.88 for the scalable wall function ({\tt iwallf}=2),
otherwise it is initialised to $1/\kappa\approx 2,38$\\
In LES, {\tt ypluli} is taken by default to be 10.88\\
always useful}

\minititre{ $k-\varepsilon$, $k-\varepsilon$ with linear production,
v2-f and $k-\omega$ SST}

\motcle{igrake}{i}{0 or 1}{1}{O}{L1}
{indicates if the terms related to gravity in the
equations of $k$ and $\varepsilon$ or $\omega$ are taken into account
({\tt igrake}=1) or not (0)\\
useful if and only if {\tt iturb} = 20, 21, 50 or 60, ({\tt gx, gy, gz})
$\ne$ (0,0,0) and the density is not uniform}

\motcle{igrhok}{i}{0 or 1}{0}{O}{L2}
{indicates if the term $\frac{2}{3}\grad \rho k$
is taken into account\\ ({\tt igrhok}=1) or not (0) in the velocity
equation\\
useful if and only if {\tt iturb} = 20, 21, 50 or 60.\\
This term may generate
non-physical velocities at the wall. When it is not explicitly taken into
account, it is implicitly included into the pressure.}

\motcle{ikecou}{i}{0 or 1}{0 or 1}{O}{L3}
{indicates if the coupling of the source terms of
$k$ and $\varepsilon$ or $k$ and $\omega$ is taken into account
({\tt ikecou}=1) or not (0)\\
if {\tt ikecou}=0 in $k-\varepsilon$ model, the term in $\varepsilon$ in the
equation of $k$ in made implicit\\
{\tt ikecou} is initialised to 0 if {\tt iturb} = 21 or 60,
and to 1 if {\tt iturb}= 20\\
{\tt ikecou}=1 is forbidden when using the v2f model
({\tt iturb}=50)\\
useful if and only if {\tt iturb} = 20, 21 or 60 ($k-\varepsilon$ and
$k-\omega$ models)}

\motcle{iclkep}{i}{0 or 1}{0}{O}{L3}
{indicates the clipping method used for $k$ and
$\varepsilon$, for the $k-\varepsilon$ and v2f models\\
\hspace*{1.3cm}= 0: clipping in absolute value\\
\hspace*{1.3cm}= 1: clipping from physical relations\\
useful if and only if {\tt iturb} = 20, 21 or 50 ($k-\varepsilon$ and
v2f models). The results obtained with the method corresponding to
{\tt iclkep}=1 showed in some cases a substantial sensitivity to the
values of the length scale {\tt almax}.\\
The option {\tt iclkep}=1 is therefore not recommended, and,
if chosen, must be used cautiously.}

\motcle{irccor}{i}{0 or 1}{0}{O}{L2}
{Activation of rotation/curvature correction for eddy viscosity turbulence models.\\
\hspace*{1.3cm}= 0: activated\\
\hspace*{1.3cm}= 1: not activated\\
useful if and only if {\tt iturb} = 20, 21, 50, 51, 60, 70 (eddy viscosity models)
}

\motcle{itycor}{i}{1 or 2}{1 or 2}{O}{L2}
{Type of rotation/curvature correction for eddy viscosity turbulence models:\\
\hspace*{1.3cm}= 1: Cazalbou correction (default when {\tt irccor}=1 and {\tt iturb}=20, 21 or 50, 51)\\
\hspace*{1.3cm}= 2: Spalart-Shur correction (default when {\tt irccor}=1 and {\tt iturb}=60 or 70)
}

\minititre{ $R_{ij}-\varepsilon$ (LRR and SSG)}

\motcle{iclptr}{i}{0 or 1}{0}{O}{L3}
{indicates if $R_{ij}$ is made partially implicit
({\tt iclptr}=1) or not (0) in the wall boundary conditions.\\
useful if and only if {\tt iturb} = 30 or 31 ($R_{ij}-\varepsilon$ model)}

\motcle{iclsyr}{i}{0 or 1}{0}{O}{L3}
{indicates if $R_{ij}$ is made partially implicit
({\tt iclsyr}=1) or not (0) in the symmetry boundary conditions.\\
useful if and only if {\tt iturb} = 30 or 31 ($R_{ij}-\varepsilon$ model)}

\motcle{idifre}{i}{0 or 1}{1}{O}{L3}
{complete ({\tt idifre=1}) or simplified (0)
taking into account of the diagonals of the diffusion tensors of $R_{ij}$
and $\varepsilon$, for the LLR model.\\
useful if and only if {\tt iturb} = 30 (LLR $R_{ij}-\varepsilon$ model)}

\motcle{igrari}{i}{0 or 1}{1}{O}{L1}
{indicates if the terms related to gravity are
taken into account ({\tt igrari}=1) or not (0) in the equations of
$R_{ij}-\varepsilon$. \\
useful if and only if {\tt iturb} = 30 or 31 and ({\tt gx, gy, gz}) $\ne$
(0,0,0) ($R_{ij}-\varepsilon$ model with gravity) and the density is not uniform}

\motcle{idirsm}{i}{0 or 1}{1}{O}{L3}
{model for the turbulent diffusion of $R_{ij}$ and $\varepsilon$ in second moment closure. Shir model (isotropic diffusion) if 0, Daly and Harlow model if 1, default value.}

\motcle{irijec}{i}{0 or 1}{0}{O}{L2}
{indicates if the wall echo terms in
$R_{ij}-\varepsilon$ LRR model are
taken into account ({\tt irijec}=1) or not (0).\\
useful if and only if {\tt iturb} = 30 ($R_{ij}-\varepsilon$ LRR).\\
It is not recommended to take these terms into account:
they have an influence only near the walls, their expression is hardly
justifiable according to some authors and, in the configurations
studied with \CS, they did not bring any improvement in the results.\\
In addition, their use induces an increase in the calculation
time.\\
The wall echo terms imply the calculation of the distance to the wall
for every cell in the domain. See {\tt icdpar} for potential restrictions
due to this.}

\motcle{irijnu}{i}{0 or 1}{0}{O}{L3}
{addition ({\tt irijnu}=1) or not (0) of a
turbulent viscosity in the matrix of the incremental system solved
for the velocity in $R_{ij}-\varepsilon$ models. The goal is to improve
the stability of the calculation. The usefulness of {\tt irijnu}=1 has
however not been clearly demonstrated.\\
Since the system is solved in incremental form, this extra turbulent
viscosity does not change the final solution for steady flows. However,
for unsteady flows, the parameter {\tt nswrsm} should be increased.\\
useful if and only if {\tt iturb} = 30 or 31 ($R_{ij}-\varepsilon$ model).}

\motcle{irijrb}{i}{0 or 1}{0}{O}{L3}
{reconstruction ({\tt irijrb}=1)
or not (0) of the boundary conditions at the walls for $R_{ij}$ and  $\varepsilon$.\\
useful if and only if {\tt iturb} = 30 or 31 ($R_{ij}-\varepsilon$ model)}


\minititre{$LES$}

\motcle{ivrtex}{i}{0 or 1}{0}{O}{L1}
{activates (=1) or not (=0) the generation of synthetic turbulence at the
different inlet boundaries with the LES model (generation of unsteady synthetic
eddies)\\
useful if {\tt iturb}=40, 41 or 42\\
this keyword requires the completion of the routine
\texttt{usvort}}

\motcle{isuivo}{i}{0 or 1}{isuite}{O}{L1}
{for the vortex method, indicates whether the synthetic vortices at the inlet
should be initialised (=0) or read from the restart file.\\
useful if {\tt iturb}=40, 41, 42 and {\tt ivrtex}=1}

\motcle{isuisy}{i}{0 or 1}{isuite}{O}{L1}
{Reading of the LES inflow module restart file.\\
\hspace*{1.3cm}= 0: not activated \\
\hspace*{1.3cm}= 1: activated\\
If {\tt isuisy}=1, synthetic fluctuations are not re-initialized in case of restart calculation.
useful if {\tt iturb}=40, 41 or 42
}

\motcle{idries}{i}{0 or 1}{0,1}{O}{L2}
{{\tt idries} activates (1) or not (0) the van
Driest wall-damping for the Smagorinsky constant (the Smagorinsky
constant is multiplied by the damping function
$1-e^{-y^+/{\tt cdries}}$, where $y^+$ designates the non-dimensional
distance to the nearest wall). The default value is 1 for the
Smagorinsky model and 0 for the dynamic model.\\
the van Driest wall-damping requires the knowledge of the distance to the
nearest wall for each cell in the domain. Refer to keyword {\tt icdpar}
for potential limitations\\
useful if and only if {\tt iturb} = 40 or 41}

\motcle{cdries}{r}{real number $>$ 0}{26}{O}{L3}
{{\tt cdries} is the constant appearing in the
van Driest damping function applied to the Smagorinsky constant:
 $1-e^{-y^+/{\tt cdries}}$\\
useful if and only if {\tt iturb} = 40 or 41}

\motcle{csmago}{r}{real number $>$ 0}{0.065}{O}{L2}
{{\tt csmago} is the Smagorinsky constant used in
the Smagorinsky model for LES\\
the sub-grid scale viscosity is calculated by
 $\displaystyle\mu_{sg}=\rho C_{smago}^2\bar{\Delta}^2\sqrt{2\bar{S}_{ij}\bar{S}_{ij}}$
where $\bar{\Delta}$ is the width of the filter and $\bar{S}_{ij}$ the filtered
strain rate\\
useful if and only if {\tt iturb} = 40}

\motcle{smagmx}{r}{real number $>$ 0}{10*csmago}{O}{L3}
{${\tt smagmx}^2$ is
the maximum allowed value for the variable $C$ appearing in the LES dynamic
model (the ``square'' comes from the fact that the
variable of the dynamic model corresponds to the square of the
constant of the Smagorinsky model). Any larger value yielded by the calculation
procedure of the dynamic model will be clipped to ${\tt smagmx}^2$\\
useful if and only if {\tt iturb} = 41}

\motcle{xlesfl}{r}{real number $>$ 0}{2}{O}{L3}
{{\tt xlesfl} is a constant used to define, for
each cell $\Omega_i$, the width of the (implicit) filter:\\
$\overline{\Delta}=xlesfl(ales*|\Omega_i|)^{bles}$\\
useful if and only if {\tt iturb} = 40 or 41}

\motcle{ales}{r}{real number $>$ 0}{1}{O}{L3}
{{\tt ales} is a constant used to define, for
each cell $\Omega_i$, the width of the (implicit) filter:\\
$\overline{\Delta}=xlesfl(ales*|\Omega_i|)^{bles}$\\
useful if and only if {\tt iturb} = 40 or 41}

\motcle{bles}{r}{real number $>$ 0}{1/3}{O}{L3}
{{\tt bles} is a constant used to define, for
each cell $\Omega_i$, the width of the (implicit) filter:\\
$\overline{\Delta}=xlesfl(ales*|\Omega_i|)^{bles}$\\
useful if and only if {\tt iturb} = 40 or 41}

\motcle{xlesfd}{r}{real number $>$ 0}{1.5}{O}{L3}
{{\tt xlesfd} is the constant used to define, for
each cell $\Omega_i$, the width of the explicit filter used in the framework of
the LES dynamic model:\\
$\widetilde{\overline{\Delta}}=xlesfd\overline{\Delta}$\\
useful if and only if {\tt iturb} = 41}



%==================================
\subsubsection{Time scheme}
%==================================

By default, the standard time scheme is a first-order.
A second-order scheme is activated automatically with LES modelling.
On the other hand, when ``specific physics'' (gas combustion, pulverised coal,
compressible module) are activated, the second-order scheme is not allowed.

In the current version, the second-order time scheme is not compatible
with the estimators ({\tt iescal}), the velocity-pressure coupling
({\tt ipucou}), the modelling of hydrostatic pressure ({\tt icalhy} and
{\tt iphydr}) and the time- or space-variable time step ({\tt idtvar}).

Also, in the case of a rotation periodicity, a proper second-order is not
ensured for the velocity, but calculations remain possible.

It is recommended to keep the default values of the variables listed
below. Hence, in standard cases, the user does not need to specify these
options.


\motcle{ischtp}{i}{1 or 2}{1 or 2}{O}{L2}
{{\tt ischtp} indicates the order of the
activated time scheme (this indicator allows the code to automatically complete
the other indicators related to the time scheme)\\
\hspace*{1.3cm}= 1: first-order \\
\hspace*{1.3cm}= 2: second-order \\
when {\tt ischtp}=2, the physical properties are by default not
second-order. It it possible to modify this by means of the
following indicators.\\
due to specific coupling between certain variables, the source terms in the
turbulence equations (except convection and diffusion) cannot be second order,
except with the $R_{ij}$ models (cf. keyword {\tt isto2t})\\
by default, {\tt ischtp} is initialised to 2 with the LES model and 1
otherwise\\
always useful}

\motcle{istmpf}{i}{0, 1 or 2}{0 or 1}{O}{L3}
{{\tt istmpf} specifies the time scheme activated
for the mass flow. The chosen value for {\tt istmpf} will automatically
determine the value given to the variable {\tt thetfl}\\
\hspace*{1.3cm}= 0: ``explicit'' first-order: the mass flow calculated
at the previous time step (``n'') is used in the convective terms of all
the equations (momentum, turbulence and scalars\\
\hspace*{1.3cm}= 1: ``standard'' first-order: the mass flow calculated
at the previous time step (``n'') is used in the convective terms of the
momentum equation, and the updated mass flow (time ``n+1'') is used in the
equations of turbulence and scalars\\
\hspace*{1.3cm}= 2: second-order: the mass flow used in the momentum equations
is extrapolated at ``n+{\tt thetfl}'' (=n+1/2) from the values at the two former time
steps (Adams Bashforth); the mass flow used in the equations for turbulence and
scalars is interpolated at time ``n+{\tt thetfl}'' (=n+1/2) from the values at the
former time step and at the newly calculated ``n+1'' time step.\\
by default, {\tt istmpf}=2 is used in the case of a second-order time
scheme (if {\tt ischtp}=2) and {\tt istmpf}=1 otherwise\\
always useful}

\motcle{isno2t}{i}{0, 1 or 2}{0 or 1}{O}{L3}
{{\tt isno2t} specifies the time scheme activated
for the source terms of the momentum equation, apart from convection and
diffusion (for instance: head loss, transposed gradient, ...).\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the terms which are linear
functions of the solved variable are implicit and the others are explicit\\
\hspace*{1.3cm}= 1: second-order: the terms of the form $S_i\phi$ which are
linear functions of the solved variable
$\phi$ are expressed as second-order terms by interpolation (according
to the formula
$(S_i\phi)^{n+\theta}=S_i^n[(1-\theta)\phi^n+\theta\phi^{n+1}]$, $\theta$
being given by the value of {\tt thetav} associated with the variable $\phi$)
; the other terms $S_e$ are expressed as second-order terms by
extrapolation (according to the formula
$(S_e)^{n+\theta}=[(1+\theta)S_e^n-\theta S_e^{n-1}]$, $\theta$ being
given by the value of {\tt thetsn}=0.5)\\
\hspace*{1.3cm}= 2: the linear terms $S_i\phi$ are treated in the same
way as when {\tt isno2t}=1;
the other terms $S_e$ are extrapolated according to the same formula
as when {\tt isno2t}=1, but with $\theta$={\tt thetsn}=1\\
by default, {\tt isno2t} is initialised to 1 (second-order) when
the selected time scheme is second-order ({\tt ischtp}=2), otherwise to 0.\\
always useful}

\motcle{isto2t}{i}{0, 1 or 2}{0}{O}{L3}
{{\tt isto2t} specifies the time scheme
activated for the source terms of the turbulence equations ({\em i.e.} related to $k$,
$R_{ij}$, $\varepsilon$, $\omega$, $\varphi$, $\overline{f}$), apart
from convection and diffusion.\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the terms which are linear
functions of the solved variable are implicit and the others are explicit\\
\hspace*{1.3cm}= 1: second-order: the terms of the form $S_i\phi$ which are
linear functions of the solved variable
$\phi$ are expressed as second-order terms by interpolation (according
to the formula
$(S_i\phi)^{n+\theta}=S_i^n[(1-\theta)\phi^n+\theta\phi^{n+1}]$, $\theta$
being given by the value of {\tt thetav} associated with the variable $\phi$);
the other terms $S_e$ are expressed as second-order terms by
extrapolation (according to the formula
$(S_e)^{n+\theta}=[(1+\theta)S_e^n-\theta S_e^{n-1}]$, $\theta$ being
given by the value of {\tt thetst}=0.5)\\
\hspace*{1.3cm}= 2: the linear terms $S_i\phi$ are treated in the same
way as when {\tt isto2t}=1;
the other terms $S_e$ are extrapolated according to the same formula
as when {\tt isto2t}=1, but with $\theta$={\tt thetst}=1\\
due to certain specific couplings between the turbulence equations,
{\tt isto2t} is allowed the value 1 or 2 only for the $R_{ij}$ models
({\tt iturb}=30 or 31); hence, it is always initialised to 0.\\
always useful}


\motcle{isso2t}{ia}{0, 1 or 2}{0 or 1}{O}{L3}
{for each scalar {\tt iscal}, {\tt isso2t(iscal)} specifies the time scheme activated
for the source terms of the equation for the scalar, apart from convection and
diffusion (for instance: variance production, user-specified terms, ...).\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the terms which are linear
functions of the solved variable are implicit and the others are explicit\\
\hspace*{1.3cm}= 1: second-order: the terms of the form $S_i\phi$ which are
linear functions of the solved variable
$\phi$ are expressed as second-order terms by interpolation (according
to the formula
$(S_i\phi)^{n+\theta}=S_i^n[(1-\theta)\phi^n+\theta\phi^{n+1}]$, $\theta$
being given by the value of {\tt thetav} associated with the variable $\phi$);
the other terms $S_e$ are expressed as second-order terms by
extrapolation (according to the formula
$(S_e)^{n+\theta}=[(1+\theta)S_e^n-\theta S_e^{n-1}]$, $\theta$ being
given by the value of {\tt thetss(iscal)}=0.5)\\
\hspace*{1.3cm}= 2: the linear terms $S_i\phi$ are treated in the same
way as when {\tt isso2t}=1;
the other terms $S_e$ are extrapolated according to the same formula
as when {\tt isso2t}=1, but with $\theta$={\tt thetss(iscal)}=1\\
by default, {\tt isso2t(iscal)} is initialised to 1 (second-order) when the selected
time scheme is second-order ({\tt ischtp}=2), otherwise to 0.\\
always useful}


\motcle{iroext}{i}{0, 1 or 2}{0}{O}{L3}
{{\tt iroext} specifies the time scheme activated
for the physical property $\phi$ ``density''.\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the value calculated at
the beginning of the current time step (from the
variables known at the end of the previous time step) is used \\
\hspace*{1.3cm}= 1: second-order: the physical property $\phi$ is
extrapolated according to the formula
$\phi^{n+\theta}=[(1+\theta)\phi^n-\theta \phi^{n-1}]$, $\theta$ being
given by the value of {\tt thetro}=0.5 \\
\hspace*{1.3cm}= 2: first-order: the physical property $\phi$ is
extrapolated at $n+1$ according to the
same formula as when {\tt iroext}=1 but with $\theta$={\tt thetro}=1\\
always useful}

\motcle{iviext}{i}{0, 1 or 2}{0}{O}{L3}
{{\tt iviext} specifies the time scheme activated
for the physical property $\phi$ ``total viscosity''
(molecular+turbulent or sub-grid viscosities).\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the value calculated at
the beginning of the current time step (from the
variables known at the end of the previous time step) is used \\
\hspace*{1.3cm}= 1: second-order: the physical property $\phi$ is
extrapolated according to the formula
$\phi^{n+\theta}=[(1+\theta)\phi^n-\theta \phi^{n-1}]$, $\theta$ being
given by the value of {\tt thetvi}=0.5 \\
\hspace*{1.3cm}= 2: first-order: the physical property $\phi$ is
extrapolated at $n+1$ according to the
same formula as when {\tt iviext}=1, but with $\theta$={\tt thetvi}=1\\
always useful}

\motcle{icpext}{i}{0, 1 or 2}{0}{O}{L3}
{{\tt icpext} specifies the time scheme activated
for the physical property $\phi$ ``specific heat''.\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the value calculated at
the beginning of the current time step (from the
variables known at the end of the previous time step) is used \\
\hspace*{1.3cm}= 1: second-order: the physical property $\phi$ is
extrapolated according to the formula
$\phi^{n+\theta}=[(1+\theta)\phi^n-\theta \phi^{n-1}]$, $\theta$ being
given by the value of {\tt thetcp}=0.5 \\
\hspace*{1.3cm}= 2: first-order: the physical property $\phi$ is
extrapolated at $n+1$ according to the
same formula as when {\tt icpext}=1, but with $\theta$={\tt thetcp}=1\\
always useful}

\motcle{ivsext}{ia}{0, 1 or 2}{0}{O}{L3}
{for each scalar {\tt iscal}, {\tt ivsext(iscal)} specifies the time scheme
activated for the physical property $\phi$ ``diffusivity''.\\
\hspace*{1.3cm}= 0: ``standard'' first-order: the value calculated at
the beginning of the current time step (from the
variables known at the end of the previous time step) is used \\
\hspace*{1.3cm}= 1: second-order: the physical property $\phi$ is
extrapolated according to the formula
$\phi^{n+\theta}=[(1+\theta)\phi^n-\theta \phi^{n-1}]$, $\theta$ being
given by the value of {\tt thetvs(iscal)}=0.5 \\
\hspace*{1.3cm}= 2: first-order: the physical property $\phi$ is
extrapolated at $n+1$ according to the
same formula as when {\tt ivsext}=1, but with $\theta$={\tt thetvs(iscal)}=1\\
always useful}

\motcle{thetav}{ra}{0 $\leqslant$ real $\leqslant$1}{1 or 0.5}{O}{L3}
{for each variable {\tt ivar}, {\tt thetav(ivar)} is the value of $\theta$ used to
express at the second-order the terms of convection, diffusion and the
source terms which are linear functions of the solved variable
(according to the formula
$\phi^{n+\theta}=(1-\theta)\phi^n+\theta\phi^{n+1}$). Generally,
only the values 1 and 0.5 are used. The user is not allowed to modify
this variable.\\
\hspace*{1.3cm}= 1: first-order \\
\hspace*{1.3cm}= 0.5: second-order \\
Concerning the pressure, the value of {\tt thetav} is always 1. Concerning
the other variables, the value {\tt thetav}=0.5 is used when the
second-order time scheme is activated by {\tt ischtp}=2 (standard value for
LES calculations), otherwise {\tt thetav} is set to 1.\\
always useful}

\motcle{thetfl}{r}{0 $\leqslant$ real $\leqslant$1}{0 or 0.5}{O}{L3}
{{\tt thetfl} is the value of $\theta$ used to
interpolate the convective fluxes of the variables when a second-order time
scheme has been activated for the mass flow (see {\tt istmpf})\\
generally, only the value 0.5 is used. The user is not allowed to
modify this variable.\\
\hspace*{1.3cm}= 0.0: ``explicit'' first-order (corresponds to
{\tt istmpf}=0 or 1)\\
\hspace*{1.3cm}= 0.5: second-order (corresponds to {\tt istmpf}=2). The mass
flux will be interpolated according to the formula
$Q^{n+\theta}=\frac{1}{2-\theta}Q^{n+1}+\frac{1-\theta}{2-\theta}Q^{n+1-\theta}$).\\
always useful}

\motcle{thetsn}{r}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{{\tt thetsn} is the value of $\theta$ used to
extrapolate the nonlinear explicit source terms $S_e$ of the momentum equation,
when the source term extrapolation has been activated (see {\tt isno2t}),
following the formula\\
$(S_e)^{n+\theta}=(1+\theta)S_e^n-\theta S_e^{n-1}$\\
the value
of $\theta$={\tt thetsn} is deduced from the value chosen for
{\tt isno2t}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to {\tt isno2t}=0) \\
\hspace*{1.3cm}= 0.5: second-order (used when {\tt isno2t}=1) \\
\hspace*{1.3cm}= 1: first-order (used when {\tt isno2t}=2) \\
always useful}

\motcle{thetst}{r}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{{\tt thetst} is the value of $\theta$ used to
extrapolate the nonlinear explicit source terms $S_e$ of the turbulence equations,
when the source term extrapolation has been activated (see {\tt isto2t}),
following the formula\\
$(S_e)^{n+\theta}=(1+\theta)S_e^n-\theta S_e^{n-1}$\\
the value
of $\theta$={\tt thetsn} is deduced from the value chosen for
{\tt isto2t}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to {\tt isto2t}=0) \\
\hspace*{1.3cm}= 0.5: second-order (used when {\tt isto2t}=1) \\
\hspace*{1.3cm}= 1: first-order (used when {\tt isto2t}=2) \\
always useful}

\motcle{thetss}{ra}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{for each scalar {\tt iscal}, {\tt thetss(iscal)} is the value of $\theta$ used to
extrapolate the nonlinear explicit source terms $S_e$ of the scalar equation,
when the source term extrapolation has been activated (see {\tt isso2t}),
following the formula\\
$(S_e)^{n+\theta}=(1+\theta)S_e^n-\theta S_e^{n-1}$\\
the value
of $\theta$={\tt thetss(iscal)} is deduced from the value chosen for
{\tt isso2t(iscal)}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to {\tt isso2t(iscal)}=0) \\
\hspace*{1.3cm}= 0.5: second-order (used when {\tt isso2t(iscal)}=1) \\
\hspace*{1.3cm}= 1: first-order (used when {\tt isso2t(iscal)}=2) \\
useful if {\tt nscal}$>$1}


\motcle{thetro}{r}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{{\tt thetro} is the value of $\theta$ used to
extrapolate the physical property $\phi$ ``density'' when the extrapolation has
been activated (see {\tt iroext}),according to the
formula $\phi^{n+\theta}=(1+\theta)\phi^n-\theta \phi^{n-1}$\\
the value of $\theta$={\tt thetro} is deduced from the value chosen for
{\tt iroext}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to
{\tt iroext}=0)\\
\hspace*{1.3cm}= 0.5: second-order (corresponds to {\tt iroext}=1) \\
\hspace*{1.3cm}= 1: first-order (corresponds to {\tt iroext}=2) \\
always useful}

\motcle{thetvi}{r}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{{\tt thetvi} is the value of $\theta$ used to
extrapolate the physical property $\phi$ ``total viscosity'' when the extrapolation has
been activated (see {\tt iviext}),according to the
formula $\phi^{n+\theta}=(1+\theta)\phi^n-\theta \phi^{n-1}$\\
the value of $\theta$={\tt thetvi} is deduced from the value chosen for
{\tt iviext}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to
{\tt iviext}=0)\\
\hspace*{1.3cm}= 0.5: second-order (corresponds to {\tt iviext}=1) \\
\hspace*{1.3cm}= 1: first-order (corresponds to {\tt iviext}=2) \\
always useful}

\motcle{thetcp}{r}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{{\tt thetcp} is the value of $\theta$ used to
extrapolate the physical property $\phi$ ``specific heat'' when the extrapolation has
been activated (see {\tt icpext}),according to the
formula $\phi^{n+\theta}=(1+\theta)\phi^n-\theta \phi^{n-1}$\\
the value of $\theta$={\tt thetcp} is deduced from the value chosen for
{\tt icpext}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to
{\tt icpext}=0)\\
\hspace*{1.3cm}= 0.5: second-order (corresponds to {\tt icpext}=1) \\
\hspace*{1.3cm}= 1: first-order (corresponds to {\tt icpext}=2) \\
always useful}

\motcle{thetvs}{ra}{0 $\leqslant$ real $\leqslant$1}{0, 0.5 or 1}{O}{L3}
{for each scalar {\tt iscal}, {\tt thetvs(iscal)} is the value of $\theta$ used to
extrapolate the physical property $\phi$ ``diffusivity'' when the extrapolation has
been activated (see {\tt ivsext}), according to the
formula $\phi^{n+\theta}=(1+\theta)\phi^n-\theta \phi^{n-1}$\\
the value of $\theta$={\tt thetvs(iscal)} is deduced from the value chosen for
{\tt ivsext(iscal)}. Generally, only the value 0.5 is used. The user is not
allowed to modify this variable.\\
\hspace*{1.3cm}= 0: first-order (unused, corresponds to
{\tt ivsext(iscal)}=0)\\
\hspace*{1.3cm}= 0.5: second-order (corresponds to {\tt ivsext(iscal)}=1) \\
\hspace*{1.3cm}= 1: first-order (corresponds to {\tt ivsext(iscal)}=2) \\
useful if {\tt nscal}$>$1}


%==================================
\subsubsection{Gradient reconstruction}
%==================================

\motcle{imrgra}{i}{0, 1, 2, 3, 4, 5, or 6}{0}{O}{L2}
{indicates the type of gradient reconstruction (one method for all the
variables)\\
\hspace*{1.3cm}= 0: iterative reconstruction of the non-orthogonalities\\
\hspace*{1.3cm}= 1: least squares method based on the first neighbour cells
(cells which share a face with the treated cell)\\
\hspace*{1.3cm}= 2: least squares method based on the extended neighbourhood
(cells which share a node with the treated cell)\\
\hspace*{1.3cm}= 3: least squares method based on a partial extended
neighbourhood (all first neighbours plus the extended neighbourhood cells that
are connected to a face where the non-orthogonality angle is larger than
parameter {\tt anomax})\\
\hspace*{1.3cm}= 4: iterative reconstruction with initialisation using the least
squares method (first neighbours)\\
\hspace*{1.3cm}= 5: iterative reconstruction with initialisation using the least
squares method based on an extended neighbourhood\\
\hspace*{1.3cm}= 6: iterative reconstruction with initialisation using the least
squares method based on a partial extended neighbourhood\\
if {\tt imrgra} fails due to probable mesh quality problems, it is usually effective
to use {\tt imrgra}=3. Moreover, {\tt imrgra}=3 is usually faster than
{\tt imrgra}=0 (but with less feedback on its use).\\
It should be noted that {\tt imrgra}=1, 2 or 3 automatically triggers a gradient
limitation procedure. See {\tt imligr}.\\
useful if and only if there is {\tt n} so that {\tt nswrgr(n)} $>$ 1.
Also, pressure gradients (or other gradients deriving from a potential)
always use an iterative reconstruction. To force a non-iterative
reconstruction for those gradients, a negative value of this keyword may be
used, in which case the method matching the absolute value of the keyword will
be used.}

\motcle{nswrgr}{ia}{positive integer}{100}{O}{L3}
{for each unknown {\tt ivar}, {\tt nswrgr(ivar)} $\leqslant$ 1 indicates that the
gradients are not reconstructed\\
\hspace*{1.3cm}if {\tt imrgra} = 0 or 4, {\tt nswrgr(ivar)} is the number of
iterations for the gradient reconstruction\\
\hspace*{1.3cm}if {\tt imrgra} = 1, 2 or 3, {\tt nswrgr(ivar)} $>$ 1 indicates that
the gradients are reconstructed (but the method is not iterative, so any value
larger than 1 for {\tt nswrgr} yields the same result)\\
useful for all the unknowns}

\motcle{epsrgr}{ra}{real number $>$ 0}{$10^{-5}$}{O}{L3}
{for each unknown {\tt ivar}, relative precision for the iterative gradient
reconstruction: {\tt epsrgr(ivar)}\\
useful for all the unknowns when {\tt imrgra} = 0 or 4}

\motcle{imligr}{ia}{-1, 0 or 1}{-1 or 1}{O}{L3}
{for each unknown {\tt ivar}, indicates the type of gradient limitation:
{\tt imligr(ivar)}\\
\hspace*{1.3cm}=-1: no limitation\\
\hspace*{1.3cm}= 0: based on the neighbours\\
\hspace*{1.3cm}= 1: superior order\\
for all the unknowns, {\tt imligr} is initialised to -1 if {\tt imrgra}=0 or 4
 and to 1 if \mbox{{\tt imrgra} = 1, 2 or 3}\\
useful for all the unknowns}

\motcle{climgr}{ra}{real number $>$ 0}{1.5}{O}{L3}
{for each unknown {\tt ivar}, factor of gradient limitation: {\tt climgr(ivar)}
(high value means little limitation)\\
useful for all the unknowns {\tt ivar} for which {\tt imligr(ivar)} $\ne$ -1}

\motcle{extrag}{ra}{0, 0.5 or 1}{0}{O}{L3}
{for the variable ``pressure'' {\tt ivar=ipr}, extrapolation coefficient
of the gradients at the boundaries. It affects only the Neumann conditions.
The only possible values of {\tt extrag(ipr)} are:\\
\hspace*{1.3cm}= 0: homogeneous Neumann calculated at first-order\\
\hspace*{1.3cm}= 0.5: improved homogeneous Neumann, calculated at
second-order in the case of an orthogonal mesh and at first-order otherwise\\
\hspace*{1.3cm}= 1: gradient extrapolation (gradient at the boundary face
equal to the gradient in the neighbour cell), calculated at
second-order in the case of an orthogonal mesh and at first-order otherwise\\
{\tt extrag} often allows to correct the non-physical velocities that
appear on horizontal walls when density is variable and there is gravity.
It is strongly advised to keep {\tt extrag}=0 for the variables apart from
pressure. See also {\tt iphydr}.\\
In practice, only the values 0 and 1 are allowed. The
value 0.5 is not allowed by default (but the lock can be overridden if
necessary, contact the development team).\\
always useful}

\motcle{anomax}{r}{0 $\leqslant$ real $\leqslant\pi/2$}{$\pi/4$}{O}{L3}
{limit non-orthogonality angle used to restrict the extended neighbourhood for
the gradient calculation with {\tt imrgra}=3.\\
{\tt anomax}=0 will yield the same result as {\tt imrgra}=2 (full extended
neighbourhood). {\tt anomax}=$\pi/2$ will yield the same result as
{\tt imrgra}=1
(first neighbours only)\footnote{Except for pathological cases where the
non-orthogonality angle of a face would be larger than $\pi/2$}\\
useful if and only if {\tt imrgra}=3}

%==================================
\subsubsection{Solution of the linear systems}
%==================================

See \doxygenfile{parameters.html}{the dedicated \texttt{Doxygen} documentation}
for most settings related to linear solver options.

\motcle{epsilo}{ra}{real number $>$ 0}{$10^{-8}$,$10^{-5}$}{O}{L3}
{for each unknown {\tt ivar}, relative precision for the solution of the linear
system. The default value is {\tt epsilo(ivar)=$10^{-8}$}. This value is set low
on purpose. When there are enough iterations on the reconstruction of the
right-hand side of the equation,
the value may be increased (by default, in case of second-order in time,
with {\tt nswrsm} = 5 or 10, {\tt epsilo} is increased to $10^{-5}$).\\
always useful}

%==================================
\subsubsection{Convective scheme}
%==================================

\motcleb{blencv}{ra}{0 $\leqslant$ real $\leqslant$ 1}{0 or 1}{O}{L1}
{for each unknown {\tt ivar} to calculate, {\tt blencv(ivar)} indicates the
 proportion of second-order convective scheme (0 corresponds to an
``upwind'' first-order scheme); in case of LES calculation, a
second-order scheme is recommended and activated by default ({\tt blencv=1})\\
useful for all the unknowns {\tt ivar} for which {\tt iconv(ivar)} = 1}

\motcle{ischcv}{ia}{0 or 1}{1}{O}{L2}
{for each unknown {\tt ivar} to calculate, {\tt ischcv(ivar)} indicates the type of second-order
convective scheme\\
\hspace*{1.3cm}= 0: Second Order Linear Upwind\\
\hspace*{1.3cm}= 1: Centered\\
useful for all the unknowns {\tt ivar} which are convected
({\tt iconv(ivar)}=1) and
for which a second-order scheme is used ({\tt blencv(ivar)} $>$ 0)}

\motcle{isstpc}{ia}{0 or 1}{0}{O}{L2}
{for each unknown {\tt ivar} to calculate, {\tt isstpc(ivar)}
indicates whether a ``slope test'' should
be used to switch from a second-order to an ``upwind'' convective
scheme under certain conditions, to ensure stability.\\
\hspace*{1.3cm}= 0: ``slope test'' activated for the considered unknown\\
\hspace*{1.3cm}= 1: ``slope test'' deactivated for the considered unknown\\
useful for all the unknowns {\tt ivar}  which are convected
({\tt iconv(ivar)}=1) and
for which a second-order scheme is used ({\tt blencv(ivar)} $>$ 0).\\
the use of the ``slope test'' stabilises the calculation but may bring
the order in space to decrease quickly.}

%==================================
\subsubsection{Pressure-continuity step}
%==================================

\motcle{iprco}{i}{0 or 1}{1}{O}{L3}
{indicates if the pressure-continuity step is taken into account (1) or
not (0)\\
always useful}

\motcle{arak}{ra}{0 $<$ real $\leqslant$ 1}{1}{O}{L3}
{{\tt arak} is the Arakawa coefficient before the
Rhie\& Chow filter\\
always useful}

\motcle{irevmc}{i}{0}{0}{O}{L3}
{method used to update the velocity after the pressure
correction:\\
\hspace*{0,5cm}- standard gradient of pressure increment
({\tt irevmc}=0)\\
always useful}

\motcle{iphydr}{i}{0 or 1 or 2}{0}{O}{L2}
{method for taking into account the balance between the pressure gradient and
the source terms (gravity and head losses): by extension it will be
referenced as ``taking into account of the hydrostatic pressure''\\
\hspace*{1.3cm}= 0: standard algorithm\\
\hspace*{1.3cm}= 1: improved algorithm\\
always useful\\
When the density effects are important, the choice of
{\tt iphydr}=1 allows to improve the interpolation of the pressure and correct the
non-physical velocities which may appear in highly
stratified areas or near horizontal walls (thus
avoiding the use of {\tt extrag} if the non-physical velocities are due only to
gravity effects).\\
The improved algorithm also allows eradicating the velocity oscillations
which tend to appear at the frontiers of areas with high head losses.\\
In the case of a stratified flow, the calculation cost is higher when the
improved algorithm is used (about 30\% depending on the case) because
the hydrostatic pressure must be recalculated at the outlet boundary
conditions: see {\tt icalhy}.\\
On meshes of insufficient quality, in order to
improve the convergence, it may be useful to increase the number of
iterations for the reconstruction of the pressure right-hand side,
{\em i.e.} \mbox{\tt nswrsm(ipr)}.\\
If head losses are present just along an outlet boundary, it is necessary to
specify {\tt icalhy}=0 in order to deactivate the recalculation of the hydrostatic
pressure at the boundary, which may otherwise cause instabilities.}

\motcle{icalhy}{i}{0 or 1}{0 or 1}{O}{L3}
{activates the calculation of hydrostatic pressure boundary conditions at outlet
boundaries\\
\hspace*{1.3cm}= 0: no calculation of the hydrostatic pressure at the outlet boundary\\
\hspace*{1.3cm}= 1: calculation of the hydrostatic pressure at the outlet boundary\\
always useful\\
This option is automatically specified depending on the
choice of {\tt iphydr} and the value of gravity
({\tt icalhy}=1 if {\tt iphydr}=1 and gravity is different from 0; otherwise
{\tt icalhy}=0). The activation of this option generates an additional
calculation cost (about 30\% depending on the case).\\
If head losses are present just along an outlet boundary, it is necessary to
specify {\tt icalhy}=0 in order to deactivate the recalculation of the hydrostatic
pressure at the boundary, which may otherwise cause instabilities}

\motcle{epsdp}{r}{real number $>$ 0}{$10^{-12}$}{O}{L3}
{Parameter of diagonal pressure strengthening
}

\motcle{iporos}{i}{0 or 1}{0}{O}{L2}
{indicates if the porosity formulation is taken into account\\
\hspace*{1.3cm}= 0: standard algorithm (without porosity)\\
\hspace*{1.3cm}= 1: porosity taken into account\\
useful when head losses are taken into account
}

%==================================
\subsubsection{Error estimators for Navier-Stokes}
%==================================

There are currently {\tt nestmx\index{nestmx}}=4 types of local estimators
provided at every time step, with two possible definitions for
each\footnote{Choice made by the user}. These scalars indicate the areas
(cells) in which some error types may be important. They are
stored in the array {\tt propce} containing the properties at the cells (see
{\tt iestim\index{iestim}}). For each estimator, the code writes the minimum and
maximum values in the listing and generates post-processing outputs along with
the other variables.

The additional memory cost is about one real number per cell and per
estimator. The additional calculation cost is variable. For instance, on a
simple test case, the total estimator {\tt iestot} generates an additional cost
of 15 to 20 $\%$ on the CPU time\footnote{Indeed, all the first-order in
space differential terms have to be recalculated at the time $t^{\,n+1}$};
the cost of the three others may be neglected. If the user wants to
avoid the calculation of the estimators during the computation, it is
possible to run a calculation without estimators first, and then activate them on
a restart of one or two time steps.

It is recommended to use the estimators only for visual and qualitative
analysis. Also, their use is compatible neither with a second-order time scheme
nor with a calculation with a frozen velocity field.

{\tt \bf iest = iespre\index{iespre}: prediction} (default name: EsPre).
After the velocity prediction step (yielding $\vect{\widetilde{u}}$), the
estimator $\eta^{\,pred}_{\,i,k}(\vect{\widetilde{u}})$, local variable calculated
at every cell $\Omega_i$, is created from $\vect{\mathcal
R}^{\,pred}(\vect{\widetilde{u}})$, which represents the residual of the equation
solved during this step:
\begin{equation*}
\begin{array}{r c l}
\vect{\mathcal{R}}^{\,pred}(\vect{\widetilde{u}})&= & \rho^n
    \dfrac{\vect{\widetilde{u}}-\vect{u}^n}{\Delta t}
  + \gradt \left(\vect{\widetilde{u}} \right) \cdot \left(\rho  \vect{u}\right)^n
              - \divv \left((\mu+\mu_t)^n \gradt(\vect{\widetilde{u}}) \right)
              + \grad(P^n)     \\
              &- &\text{rest of the right-hand side}
                        (\vect{u}^n, P^n, \text{other variables}^n)
\end{array}
\end{equation*}

By definition:
$$ \eta^{\,pred}_{\,i,k}(\vect{\widetilde{u}})= {|\Omega_i|}^{\,(k-2)/2}\ ||\vect{\mathcal R}^{\,pred}(\vect{\widetilde{u}})||
_{{\mathbb{L}}^{2}(\Omega_i)}$$
%
\begin{itemize}
\item The first family, $k=1$, suppresses the
volume $|\Omega_i|$ which intrinsically appears with the norm
${{\mathbb{L}}^{2}(\Omega_i)}$.
\item The second family, $k=2$, exactly represents the norm
${{\mathbb{L}}^{2}(\Omega_i)}$. The size of the cell therefore
appears in its calculation and induces a weighting effect.
\end{itemize}
$ \eta^{\,pred}_{\,i,k}(\vect{\widetilde{u}})$  is ideally equal to zero when the
reconstruction methods are perfect and the associated system is
solved exactly.

{\tt \bf iest = iesder\index{iesder}: drift}  (default name: EsDer).
The estimator $\eta^{\,der}_{\,i,k}(\vect{u}^{\,n+1})$ is based on the
following quantity (intrinsic to the code):
\begin{equation}
\begin{array}{lll}
 \eta^{der}_{i,k}(\vect{u}^{n+1})
&=& {|\Omega_i|}^{\,(k-2)/2}
||\divs \left(\text{corrected mass flow after the pressure step}\right)
                                              -\ \Gamma||_{{L}^{2}(\Omega_i)} \\
&=& {|\Omega_i|}^{\,(1-k)/2}
|div (\text{corrected mass flow after the pressure step})-\ \Gamma|
\end{array}
\end{equation}
Ideally, it is equal to zero when the Poisson equation related to the pressure is
solved exactly.

{\tt \bf iest = iescor\index{iescor}: correction}  (default name: EsCor).
The estimator $ \eta^{\,corr}_{\,i,k}(\vect{u}^{\,n+1})$ comes directly
from the mass flow calculated with the updated velocity field:
\begin{eqnarray*}
            \eta^{\,corr}_{\,i,k}(\vect{u}^{\,n+1})=
|\Omega_i|^{\,\delta_{\,2,k}}\ |div (\rho^n \vect{u}^{n+1}) -\ \Gamma|
\end{eqnarray*}
The velocities $\vect{u}^{n+1}$ are taken at the cell centers,
the divergence is calculated after projection on the faces.\\
            $ \,\delta_{\,2,k}$ represents the Kronecker symbol.\\
\hspace*{0.5cm}$\bullet$ The first family, $k=1$, is the absolute raw
value of the divergence of the mass flow minus the mass source term.\\
\hspace*{0.5cm}$\bullet$ The second family, $k=2$, represents a physical
property and allows to evaluate the difference in $kg.s^{\,-1}$.\\
Ideally, it is equal to zero when the Poisson equation is solved exactly and
the projection from the mass flux at the faces to the velocity at the cell
centers is made in a set of  functions with null divergence.

{\tt \bf iest = iestot\index{iestot}: total} (default name: EsTot).
The estimator $ \eta^{tot}_{\,i,k}(\vect{u}^{n+1})$, local variable
calculated at every cell $\Omega_i$, is based on the quantity
$\vect{\mathcal R}^{tot}(\vect{u}^{\,n+1})$, which represents the
residual of the equation using the updated values of
$\vect{u}$ and $P$:
\begin{equation*}
\begin{array}{@{}r@{\,} c@{\,} l}
\vect{\mathcal{R}}^{tot}({\vect{u}^{n+1}})&= & \rho^n
    \dfrac{{\vect{u}^{n+1}}-\vect{u}^n}{\Delta t}
  + \gradt \left({\vect{u}^{n+1}} \right) \cdot {\left(\rho  \vect{u}\right)}^{n+1}
              - \divv \left((\mu+\mu_t)^n \gradt({\vect{u}^{n+1}}) \right)
              + \grad({P^{n+1}})     \\
              &- &\text{rest of the right-hand side}
                        ({\vect{u}^{n+1}}, {P^{n+1}}, \text{other variables}^n)
\end{array}
\end{equation*}
%
By definition:
$$ \eta^{tot}_{i,k}(\vect{u}^{n+1})= {|\Omega_i|}^{\,(k-2)/2}\ ||\vect{\mathcal R}^{tot}(\vect{u}^{\,n+1})||
_{\mathbb{L}^{2}(\Omega_i)}$$

The mass flux in the convective term is recalculated from $\vect{u}^{n+1}$
expressed at the cell centres (and not taken from the updated mass flow at the
faces).\\

As for the prediction estimator:
\begin{itemize}
\item The first family, $k=1$, suppresses the
volume $|\Omega_i|$ which intrinsicly appears  with the norm
${\mathbb{L}^{2}(\Omega_i)}$.
\item The second family, $k=2$, exactly represents the norm
${\mathbb{L}^{2}(\Omega_i)}$. The size of the cell therefore
appears in its calculation and induces a weighting effect.
\end{itemize}

The estimators are evaluated depending on the values of {\tt iescal}.


\motcleb{iescal}{ia}{0, 1 or 2}{0}{O}{L1}
{{\tt iescal(iest)} indicates the calculation mode
for the error estimator {\tt iest} ({\tt iespre}, {\tt iesder}, {\tt iescor} or
{\tt iestot}), for
the Navier-Stokes equation:\\
 {\tt iescal} = 0: estimator not calculated, \\
 {\tt iescal} = 1: the estimator $ \eta^{*}_{i,1}$ is calculated,
                   without contribution of the volume, \\
 {\tt iescal} = 2: the estimator $ \eta^{*}_{i,2}$ is calculated,
                   with contribution of the volume ("norm $L^2$"),
                   except for {\tt iescor}, for which
                   $|\Omega_i|\ \eta^{corr}_{i,1}\ $
                   is calculated.

The names of the estimators appearing in the listing and the post-processing are
made up of the default name (given before), followed by the value of
{\tt iescal}. For
instance, EsPre2 is the estimator {\tt iespre} calculated with {\tt iescal}=2.\\
always useful}


%==================================
\subsubsection{Calculation of the distance to the wall}
%==================================

\motcle{icdpar}{i}{-1, 1, -2 or 2}{-1}{O}{L2}
{specifies the method used to calculate the distance to the wall $y$ and the
non-dimensional distance $y^+$ for all the
cells of the calculation domain (when necessary):\\
\hspace*{1.3cm}= 1: standard algorithm (based on a Poisson equation for $y$ and
convection equation for $y^+$),
with reading of the distance to the wall from the restart file
if possible\\
\hspace*{1.3cm}=-1: standard algorithm (based on a Poisson equation for $y$ and
convection equation for $y^+$),
with systematic recalculation of the distance to the wall in case of
calculation restart\\
\hspace*{1.3cm}= 2: former algorithm (based on geometrical
considerations),
with reading of the distance to the wall from the restart file
if possible\\
\hspace*{1.3cm}=-2: former algorithm (based on geometrical
considerations) with systematic recalculation of the distance to the
wall in case of calculation restart\\
In case of restart calculation, if the position of the walls haven't changed,
reading the distance to the wall from the restart file can save a fair amount of
CPU time.\\
Useful in $R_{ij}-\varepsilon$ model with wall echo ({\tt iturb}=30 and
{\tt irijec}=1), in LES with van Driest damping ({\tt iturb}=40 and
{\tt idries}=1) and in $k-\omega$ SST ({\tt iturb}=60). \\
By default, {\tt icdpar} is initialised to -1, in case there has been a change in the
definition of the boundary conditions between two computations (change in the
number or the positions of the walls). Yet, with the $k-\omega$ SST model, the
distance to the wall is needed to calculate the turbulent viscosity, which is
done before the calculation of the distance to the wall. Hence, when this model
is used (and only in that case), {\tt icdpar} is set to 1 by default, to ensure total
continuity of the calculation at restart.\\
{\bf As a consequence, with the \boldmath$k-\omega$\unboldmath\ SST model, if
the number and positions of the walls are changed at a calculation restart, it
is mandatory for the user to set {\tt icdpar} explicitly to -1}, otherwise the
distance to the wall used will not correspond to the actual position of the
walls.\\
The former algorithm is not compatible with parallelism nor periodicity. Also,
whatever the value chosen for {\tt icdpar}, the calculation of the distance to the
wall is made at the most once for all a the beginning of the calculation; it is
therefore not compatible with moving walls. Please contact the development team
if you need to override this limitation.}

The following options are related to {\tt icdpar} $\neq$\ 0. The options of
level 2 are described first. Some options are used only in the case of
the calculation of the non-dimensional distance to the wall $y^+$ (LES model with
van Driest damping). Most of the following keywords are simple copies of the
keywords for the numerical options of the general equations, with a potentially
specific value in the case of the calculation of the distance to the wall.\\

\motcle{iwarny}{i}{integer}{0}{O}{L2}
{specifies the level of the output writing concerning the calculation of the
distance to the wall with {\tt icdpar} $\neq$\ 0. The higher the value, the more
detailed the outputs\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{ntcmxy}{i}{positive integer}{1000}{O}{L2}
{number of pseudo-time iterations for the calculation of the non-dimensional
distance to the wall $y^+$\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}

\motcle{nitmay}{i}{integer  $>$ 0}{10000}{O}{L3}
{maximum number of iterations for the solution of the linear systems\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{nswrsy}{i}{positive integer}{1}{O}{L3}
{number of iterations for the reconstruction of the right-hand sides:
corresponds to {\tt nswrsm}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{nswrgy}{i}{positive integer}{100}{O}{L3}
{number of iterations for the gradient reconstruction: corresponds to {\tt nswrgr}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{imligy}{i}{-1, 0 or 1}{-1 or 1}{O}{L3}
{type of gradient limitation: corresponds to {\tt imligr}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{ircfly}{i}{0 or 1}{1}{O}{L3}
{indicates the reconstruction of the convective and diffusive fluxes at
the faces: corresponds to {\tt ircflu}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{ischcy}{i}{0 or 1}{1}{O}{L3}
{indicates type of second-order convective scheme: corresponds to {\tt ischcv}\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}

\motcle{isstpy}{i}{0 or 1}{0}{O}{L3}
{indicates if a ``slope test'' should be used for a second-order convective
scheme: corresponds to {\tt isstpc}\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}

\motcle{imgrpy}{i}{0 or 1}{0}{O}{L3}
{indicates whether the algebraic
multi-grid method should be used ({\tt imgr(ivar)}=1) or not (0): corresponds
to {\tt imgr}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{blency}{r}{0 $\leqslant$ real $\leqslant$ 1}{0}{O}{L3}
{proportion of second-order convective scheme: corresponds to {\tt blencv}\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}

\motcle{epsily}{r}{real number $>$ 0}{$10^{-8}$}{O}{L3}
{relative precision for the solution of the linear systems:
corresponds to {\tt epsilo}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{epsrgy}{r}{real number $>$ 0}{$10^{-5}$}{O}{L3}
{relative precision for the iterative gradient reconstruction:
corresponds to {\tt epsrgr}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{epsrsy}{r}{real number $>$ 0}{$10^{-5}$}{O}{L3}
{relative precision for the right-hand side reconstruction:
corresponds to {\tt epsrsm}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{climgy}{r}{real number $>$ 0}{1.5}{O}{L3}
{limitation factor of the gradients: corresponds to {\tt climgr}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{extray}{r}{0, 0.5 or 1}{0}{O}{L3}
{extrapolation coefficient of the gradients at the boundaries:
corresponds to {\tt extrag}\\
useful when {\tt icdpar} $\neq$\ 0}

\motcle{coumxy}{r}{strictly positive real number}{5000}{O}{L3}
{Target Courant number for the calculation of the non-dimensional distance
to the wall\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}

\motcle{epscvy}{r}{strictly positive real number}{$10^{-8}$}{O}{L3}
{relative precision for the convergence of the pseudo-transient regime
for the calculation of the non-dimensional distance to the wall\\
useful when {\tt icdpar} $\neq$\ 0  for the calculation of $y^+$}

\motcle{yplmxy}{r}{real number}{200}{O}{L3}
{value of the non-dimensional distance to the wall above which the
calculation of the distance is not necessary (for the damping)\\
useful when {\tt icdpar} $\neq$\ 0 for the calculation of $y^+$}


%==================================
\subsubsection{Others}
%==================================

\motcleb{iccvfg}{i}{0 or 1}{0}{O}{L1}
{indicates whether the dynamic field should be frozen (1) or not (0)\\
in such a case, the values of velocity,
pressure and the variables related to the potential turbulence model
($k$, $R_{ij}$, $\varepsilon$, $\varphi$, $\bar{f}$, $\omega$, turbulent viscosity) are kept
constant over time and only the equations for the scalars are solved\\
also, if {\tt iccvfg}=1, the physical properties modified in \texttt{usphyv} will keep
being updated. Beware of non-consistencies if these properties would normally
affect the dynamic field (modification of density for instance)\\
useful if and only if {\tt nscal} $>$ 0 and the calculation is a restart}

\motcleb{ivelco}{i}{0 or 1}{1}{O}{L1}
{indicates the algorithm for the velocity components coupling\\
\hspace*{1.3cm}= 0: segregated (deprecated)\\
\hspace*{1.3cm}= 1: coupled (default)\\
always useful
}

\motcleb{ipucou}{i}{0 or 1}{0}{O}{L1}
{indicates the algorithm for velocity/pressure coupling\\
\hspace*{1.3cm}= 0: standard algorithm\\
\hspace*{1.3cm}= 1: reinforced coupling in case calculation with long
time steps\\
always useful (it is seldom advised, but it can prove very useful, for instance,
in case of flows with weak convection effects and highly variable viscosity)}

\motcleb{nterup}{i}{real number $>$ 0}{1}{O}{L2}
{number of iterations on the pressure-velocity coupling in the Navier-Stokes equations (for the PISO algorithm).
useful for unsteady algorithm
}

\motcleb{epsup}{r}{real number $>$ 0}{$10^{-5}$}{O}{L2}
{relative precision for the convergence test of the iterative process on
pressure-velocity coupling (PISO).
useful for unsteady algorithm
}

\motcleb{isuit1}{i}{0 or 1}{0}{O}{L1}
{for the  1D wall thermal module, activation (1) or not(0) of the reading
of the mesh and of the wall temperature from the {\tt ficmt1} restart file\\
useful if {\tt nfpt1d}$>$0.}

\motcle{imvisf}{i}{0 or 1}{0}{O}{L3}
{indicates the interpolation method used to project variables from the cell
centers to the faces\\
\hspace*{1.3cm}= 0: linear\\
\hspace*{1.3cm}= 1: harmonic\\
always useful}

\motcle{ircflu}{ia}{0 or 1}{1}{O}{L2}
{for each unknown {\tt ivar}, {\tt ircflu(ivar)} indicates whether the convective
and diffusive fluxes at the faces should be reconstructed: \\
\hspace*{1.3cm}= 0: no reconstruction\\
\hspace*{1.3cm}= 1: reconstruction\\
deactivating the reconstruction of the fluxes can have a stabilising effect on
the calculation. It is sometimes useful with the $k-\varepsilon$ model, if the
mesh is strongly non-orthogonal in the near-wall region, where the gradients of
$k$ and $\varepsilon$ are strong. In such a case, setting {\tt ircflu(ik)}=0
and {\tt ircflu(iep)}=0 will probably help (switching to a first order
convective scheme, {\tt blencv=0}, for $k$ and $\varepsilon$ might also help in
that case)\\
always useful}

\motcle{nswrsm}{ia}{positive integer}{1, 2, 5 or 10}{O}{L3}
{for each unknown {\tt ivar}, {\tt nswrsm(ivar)} indicates the number of iterations for the
reconstruction of the right-hand sides of the equations\\
with a first-order scheme in time
(standard case), the default values are 2 for pressure and 1 for the
other variables. With a second-order scheme in time ({\tt ischtp}=2) or LES, the
default values are 5 for pressure and 10 for the other variables.\\
useful for all the unknowns}

\motcle{epsrsm}{ra}{real number $>$ 0}{$10^{-8}$,$10^{-5}$}{O}{L3}
{for each unknown {\tt ivar}, relative precision on the reconstruction of the
right hand-side. The default value is {\tt epsrsm(ivar)}=$10^{-8}$. This value is set low
on purpose. When there are not enough iterations on the reconstruction of the
right-hand side of the equation,
the value may be increased (by default, in case of second-order in time,
with {\tt nswrsm} = 5 or 10, {\tt epsrsm} is increased to $10^{-5}$).\\
always useful}


%====================================================================================
\subsection{Numerical, physical and modelling parameters}
%=============================================================================
\subsubsection{Numeric parameters}
%================================

These parameters correspond to numeric reference values in the code.
They can be used but shall not be modified (they are defined as \texttt{parameter}).

\motcle{zero}{r}{0}{0}{O}{L3}
{Parameter containing the value 0}

\motcle{epzero}{r}{$10^{-12}$}{$10^{-12}$}{O}{L3}
{``Small'' real parameter, used for the comparisons of real numbers (absolute
value of the difference lower than {\tt epzero})}

\motcle{pi}{r}{3.141592653589793}{3.141592653589793}{O}{L3}
{Parameter containing an approximate value of $\pi$}

\motcle{grand}{r}{$10^{12}$}{$10^{12}$}{O}{L3}
{``Large'' real parameter, generally used by default as a non physical value for
the initialisations of variables which have to be modified by the user}

\motcle{rinfin}{r}{$10^{30}$}{$10^{30}$}{O}{L3}
{Real parameter used to represent ``infinity''}

%==================================
\subsubsection{Physical parameters}
%==================================
These parameters correspond to physical reference values in the code.
They can be used but shall not be modified (they are defined as {\tt parameter}).

\motcle{tkelvi}{r}{273.15}{273.15}{O}{L3}
{Temperature in Kelvin corresponding to 0 degrees Celsius.}

\motcle{tkelvn}{r}{-273.15}{-273.15}{O}{L3}
{Temperature in degrees Celsius corresponding to 0 Kelvin.}

\motcle{\footnotesize cs\_physical\_constants\_r}{~~~~~~~~~~~~r}{~~~~~~8.31446}{8.31446}{O}{L3}
{Perfect gas constant in $J/mol/K$}

\motcle{trefth}{r}{25 + tkelvi}{25 + tkelvi}{O}{L3}
{Reference temperature for the specific physics, in $K$}

\motcle{prefth}{r}{101325}{101325}{O}{L3}
{Reference pressure for the specific physics, in $Pa$}

\motcle{volmol}{r}{$22.41.10^{-3}$}{$22.41.10^{-3}$}{O}{L3}
{Molar volume under normal pressure and temperature conditions (1 atmosphere,
0\degresC) in $m^{-3}$}

\motcle{stephn}{r}{$5.6703.10^{-8}$}{$5.6703.10^{-8}$}{O}{L3}
{Stephan's constant for the radiative module $\sigma$ in $W.m^{-2}.K^{-4}$}

\motcle{permvi}{r}{$1.2566.10^{-6}$}{$1.2566.10^{-6}$}{O}{L3}
{Vacuum magnetic permeability $\mu_0$ (=$4\pi.10^{-7}$) in $kg.m.A^{-2}.s^{-2}$}

\motcle{epszer}{r}{$8.854.10^{-12}$}{$8.854.10^{-12}$}{O}{L3}
{Vacuum permittivity $\varepsilon_0$ in $F.m^{-1}$}


%==================================
\subsubsection{Physical variables}
%==================================

\motcleb{gx,gy,gz}{r}{3 real numbers}{0,0,0}{O}{L1}
{gravity components\\
always useful }

\motcleb{irovar}{ia}{0 or 1}{\tt -1}{C}{L1}
{{\tt irovar}=0 indicates that the density is
constant. Its value is the reference density {\tt ro0}.\\
{\tt irovar}=1 indicates that the density is variable: its variation
law must be given in the user subroutine \texttt{usphyv}\\
negative value: not initialised\\
always useful}

\motcleb{ivivar}{ia}{0 or 1}{\tt -1}{C}{L1}
{{\tt ivivar}=0 indicates that the molecular
dynamic viscosity is constant. Its value is the reference molecular
dynamic viscosity {\tt viscl0}.\\
{\tt ivivar}=1 indicates that the molecular dynamic viscosity is
variable: its variation law must be given in the user subroutine
\texttt{usphyv}\\
negative value: not initialised\\
always useful}

\motcleb{ro0}{ra}{real number $\geqslant$ 0}{\tt -grand*10}{C}{L1}
{{\tt ro0} is the reference density\\
negative value: not initialised\\
its value is not used in gas or coal combustion modelling (it
will be calculated following the perfect gas law, with $P0$ and $T0$). With the
compressible module, it is also not used by the code, but it may be (and often
is) referenced by the user in user subroutines; it is therefore better to
specify its value.\\
always useful otherwise, even if a law defining the density is given by
the user subroutine \texttt{usphyv} or \texttt{uselph}\\
indeed, except with the
compressible module, \CS does not
use the total pressure $P$ when solving the Navier-Stokes equation, but a
reduced pressure \\
$P^*=P-\rho_0\vect{g}.(\vect{x}-\vect{x}_0)+P^*_0-P_0$\\
where
$\vect{x_0}$ is a reference point (see {\tt xyzp0}) and $P^*_0$ and $P_0$ are
reference values (see {\tt pred0} and {\tt p0}). Hence, the term
$-\grad{P}+\rho\vect{g}$ in the equation is treated as
$-\grad{P^*}+(\rho-\rho_0)\vect{g}$. The closer {\tt ro0} is to the value of $\rho$,
the more $P^*$ will tend to represent only the dynamic part of the pressure and
the faster and more precise its solution will be. Whatever the value of {\tt ro0},
both $P$ and $P^*$ appear in the listing and the post-processing outputs.\\
with the compressible module, the calculation is made directly on the total
pressure}

\motcleb{viscl0}{ra}{real number $>$ 0}{\tt -grand*10}{C}{L1}
{ {\tt viscl0} is the reference molecular dynamic
viscosity\\
negative value: not initialised\\
always useful, it is the used value unless the user specifies the
viscosity in the \texttt{usphyv}} subroutine

\motcleb{srrom}{r}{$0 \leqslant \text{real number} < 1$}{\tt -grand or 0}{c or O}{L1}
{With gas combustion, pulverised coal or the electric module, {\tt srrom}
 is the sub-relaxation coefficient for the density, following the formula:\\
$\rho^{n+1}$\,=\,srrom\,$\rho^n$+(1-srrom)\,$\rho^{n+1}$\\
hence, with a zero value, there is no sub-relaxation.
With combustion and pulverised coal, {\tt srrom} is initialised to {\tt -grand}
and the user must specify a proper value through the Interface or the
initialisation subroutines (\texttt{cs\_user\_combustion}). With the electric module, {\tt srrom} is initialised in to 0
and may be modified by the user in \texttt{useli1}.\\
With gas combustion, pulverised coal or electric arcs, {\tt srrom} is
automatically used after the second time-step. With the Joule effect module,
the user decides whether or not it will be used in \texttt{uselph}
from the coding law giving the density.}\\
always useful with gas combustion, pulverized coal or the electric module.

\motcleb{p0}{ra}{real number}{$1.013e-5$}{O}{L1}
{{\tt p0} is the reference pressure for the total
pressure\\
except with the compressible module, the total pressure $P$ is evaluated
from the reduced pressure $P^*$ so that $P$
is equal to {\tt p0} at the reference position $\vect{x}_0$ (given by {\tt xyzp0})\\
with the compressible module, the total pressure is solved directly\\
always useful}

\motcle{pred0}{ra}{real number}{0}{O}{L3}
{{\tt pred0} is the reference value for the reduced
pressure $P^*$ (see {\tt ro0})\\
it is especially used to initialise the reduced pressure and as a reference
value for the outlet boundary conditions\\
for an optimised precision in the resolution of $P^*$, it is better to keep {\tt pred0}
to 0\\
with the compressible module, the ``pressure'' variable appearing in the
equations directly represents the total pressure. It is therefore initialised
to {\tt p0} and not {\tt pred0} (see {\tt ro0})\\
always useful, except with the compressible module}

\motcleb{xyzp0}{ra}{3 real numbers}{0,0,0}{O}{L1}
{{\tt xyzp0(ii)} is the {\tt ii} coordinate
(1$\leqslant$II$\leqslant$3) of the reference point $\vect{x}_0$ for the
total pressure\\
when there are no Dirichlet conditions for the pressure (closed domain), {\tt xyzp0}
does not need to be specified (unless the total pressure has a clear physical
meaning in the configuration treated)\\
when Dirichlet conditions on the pressure are specified but only through standard
outlet conditions (as it is in most configurations),
{\tt xyzp0} does not need to be specified by the user, since it will be set to the
coordinates of the reference outlet face ({\em i.e.} the code will automatically
select a
reference outlet boundary face and set {\tt xyzp0} so that $P$ equals {\tt p0} at this
face). Nonetheless, if {\tt xyzp0} is specified by the user, the calculation will remain
correct\\
when direct Dirichlet conditions are specified by the user (specific value set
on specific boundary faces), it is better to specify the corresponding reference
point ({\em i.e.} specify where the total pressure is {\tt p0}). This way, the
boundary conditions for the reduced pressure will be close to {\tt pred0}, ensuring an
optimal precision in the resolution. If {\tt xyzp0} is not specified, the reduced
pressure will be shifted, but the calculations will remain correct.\\
with the compressible module, the ``pressure'' variable appearing in the
equations directly represents the total pressure. {\tt xyzp0} is therefore not used.\\
always useful, except with the compressible module}

\motcleb{t0}{ra}{real number}{0}{O}{L1}
{{\tt t0} is the reference temperature \\
useful for the specific physics gas or coal combustion (initialisation
of the density), for the electricity modules to initialise the domain
temperature and for the compressible module (initialisations). It must be given
in Kelvin.}

\motcleb{cp0}{ra}{real number $>$ 0}{\tt -grand*10}{O}{L1}
{{\tt cp0} is the reference specific heat\\
useful if there is 1$\leqslant$n$\leqslant$nscaus\footnote{None of the scalars
from the specific physics is a temperature} so that {\tt iscsth(n)}=1
(there is a scalar ``temperature''); unless the user specifies the
specific heat in the user subroutine \texttt{usphyv}\footnote{When using the
Graphical Interface, {\tt cp0} is also used to calculate the diffusivity of the
thermal scalars, based on their conductivity; it is therefore needed, unless the
diffusivity is also specified in \texttt{usphyv}} ({\tt icp} $>$ 0)\\
with the compressible module or coal combustion, {\tt cp0} is also needed even when
there is no user scalar}

\motcleb{icp}{ia}{0 or 1}{0}{O}{L1}
{indicates if the specific heat $C_p$ is variable
({\tt icp}=1) or not (0)\\
When gas or coal combustion is activated, {\tt icp} is automatically set to 0
(constant $C_p$). With the electric module, it is automatically set to 1.
The user is not allowed to modify these default choices.\\
When {\tt icp}=1 is specified, the code automatically modifies this value to
make {\tt icp} designate the effective index-number of the property
``specific heat''. For each cell {\tt iel}, the value of
$C_p$ is then specified by the user in the appropriate subroutine
(\texttt{usphyv} for the standard physics) and stored in the array\\
{\tt propce(iel,ipproc(icp))}
({\em see p.~\pageref{sec:prg_propvar} for specific conditions of use})
useful if there is 1$\leqslant$N$\leqslant${\tt nscal} so that {\tt iscsth(n)}=1
(there is a scalar ``temperature'') or with the compressible module for non
perfect gases}

\motcleb{visls0}{ra}{real number $>$ 0}{\tt -grand*10}{C}{L1}
{{\tt visls0(j)}: reference molecular diffusivity related to the scalar J
($kg.m^{-1}.s^{-1}$)\\
negative value: not initialised\\
useful if 1$\leqslant$J$\leqslant$ {\tt nscal}, unless the user specifies the
molecular diffusivity in the appropriate user subroutine (\texttt{usphyv} for
the standard physics) ({\tt field\_get\_key\_id(ivarfl(isca(iscal)),kivisl,...)} $>$ -1)\\
{\em Warning: {\tt visls0} corresponds to the diffusivity. For the temperature, it is
therefore defined as $\lambda/C_p$ where $\lambda$ and $C_p$ are the
conductivity and specific heat. When using the Graphical Interface, $\lambda$ and
$C_p$ are specified separately, and {\tt visls0} is calculated automatically\\
With the compressible module, {\tt visls0} (given in \texttt{uscfx2}) is directly the
thermal conductivity $W.m^{-1}.K^{-1}$\\
With gas or coal combustion, the molecular diffusivity of the enthalpy
($kg.m^{-1}.s^{-1}$) must be specified by the user in the variable {\tt diftl0}
(\texttt{cs\_user\_combustion})\\
With the electric module, for the Joule effect, the diffusivity is specified by
the user in \texttt{uselph} (even if it is constant). For the electric arcs, it
is calculated from the thermochemical data file}}

\motcleb{diftl0}{r}{real number $>$ 0}{\tt -grand}{C}{L1}
{molecular diffusivity for the enthalpy ($kg.m^{-1}.s^{-1}$) for gas or coal
combustion (the code then automatically sets {\tt visls0} to {\tt diftl0} for the scalar
representing the enthalpy)\\
always useful for gas or coal combustion}

\motcleb{min\_scalar\_clipping}{ra}{real number}{\tt grand}{O}{L1}
{field key work (get the index of the key using
\code{call field\_get\_key\_id("min\_scalar\_clipping", kscmin)})
which is the lower limit value for the scalar {\tt iscal}. At each time step,
in every cell where the calculated value for the field \code{ivarfl(isca(iscal))}
is less than the set \code{min\_value}
(\code{call field\_set\_key\_double(ivarfl(isca(iscal)), kscmin, min\_value)})
the field will be reset to
\mbox{\code{min\_value}}\\
there is no limitation if \code{min\_value}$>$\code{max\_value}\\
\code{min\_value} shall not be specified for non-user scalars (specific physics) or for
scalar variances
}

\motcleb{max\_scalar\_clipping}{ra}{real number}{\tt grand}{O}{L1}
{field key work (get the index of the key using
\code{call field\_get\_key\_id("max\_scalar\_clipping", kscmax)})
which is the upper limit value for the scalar {\tt iscal}. At each time step,
in every cell where the calculated value for the field \code{ivarfl(isca(iscal))}
is greater than the set \code{max\_value}
(\code{call field\_set\_key\_double(ivarfl(isca(iscal)), kscmax, max\_value)})
the field will be reset to
\mbox{\code{max\_value}}\\
there is no limitation if \code{max\_value}$>$\code{min\_value}\\
\code{max\_value} shall not be specified for non-user scalars (specific physics) or for
scalar variances
}

\motcle{sigmas}{ra}{real number $>$ 0}{1}{O}{L2}
{{\tt sigmas(iscal)}: turbulent Prandtl (or Schmidt) number for the scalar
 {\tt iscal}\\
useful if and only if  1$\leqslant${\tt iscal}$\leqslant$ {\tt nscaus}}

\motcle{rvarfl}{ra}{real number $>$ 0}{0.8}{O}{L2}
{when {\tt iscavr(iscal)}$>$0, {\tt rvarfl(iscal)} is the coefficient $R_f$ in
the dissipation term $\displaystyle -\frac{\rho}{R_f}\frac{\varepsilon}{k}$
of the equation concerning the scalar {\tt iscal},
which represents the root mean square of the
fluctuations of the scalar {\tt iscavr(iscal)}\\
useful if and only if there is 1$\leqslant${\tt iscal}$\leqslant$ {\tt nscal} such as
 {\tt iscavr(iscal)}$>$0}


%==================================
\subsubsection{Modelling parameters}
%==================================

\motcleb{xlomlg}{ra}{real number $>$ 0}{\tt -grand*10}{O}{L1}
{{\tt xlomlg} is the mixing length\\
useful if and only if {\tt iturb}= 10 (mixing length)}

\motcle{almax}{ra}{\texttt{-grand}, real number $>$ 0}{\tt -grand*10}{O}{L2}
{{\tt almax} is a characteristic macroscopic
length of the domain, used for the initialisation of the turbulence and
the potential clipping (with {\tt iclkep}=1)\\
negative value: not initialised (the code then uses the cubic root of
the domain volume)\\
useful if and only if {\tt turb}= 20, 21, 30, 31, 50 or 60 (RANS models)}

\motcleb{uref}{ra}{real number $>$ 0}{\tt -grand*10}{C}{L1}
{{\tt uref} is the characteristic flow velocity,
used for the initialisation of the turbulence\\
negative value: not initialised\\
useful if and only if {\tt iturb}= 20, 21, 30, 31, 50 or 60 (RANS model)
and the turbulence is not initialised somewhere
else (restart file or subroutine \texttt{cs\_user\_initialization})}


\minititre{Basic constants of the $k-\varepsilon$ and the other RANS models}

\motcle{xkappa}{r}{real number $>$ 0}{0.42}{O}{L3}
{K\'arm\'an constant\\
useful if and only if {\tt iturb}$\geqslant$10
(mixing length, $k-\varepsilon$, $R_{ij}-\varepsilon$, LES, v2f or $k-\omega$)}

\motcle{cstlog}{r}{real number $>$ 0}{5.2}{O}{L3}
{constant of the logarithmic wall function\\
useful if and only if {\tt iturb}$\geqslant$10
(mixing length, $k-\varepsilon$, $R_{ij}-\varepsilon$, LES, v2f or $k-\omega$)}

\motcle{cmu}{r}{real number $>$ 0}{0.09}{O}{L3}
{constant $C_\mu$ for all the RANS turbulence models except for the v2f model
(see {\tt cv2fmu\index{cv2fmu}} for the value of $C_\mu$ in case of v2f modelling)\\
useful if and only if {\tt iturb}= 20,
21, 30, 31 or 60 ($k-\varepsilon$, $R_{ij}-\varepsilon$ or $k-\omega$)}

\motcle{ce1}{r}{real number $>$ 0}{1.44}{O}{L3}
{constant $C_{\varepsilon 1}$ for all the RANS turbulence models except
for the v2f and the $k-\omega$ models\\
useful if and only if {\tt iturb}= 20,
21, 30 or 31 ($k-\varepsilon$ or $R_{ij}-\varepsilon$)}

\motcle{ce2}{r}{real number $>$ 0}{1.92}{O}{L3}
{constant $C_{\varepsilon 2}$ for the $k-\varepsilon$ and
$R_{ij}-\varepsilon$ LRR models\\
useful if and only if {\tt iturb}= 20, 21 or 30
($k-\varepsilon$ or $R_{ij}-\varepsilon$ LRR)}

%\motcle{ce3}{r}{real number $>$ 0}{1}{O}{L3}
%{constante $C_{\varepsilon 3}$\\
%ne sert pas dans la version consid\'er\'ee}

\motcle{ce4}{r}{real number $>$ 0}{1.2}{O}{L3}
{constant $C_{\varepsilon 4}$ for the interfacial term (Lagrangian module) in
case of two-way coupling\\
useful in case of Lagrangian modelling, in $k-\varepsilon$ and $R_{ij}-\varepsilon$
with two-way coupling}

\motcle{sigmak}{r}{real number $>$ 0}{1.0}{O}{L3}
{Prandtl number for $k$ with $k-\varepsilon$ and v2f models\\
useful if and only if {\tt iturb}=20, 21 or 50
($k-\varepsilon$ or v2f)}

\motcle{sigmae}{r}{real number $>$ 0}{1.3}{O}{L3}
{Prandtl number for $\varepsilon$\\
useful if and only if {\tt iturb}= 20,
21, 30, 31 or 50 ($k-\varepsilon$, $R_{ij}-\varepsilon$ or v2f)}

\minititre{Constants specific to the $R_{ij}-\varepsilon$ LRR model ({\tt iturb}=30)}

\motcle{crij1}{r}{real number $>$ 0}{1.8}{O}{L3}
{constant $C_1$ for the $R_{ij}-\varepsilon$ LRR model\\
useful if and only if {\tt iturb}=30
($R_{ij}-\varepsilon$ LRR)}

\motcle{crij2}{r}{real number $>$ 0}{0.6}{O}{L3}
{constant $C_2$ for the $R_{ij}-\varepsilon$ LRR model\\
useful if and only if {\tt iturb}=30
($R_{ij}-\varepsilon$ LRR)}

\motcle{crij3}{r}{real number $>$ 0}{0.55}{O}{L3}
{constant $C_3$ for the $R_{ij}-\varepsilon$ LRR model\\
useful if and only if {\tt iturb}=30
($R_{ij}-\varepsilon$ LRR)}

\motcle{csrij}{r}{real number $>$ 0}{0.22}{O}{L3}
{constant $C_s$ for the $R_{ij}-\varepsilon$ LRR model\\
useful if and only if {\tt iturb}=30
($R_{ij}-\varepsilon$ LRR)}

\motcle{crijp1}{r}{real number $>$ 0}{0.5}{O}{L3}
{constant $C_1^\prime$ for the $R_{ij}-\varepsilon$ LRR model, corresponding to
the wall echo terms\\
useful if and only if {\tt iturb}=30
and {\tt irijec}=1
($R_{ij}-\varepsilon$ LRR)}

\motcle{crijp2}{r}{real number $>$ 0}{0.3}{O}{L3}
{constant $C_2^\prime$ for the $R_{ij}-\varepsilon$ LRR model, corresponding to
the wall echo terms\\
useful if and only if {\tt iturb}=30 and {\tt irijec}=1
($R_{ij}-\varepsilon$ LRR)}

\minititre{Constants specific to the $R_{ij}-\varepsilon$ SSG model}

\motcle{cssgs1}{r}{real number $>$ 0}{1.7}{O}{L3}
{constant $C_{s1}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgs2}{r}{real number $>$ 0}{-1.05}{O}{L3}
{constant $C_{s2}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgr1}{r}{real number $>$ 0}{0.9}{O}{L3}
{constant $C_{r1}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgr2}{r}{real number $>$ 0}{0.8}{O}{L3}
{constant $C_{r2}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgr3}{r}{real number $>$ 0}{0.65}{O}{L3}
{constant $C_{r3}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgr4}{r}{real number $>$ 0}{0.625}{O}{L3}
{constant $C_{r4}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssgr5}{r}{real number $>$ 0}{0.2}{O}{L3}
{constant $C_{r1}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\motcle{cssge2}{r}{real number $>$ 0}{1.83}{O}{L3}
{constant $C_{\varepsilon 2}$ for the $R_{ij}-\varepsilon$ SSG model\\
useful if and only if {\tt iturb}=31
($R_{ij}-\varepsilon$ SSG)}

\minititre{Constants specific to the v2f $\varphi$-model}

\motcle{cv2fa1}{r}{real number $>$ 0}{0.05}{O}{L3}
{constant $a_1$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fe2}{r}{real number $>$ 0}{1.85}{O}{L3}
{constant $C_{\varepsilon 2}$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fmu}{r}{real number $>$ 0}{0.22}{O}{L3}
{constant $C_\mu$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fc1}{r}{real number $>$ 0}{1.4}{O}{L3}
{constant $C_1$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fc2}{r}{real number $>$ 0}{0.3}{O}{L3}
{constant $C_2$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fct}{r}{real number $>$ 0}{6}{O}{L3}
{constant $C_T$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fcl}{r}{real number $>$ 0}{0.25}{O}{L3}
{constant $C_L$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\motcle{cv2fet}{r}{real number $>$ 0}{110}{O}{L3}
{constant $C_\eta$ for the v2f $\varphi$-model\\
useful if and only if {\tt iturb}=50
(v2f $\varphi$-model)}

\minititre{Constants specific to the $k-\omega$ SST model}

\motcle{ckwsk1}{r}{real number $>$ 0}{1/0.85}{O}{L3}
{constant $\sigma_{k1}$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwsk2}{r}{real number $>$ 0}{2}{O}{L3}
{constant $\sigma_{k2}$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwsw1}{r}{real number $>$ 0}{2}{O}{L3}
{constant $\sigma_{\omega 1}$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwsw2}{r}{real number $>$ 0}{1/0.856}{O}{L3}
{constant $\sigma_{\omega 2}$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwbt1}{r}{real number $>$ 0}{0.075}{O}{L3}
{constant $\beta_1$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwbt2}{r}{real number $>$ 0}{0.0828}{O}{L3}
{constant $\beta_2$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwgm1}{r}{real number $>$ 0}
{$\frac{\beta_1}{C_\mu}-\frac{\kappa^2}{\sqrt{C_\mu}\sigma_{\omega 1}}$}{O}{L3}
{constant $\gamma_1$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)\\
{\em Warning: $\gamma_1$ is calculated before the call to
\texttt{usipsu}. Hence, if $\beta_1$, $C_\mu$, $\kappa$ or $\sigma_{\omega 1}$
is modified in \texttt{usipsu}, \texttt{ckwgm1} must also be modified in accordance}}

\motcle{ckwgm2}{r}{real number $>$ 0}
{$\frac{\beta_2}{C_\mu}-\frac{\kappa^2}{\sqrt{C_\mu}\sigma_{\omega 2}}$}{O}{L3}
{constant $\gamma_2$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)\\
{\em Warning: $\gamma_2$ is calculated before the call to
\texttt{usipsu}. Hence, if $\beta_2$, $C_\mu$, $\kappa$ or $\sigma_{\omega 2}$
is modified in \texttt{usipsu}, \texttt{ckwgm2} must also be modified in
accordance}}

\motcle{ckwa1}{r}{real number $>$ 0}{0.31}{O}{L3}
{constant $a_1$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}

\motcle{ckwc1}{r}{real number $>$ 0}{10}{O}{L3}
{constant $c_1$ for the $k-\omega$ SST model\\
useful if and only if {\tt iturb}=60
($k-\omega$ SST)}


%==================================
\subsection{ALE}
%==================================
\motcleb{iale}{i}{0 or 1}{C}{O}{L1}
{activates (=1) or not (=0)  the ALE module}

\motcleb{nalinf}{i}{0 or positive integer}{0}{C}{L2}
{The number of sub-iterations of initialization of the fluid}

\motcleb{nbstru}{i}{0 or positive integer}{0}{C}{L1}
{number of structures, automatically computed}

\motcleb{alpnmk}{r}{real}{0}{C}{L3}
{$alpha$ Newmark's method}

\motcleb{betnmk}{r}{real}{\texttt{-grand}}{C}{L3}
{$beta$ Newmark's method}

\motcleb{gamnmk}{r}{real}{\texttt{-grand}}{C}{L3}
{$gamma$ Newmark's method}

\motcleb{nalimx}{i}{positive integer}{15}{C}{L2}
{maximum number of implicitation iterations for the structure displacement}

\motcleb{epalim}{r}{positive real}{$1.10^{-5}$}{C}{L2}
{Relative precision of implicitation of the structure displacement }

\motcleb{iflxmw}{i}{0 or 1}{1}{O}{L2}
{method to compute interior mass flux due to ALE mesh velocity\\
\hspace*{1.3cm} = 1: based on cell center mesh velocity\\
\hspace*{1.3cm} = 0: based on nodes displacement
}
%==================================
\subsection{Thermal radiative transfers: global settings}
%==================================

All the following keywords may be modified in the user subroutines
\texttt{usray*} (or, for some of them, through the thermochemical data files).
It is however not recommended to modify those which do not belong to
level L1.

\motcleb{iirayo}{ia}{0, 1, 2}{0}{O}{L1}
{{\tt iirayo} activates ($>0$) or deactivates
(=0) the radiation module\\
The different values correspond to the following modelling methodes:\\
\hspace*{1.3cm} = 1: discrete ordinates method
(DOM standard option for radiation in semi-transparent media)\\
\hspace*{1.3cm} = 2: ``P-1'' methode\\
{\em Warning: the P-1 methode allows faster computations, but it
may only be applied to media with uniform large optical thickness, such as
some cases of pulverised coal combustion}}

\motcle{imodak}{i}{0 or 1}{0}{O}{L3}
{when gas or coal combustion is activated, {\tt imodak} indicates whether the
absorption coefficient shall be calculated ``automatically'' (=1) or read from
the data file (=0)\\
useful if the radiation module is activated}

\motcleb{isuird}{i}{0 or 1}{isuite}{C}{L1}
{indicates whether the radiation variables should be initialised (=0) or read
from a restart file (=1)\\
useful if and only if the radiation module is activated (in this case, a
restart file {\em rayamo} must be available)}

\motcleb{nfreqr}{i}{strictly positive integer}{1}{O}{L1}
{period of the radiation module\\
the radiation module is called every {\tt nfreqr} time steps (more precisely,
every time {\tt ntcabs} is a multiple of {\tt nfreqr}). Also, in order to
have proper initialisation of the variables, whatever the value of {\tt nfreqr},
the radiation module is called at the first time step of a calculation
(restart or not)\\
useful if and only if the radiation module is activated}

\motcleb{ndirec}{i}{32 or 128}{32}{O}{L1}
{number of directions for the angular discretisation of the radiation
propagation with the DOM model ({\tt iirayo}=1)\\
no other possible value, because of the way the directions are calculated\\
the calculation with 32 directions may break the symmetry of
physically axi-symmetric cases (but the cost in CPU time is much lower
 than with 128 directions)\\
useful if and only if the radiation module is activated with the DOM method}

\motcle{xnp1mx}{r}{real number}{10}{O}{L3}
{with the P-1 model ({\tt iirayo}=2), {\tt xnp1mx} is the percentage of cells of
the calculation domain for which it is acceptable that the optical
thickness is lower than unity\footnote{more precisely, where $KL$ is lower than
1, where $K$ is the absorption coefficient of the medium and $L$ is a
characteristic length of the domain}, although it is not to be desired\\
useful if and only if the radiation module is activated with the P-1 method}

\motcleb{idiver}{i}{0, 1 or 2}{2}{C}{L1}
{indicates the method used to calculate the radiative source term:\\
\hspace*{1.3cm}= 0: semi-analytic calculation (compulsory with transparent
media)\\
\hspace*{1.3cm}= 1: conservative calculation\\
\hspace*{1.3cm}= 2: semi-analytic calculation corrected in order to be
globally conservative\\
useful if and only if the radiation module is activated\\
{\em Note: if the medium is transparent, the choice has no effect on the calculation}}

\motcleb{iimpar}{i}{0, 1 or 2}{1}{O}{L1}
{Verbosity level in the listing concerning the calculation of
the wall temperatures:\\
\hspace*{1.3cm}= 0: no display\\
\hspace*{1.3cm}= 1: standard\\
\hspace*{1.3cm}= 2: complete\\
useful if and only if the radiation module is activated}

\motcleb{iimlum}{i}{0, 1 or 2}{1}{O}{L1}
{Verbosity level in the listing concerning the solution of
the radiative transfer equation:\\
\hspace*{1.3cm}= 0: no display\\
\hspace*{1.3cm}= 1: standard\\
\hspace*{1.3cm}= 2: complete\\
useful if and only if the radiation module is activated}

\motcleb{nbrvaf}{ca}{string of less than 80 characters}{name}{O}{L1}
{name associated for the post-processing to each of the following variables,
defined at the boundary faces ({\it see}
\cite{Douce02} for more details concerning their definitions):\\
\hspace*{1.3cm} {\tt nbrvaf(itparp)}: wall temperature at the boundary
faces ($K$)\\
\hspace*{1.3cm} {\tt nbrvaf(iqincp)}: radiative incident flux density
($W/m^2$)\\
\hspace*{1.3cm} {\tt nbrvaf(ixlamp)}: thermal conductivity of the
boundary faces ($W/m/K$)\\
\hspace*{1.3cm} {\tt nbrvaf(iepap)}: wall thickness ($m$)\\
\hspace*{1.3cm} {\tt nbrvaf(iepsp)}: wall emissivity \\
\hspace*{1.3cm} {\tt nbrvaf(ifnetp)}: net radiative flux density ($W/m^2$)\\
\hspace*{1.3cm} {\tt nbrvaf(ifconp)}: convective flux density ($W/m^2$)\\
\hspace*{1.3cm} {\tt nbrvaf(ihconp)}: convective exchange coefficient
($W/m^2/K$)\\
The default values are: \\
\hspace*{1.3cm} {\tt nbrvaf(itparp)} = Wall\_temp \\
\hspace*{1.3cm} {\tt nbrvaf(iqincp)} = Incident\_flux \\
\hspace*{1.3cm} {\tt nbrvaf(ixlamp)} = Th\_conductivity \\
\hspace*{1.3cm} {\tt nbrvaf(iepap)} = Thickness \\
\hspace*{1.3cm} {\tt nbrvaf(iepsp)} = Emissivity \\
\hspace*{1.3cm} {\tt nbrvaf(ifnetp)} = Net\_flux \\
\hspace*{1.3cm} {\tt nbrvaf(ifconp)} = Convective\_flux \\
\hspace*{1.3cm} {\tt nbrvaf(ihconp)} = Convective\_exch\_coef \\
useful if and only if the radiation module is activated}

\motcleb{irayvf}{ia}{-1 or 1}{-1}{O}{L1}
{activates (=1) or deactivates (=-1) the post-processing for each of the
following variables defined at the boundary faces:\\
\hspace*{1.3cm} {\tt irayvf(itparp)}: wall temperature at the boundary
faces ($K$)\\
\hspace*{1.3cm} {\tt irayvf(iqincp)}: incident radiative flux density
($W/m^2$)\\
\hspace*{1.3cm} {\tt irayvf(ixlamp)}: thermal conductivity of the
boundary faces ($W/m/K$)\\
\hspace*{1.3cm} {\tt irayvf(iepap)}: wall thickness ($m$)\\
\hspace*{1.3cm} {\tt irayvf(iepsp)}: wall emissivity \\
\hspace*{1.3cm} {\tt irayvf(ifnetp)}: net radiative flux density ($W/m^2$)\\
\hspace*{1.3cm} {\tt irayvf(ifconp)}: convective flux density ($W/m^2$)\\
\hspace*{1.3cm} {\tt irayvf(ihconp)}: convective exchange coefficient
($W/m^2/K$)\\
useful if and only if the radiation module is activated}

\motcle{tmin}{r}{positive real number}{0}{O}{L3}
{minimum allowed value for the wall temperatures in Kelvin\\
useful if and only if the radiation module is activated}

\motcle{tmax}{r}{positive real number}{{\tt grand} + 273.15}{O}{L3}
{maximum allowed value for the wall temperatures in Kelvin\\
useful if and only if the radiation module is activated}

%==================================
\subsection{Electric module (Joule effect and electric arcs): specificities}
%==================================

The electric module is composed of a Joule effect module
(\texttt{ippmod(ieljou)\index{ieljou}}) and an electric arcs module
(\texttt{ippmod(ielarc)\index{ielarc}}).

The Joule effect module is designed to take into account the Joule effect
(for instance in glass furnaces) with real or complex potential in the
enthalpy equation. The Laplace forces are not taken into account in the
impulse momentum equation. Specific boundary conditions can be applied to
account for the coupled effect of transformers (offset) in glass furnaces.

The electric arcs module is designed to take into account the Joule effect
(only with real potential) in the enthalpy equation. The Laplace forces
are taken into account in the impulse momentum equation.

The keywords used in the global settings are quite few. They are
found in the subroutine \texttt{useli1} (see the description of this
user subroutine \S\ref{prg_useli1}).

\motcleb{ielcor}{i}{0, 1}{0}{O}{L1}
{when \texttt{ielcor}=1, the boundary conditions for the potential will be
tuned at each time step in order to reach a user-specified target dissipated
power \texttt{puisim} (Joule effect) or a user-specified target current
intensity \texttt{couimp} (electric arcs)\\
the boundary condition tuning is controlled by subroutines \texttt{elreca} or
\texttt{uselrc}\\
always useful}

\motcleb{couimp}{r}{real number $\geqslant 0$}{0}{O}{L1}
{with the electric arcs module, \texttt{couimp} is the target current intensity ($A$)
for the calculations with boundary condition tuning for the potential\\
the target intensity will be reached if the boundary conditions are expressed
using the variable \texttt{dpot} or if the initial boundary conditions are multiplied by
the variable \texttt{coejou}\\
useful with the electric arcs module if \texttt{ielcor}=1}

\motcleb{puisim}{r}{real number $\geqslant 0$}{0}{O}{L1}
{with the Joule effect module, \texttt{puisim} is the target dissipated power ($W$)
for the calculations with boundary condition tuning for the potential\\
the target power will be reached if the boundary conditions are expressed
using the variable \texttt{dpot} or if the initial boundary conditions are multiplied by
the variable \texttt{coejou}\\
useful with the Joule effect module if \texttt{ielcor}=1}

\motcleb{dpot}{r}{real number $\geqslant 0$}{0}{O}{L1}
{\texttt{dpot} is the potential difference ($V$) which generates the current (and the Joule effect) for the
calculations with boundary conditions tuning for the potential. This value is
initialised set by the user (\texttt{useli1}). It is then automatically tuned
depending on the value of dissipated power (Joule effect module) or the
intensity of current (electric arcs module).
In order for the correct power or intensity to be reached, the boundary
conditions for the potential must be expressed with \texttt{dpot}
(\texttt{uselcl}). The tuning can be controlled in \texttt{uselrc}\\
useful if \texttt{ielcor}=1}

\motcleb{modrec}{i}{0, 1, 2}{1}{O}{L1}
{when \texttt{ielcor}=0, we use user function \texttt{uselrc} for boundary condition tuning\\
when \texttt{ielcor}=1, we use standard model for boundary condition tuning\\
when \texttt{ielcor}=2, we use plane scaling model for boundary condition tuning. In this case, we need
define plane and current density component used to}

\motcleb{idreca}{i}{1, 2, 3}{3}{O}{L1}
{defines current density component used to calculate current in plane\\
useful if \texttt{modrec}=2}

\motcleb{crit\_reca}{r}{real number $\geqslant 0$}{0}{O}{L1}
{defines plane coordinates component used to calculate current in plane\\
useful if \texttt{modrec}=2}

%=================================================
\subsection{Compressible module: specificities}
%==================================

The keywords used in the global settings are quite few. They are
found in the subroutines \texttt{uscfx1} and \texttt{uscfx2}, in
the \texttt{cs\_user\_parameters.f90} file (see the
description of these user subroutines, \S\ref{prg_uscfx12}).

\motcleb{ieos}{i}{1}{1}{C}{L1}
{\texttt{ieos} indicates the equation of state. Only perfect gas with a constant adiabatic coefficient,
\texttt{ieos=1} is available, but the user can complete the subroutine
\texttt{cfther}, which is not a user subroutine, to add new equations of state.\\
always useful
}

\motcleb{xmasmr}{r}{1}{1}{C}{L1}
{\texttt{xmasmr} is the molar mass of the perfect gas in kg/mol (\texttt{ieos=1})\\
always useful
}

\motcleb{icfgrp}{ia}{0 or 1}{1}{C}{L1}
{\texttt{icfgrp} indicates if the boundary
conditions should take into account (=1) or not (=0) the hydrostatic balance.\\
always useful.\\
In the cases where gravity is predominant, taking into account the hydrostatic
pressure allows to get rid of the disturbances which may appear near the
horizontal walls when the flow is little convective.\\
%
Otherwise, when \texttt{icfgrp}=0, the pressure condition is calculated
from the solution of the one-dimensional Euler equations for a perfect
gas near a wall, for the variables ``normal velocity'', ``density'' and
``pressure'':
\vspace{0.2cm}
\begin{list}{}{}
\item Case of an expansion ($M \leqslant 0$):\\
$$
\begin{array}{l}
\left\{\begin{array}{lll}
P_p=0 & \text{if} & 1 + \displaystyle\frac{\gamma-1}{2}M<0\\
P_p = P_i \left(1 + \displaystyle\frac{\gamma-1}{2}M\right)
^{\frac{2\gamma}{\gamma-1}} & \text{otherwise}\\
\end{array}\right.\\
\end{array}
$$

\item Case of a shock ($M > 0$):\\
$$
\begin{array}{l}
P_p = P_i \left(1 + \displaystyle\frac{\gamma(\gamma+1)}{4}M^2
+\gamma M \displaystyle\sqrt{1+\displaystyle\frac{(\gamma+1)^2}{16}M^2}\right)
\end{array}
$$

with $M = \displaystyle\frac{\vect{u}_i \cdot \vect{n}}{c_i}$, internal
      Mach number calculated with the variables taken in the cell
      adjacent to the wall.\\

\end{list}
}

\motcleb{iviscv}{i}{0 or 1}{\texttt{0}}{C}{L1}
{\texttt{iviscv=0} indicates that
the volume viscosity is constant and equal to the reference volume viscosity
\texttt{viscv0}.\\
\texttt{iviscv}=1 indicates that the volume viscosity is variable: its
variation law must be specified in the user subroutine \texttt{usphyv}.\\
always useful\\
The volume viscosity $\kappa$ is defined by the formula expressing the stress:
\begin{equation}
   \tens{\sigma} = -P\,\tens{Id} + \mu (\grad\,\vect{u} +  \ ^{t}\ggrad\,\vect{u})
           +(\kappa-\frac{2}{3}\mu)\,\dive(\vect{u})\,\tens{Id}
\end{equation}
}

\motcleb{viscv0}{r}{real number $\ge$ 0}{0}{O}{L1}
{\texttt{viscv0} is the reference volume
viscosity (noted $\kappa$ in the equation expressing $\tens{\sigma}$ in the
paragraph dedicated to \texttt{iviscv})\\
always useful, it is the used value, unless the user specifies the volume
viscosity in the user subroutine \texttt{usphyv}}

\motcle{igrdpp}{i}{0 or 1}{1}{O}{L3}
{indicates whether the pressure should be updated (=1) or not (=0) after the
solution of the acoustic equation\\
always useful}

%==================================================
\subsection{Lagrangian multiphase flows}
%==================================================
\label{sec:prg_motscles_lagr}

Most of these keywords may be modified in the user subroutines
\texttt{uslag1}, \texttt{uslag2}, \texttt{uslaen},
\texttt{uslast} and \texttt{uslaed}. It is however strongly recommended
not to modify those belonging to the level L3.

First of all, it should be noted that the Lagrangian module is compliant with
almost all the RANS turbulence models and with laminar flows. However, the standard particle
turbulent dispersion model does not take fully advantage of the second-order
$R_{ij}-\varepsilon$ models. The same isotropic model is used as in the
$k-\varepsilon$ models, with $k$ calculated from the trace of $R_{ij}$. Also,
two-way coupling is not compatible with the $k-\omega$ SST model.


\subsubsection{Global settings}

\motcleb{iilagr}{I}{0, 1, 2, 3}{0}{C}{L1}
{activates ($>$0) or deactivates (=0) the Lagrangian module\\
the different values correspond to the following modellings: \\
\hspace*{1.3cm} = 1 Lagrangian two-phase flow in one-way coupling (no influence of
the particles on the continuous phase)\\
\hspace*{1.3cm} = 2 Lagrangian two-phase flow with two-way coupling (influence of
the particles on the dynamics of the continuous phase). Dynamics, temperature and mass may be coupled independently\\
\hspace*{1.3cm} = 3 Lagrangian two-phase flow on frozen continuous phase. This option can
only be used in case of a calculation restart. All the
Eulerian fields are frozen (including the scalar fields). This option
automatically implies \texttt{iccvfg} = 1\\
always useful}

\motcleb{isuila}{i}{0, 1}{0}{C}{L1}
{activation (=1) or not (=0) of a Lagrangian calculation restart.
The calculation restart file read when this option is activated (\texttt{ficaml})
only contains the data related to the particles (see also \texttt{isuist})\\
the global calculation must also be a restart calculation\\
always useful}

\motcleb{isuist}{i}{0, 1}{0}{C}{L1}
{during a Lagrangian calculation restart, indicates whether the particle
statistics (volume and boundary) and two-way coupling terms are to be read from
a restart file (=1) or reinitialised (=0). The file to be read is
\texttt{ficmls}\\
useful if \texttt{isuila} = 1}

\motcleb{nbpmax}{i}{positive or null integer}{1000}{C}{L1}
{maximum number of particles allowed simultaneously in the calculation
domain. It must be reminded that the required memory evolves accordingly}

\motcle{nbpart}{i}{positive or null integer}{0}{O}{L3}
{number of particles treated during one Lagrangian time step\\
\texttt{nbpart} must always be lower than \texttt{nbpmax}\\
always useful, but initialised and updated without intervention of the user}

\motcle{nvls}{i}{integer between 0 and 10}{0}{O}{L2}
{number of additional variables related to the particles\\
the additional variables can be accessed in the arrays
\texttt{eptp\index{eptp}} and \texttt{eptpa\index{eptpa}} by means of the
pointer \texttt{jvls\index{jvls}}: \texttt{eptp(jvls(ii),nbpt)} and
\texttt{eptpa(jvls(ii),nbpt)} (\texttt{nbpt} is
the index-number of the treated particle, and \texttt{ii} an integer
between 1 and \texttt{nvls})}

\motcleb{isttio}{i}{0, 1}{0}{C}{L1}
{indicates the steady (=1) or unsteady (=0) state of the
continuous phase flow\\
in particular, \texttt{isttio} = 1 is needed in order to: \\
\hspace*{1cm}calculate steady statistics in the volume or at the boundaries
(starting respectively from the Lagrangian iterations \texttt{nstist} and
\texttt{nstbor}) \\
\hspace*{1cm}calculate time-averaged two-way coupling source terms (from the
Lagrangian iteration \texttt{nstits}) \\
useful if \texttt{iilagr}=1 or \texttt{iilagr}=2 (if \texttt{iilagr}=3,
then \texttt{isttio}=1 is automatically set)}

\motcleb{injcon}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) the continuous injection of particles\\
this option allows to inject particles continuously during the duration of the
Lagrangian time step \texttt{dtp\index{dtp}} rather than only once at the
beginning of the Lagrangian iteration. It helps avoiding the fractioning of
the particle cloud close to the injection areas}

\motcleb{iroule}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the particle cloning/fusion technique
(option also called ``Russian roulette'')\\
when \texttt{iroule} = 1, the importance function must be specified {\em via} the
array \texttt{croule\index{croule}} in the user subroutine \texttt{uslaru}}

\motcle{\texttt{ttclag}}{r}{positive real number}{0}{O}{L3}
{physical time of the Lagrangian simulation \\
always useful}

\motcle{iplas}{i}{integer $>$ 0}{1}{O}{L3}
{absolute iteration number (including the restarts) in the Lagrangian
module ({\em i.e.} Lagrangian time step number) \\
always useful}


%==================================================
\subsubsection{Specific physics models associated with the particles}
%==================================================

\motcleb{iphyla}{i}{0, 1, 2}{0}{C}{L1}
{activates ($>$0) or deactivates (=0) the physical models associated to the
particles:\\
\hspace*{1.3cm} = 1: allows to associate with the particles evolution
equations on their temperature (in degrees Celsius), their diameter and
their mass\\
\hspace*{1.3cm} = 2: the particles are pulverised coal particles.
Evolution equations on temperature (in degree Celsius), mass of
reactive coal, mass of char and diameter of the shrinking core are
associated with the particles. This option is available only if the
continuous phase represents a pulverised coal flame\\
always useful}

\motcleb{idpvar}{i}{0, 1}{0}{O}{L1}
{activation (=1) or not (=0) of an evolution equation on the particle
diameter\\
useful if \texttt{iphyla} = 1}

\motcleb{itpvar}{i}{0, 1}{0}{O}{L1}
{activation (=1) or not (=0) of an evolution equation on the particle
temperature (in degrees Celsius)\\
useful if \texttt{iphyla} = 1 and if there is a thermal scalar associated with
the continuous phase}

\motcleb{impvar}{i}{0, 1}{0}{O}{L1}
{activation (=1) or not (=0) of an evolution equation on the
particle mass\\
useful if si \texttt{iphyla} = 1}

\motcleb{tpart}{r}{real number $>$ \texttt{tkelvn}}{700}{O}{L1}
{initialisation temperature (in degree Celsius) for the particles already
present in the calculation domain when an evolution equation on
the particle temperature is activated during a calculation (\texttt{iphyla} =
1 and \texttt{itpvar} = 1)\\
useful if \texttt{isuila} = 1 and \texttt{itpvar} = 0 in the previous
calculation}

\motcleb{cppart}{r}{positive real number}{5200}{O}{L1}
{initialisation value for the specific heat ($J.kg^{-1}.K^{-1}$) of the
particles already present in the calculation domain when an evolution equation
on the particle temperature is activated during a calculation
(\texttt{iphyla} = 1 and \texttt{itpvar} = 1)\\
useful if \texttt{isuila} = 1 and \texttt{itpvar} = 0 in the previous calculation}

\motcleb{iencra}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) the option of coal particle
fouling. It then is necessary to specify the domain boundaries
on which fouling may take place.\\
useful if \texttt{iphyla} = 2}

\motcleb{tprenc}{r}{real number $>$ \texttt{tkelvn}}{600}{O}{L1}
{limit temperature (in degree Celsius) below which the coal particles do
not cause any fouling (if the fouling model is activated)\\
useful if \texttt{iphyla} = 2 and \texttt{iencra} = 1}

\motcleb{visref}{r}{positive real number}{10000}{O}{L1}
{ash critical viscosity in $kg.m^{-1}.s^{-1}$, in the fouling model
\footnote{J.D. Watt
and T. Fereday (\textit{J.Inst.Fuel}, Vol.42-p99)}\\
useful if \texttt{iphyla} = 2 and \texttt{iencra} = 1}

%==================================================
\subsubsection{Options for two-way coupling}
%==================================================

\motcleb{nstits}{i}{strictly positive integer}{1}{O}{L1}
{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 (\texttt{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
\texttt{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 (\texttt{isttio}=0)\\
useful if \texttt{iilagr} = 2 and \texttt{isttio} = 1}

\motcleb{ltsdyn}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the two-way coupling on the dynamics of the
continuous phase\\
useful if \texttt{iilagr} = 2 and \texttt{iccvfg} = 0}

\motcleb{ltsmas}{i}{0, 1}{0}{O}{L1}
{activation (=1) or not (=0) of the two-way coupling on the mass\\
useful if \texttt{iilagr} = 2, \texttt{iphyla} = 1 and \texttt{impvar} = 1}

\motcleb{ltsthe}{i}{0, 1}{0}{O}{L1}
{if \texttt{iphyla} = 1 and \texttt{itpvar} = 1, \texttt{ltsthe}
 activates (=1) or not (=0) the two-way coupling on temperature\\
if \texttt{iphyla} = 2, \texttt{ltsthe} activates (=1) or not (=0) the
two-way coupling on the Eulerian variables related to pulverised coal
combustion\\
useful if \texttt{iilagr} = 2}

%==================================================
\subsubsection{Numerical modelling}
%==================================================

\motcle{nordre}{i}{1, 2}{2}{O}{L2}
{order of integration for the stochastic differential equations\\
\hspace*{1.3cm} = 1 integration using a first-order scheme\\
\hspace*{1.3cm} = 2 integration using a second-order scheme\\
always useful}

\motcle{ilapoi}{i}{0, 1}{0}{O}{L3}
{activation (=1) or not (=0) of the solution of a Poisson's equation for
the correction of the particle instantaneous velocities (in order to obtain a
null divergence)\\
this option is not validated and reserved to the development team. The user must not change
the default value}

\motcle{idistu}{i}{0, 1}{1}{O}{L3}
{activation (=1) or not (=0) of the particle turbulent dispersion\\
the turbulent dispersion is compatible only with the RANS turbulent models
($k-\varepsilon$, $R_{ij}-\varepsilon$, v2f or $k-\omega$)\\
(\texttt{iturb}=20, 21, 30, 31, 50 or 60)\\
always useful}

\motcle{idiffl}{i}{0, 1}{0}{O}{L3}
{\texttt{idiffl}=1 suppresses the crossing trajectory effect, making
turbulent dispersion for the particles identical to the turbulent
diffusion of fluid particles\\
useful if \texttt{idistu}=1}

\motcleb{modcpl}{i}{positive integer}{0}{O}{L1}
{activates ($>$0) or not (=0) the complete turbulent dispersion model\\
when \texttt{modcpl} is strictly positive, its value is interpreted as the
absolute Lagrangian time step number (including restarts) after which the
complete model is applied\\
since the complete model uses volume statistics, \texttt{modcpl} must
either be 0 or be greater than \texttt{idstnt}\\
useful if \texttt{istala} = 1}

\motcleb{idirla}{i}{1, 2, 3}{1}{O}{L1}
{$x$, $y$ or $z$ direction of the complete model\\
it corresponds to the main directions of the flow\\
useful if \texttt{modcpl} $>$ 0}

%==================================================
\subsubsection{Volume statistics}
%==================================================

\motcleb{istala}{i}{0, 1}{0}{C}{L1}
{activation (=1) or not (=0) of the calculation of the volume
statistics related to the dispersed phase\\
if \texttt{istala} = 1, the calculation of the statistics is activated
starting from the absolute iteration (including the restarts) \texttt{idstnt}\\
by default, the statistics are not steady (reset to zero at every
Lagrangian iteration). But if \texttt{isttio}=1, since the flow is steady,
the statistics will be averaged overt he different time steps\\
the statistics represent the significant results on the particle cloud\\
always useful}

\motcleb{seuil}{r}{positive real number}{0}{O}{L1}
{every cell of the calculation domain contains a certain quantity of
particles, representing a certain statistical weight (sum of the
statistical weights of all the particles present in the cell). \texttt{seuil}
is the limit statistical weight value, below which the contribution of the
cell in term of statistical weight is not taken into account in the volume
statistics (for the complete turbulent dispersion model, in the
Poisson's equation used to correct the mean velocities or in the listing and
post-processing outputs)\\
useful if \texttt{istala} = 1}

\motcleb{idstnt}{i}{strictly positive integer}{1}{C}{L1}
{absolute Lagrangian iteration number (including the restarts) after
which the calculation of the volume statistics is activated\\
useful if \texttt{istala} = 1}

\motcleb{nstist}{i}{integer $\geqslant$ \texttt{idstnt}}{\texttt{idstnt}}{O}{L1}
{absolute Lagrangian iteration number (including the restarts) after
which the volume statistics are cumulated over time (they are then said to be
steady)\\
if the absolute Lagrangian iteration number is less than \texttt{nstist},
or if the flow is unsteady (\texttt{isttio}=0), the statistics are reset
to zero at each Lagrangian iteration (the volume statistics are then said
to be unsteady)\\
useful if \texttt{istala}=1 and \texttt{isttio}=1}

\motcleb{nomlag}{ca}{string of less than 50 characters}{VarLagXXXX}{O}{L1}
{name of the volumetric statistics, displayed in the listing
and the post-processing files. The default value is given above, with ``XXXX''
representing a four digit number (for instance 0001, 0011 ...)\\
useful if \texttt{istala} = 1\\
{\em Warning: this name is also used to reference information in the restart file
\mbox{(\texttt{isuist} =1)}. If the name of a variable is changed between two
calculations, then it will not be possible to read its value from the restart file}}

\motcleb{nvlsts}{i}{0 $\leqslant$ integer $\leqslant$ \texttt{nussta}=20}{0}{O}{L1}
{number of additional user volume statistics\\
the additional statistics (or their cumulated value in the steady
case) can be accessed in the array \texttt{statis} by means of the pointer
\texttt{ilvu\index{ilvu}}: \texttt{statis(iel,ilvu(ii)\index{statis}})
(\texttt{iel} is the cell index-number and \texttt{ii} an integer between
1 and \texttt{nvlsts})\\
useful if \texttt{istala} = 1}

\motcle{npst}{i}{positive integer}{0}{O}{L3}
{number of iterations during which steady volume statistics have
been cumulated\\
useful if \texttt{istala}=1, \texttt{isttio}=1 and if \texttt{nstist} is
less than or equal to the current Lagrangian iteration\\
\texttt{npst} is initialised and updated automatically by the code, its
value is not to be modified by the user}

\motcle{npstt}{i}{positive integer}{0}{O}{L3}
{number of iterations during which volume statistics have been
calculated (the potential iterations during which unsteady
statistics have been calculated are counted in \texttt{npstt})\\
useful if \texttt{istala}=1\\
\texttt{npstt} is initialised and updated automatically by the code,
its value is not to be modified by the user}

\motcle{tstat}{r}{positive real number}{\texttt{dtp}}{O}{L3}
{if the volume statistics are calculated in a steady way, \texttt{tstat}
represents the physical time during which the statistics have been cumulated\\
if the volume statistics are calculated in a unsteady way,
then \texttt{tstat=dtp\index{dtp}} (it is the Lagrangian time step, because the
statistics are reset to zero at every iteration)\\
useful if \texttt{istala}=1\\
\texttt{tstat} is initialised and updated automatically by the code,
its value is not to be modified by the user}

%==================================================
\subsubsection{Display of particles and trajectories}
%==================================================

The definition of the particle visualization output meshes
itself is done with that of all other postprocessing mesh zones, either
using the GUI, or the \texttt{cs\_user\_postprocess\_meshes} function of
\texttt{cs\_user\_postprocess.c}.

The following options determine which variables are output on those particle
or particle trajectory segment output meshes for which the ``automatic output''
is activated.

\motcleb{ivisv1}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``velocity of the locally
undisturbed fluid flow field'' with the output of particles or trajectories\\
always useful}

\motcleb{ivisv2}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``particle velocity''
with the output of particles or trajectories\\
always useful}

\motcleb{ivistp}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``residence time''
with the output of particles or trajectories\\
always useful}

\motcleb{ivisdm}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``particle diameter''
with the output of particles or trajectories\\
always useful}

\motcleb{iviste}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``particle temperature''
with the output of particles or trajectories\\
always useful}

\motcleb{ivismp}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``particle mass''
with the output of particles or trajectories\\
always useful}

\motcleb{ivisdk}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``shrinking core diameter of
the coal particles'' with the output of particles or trajectories\\
useful only if \texttt{iphyla} = 2}

\motcleb{ivisch}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``mass of reactive coal of the
coal particles'' with the output of particles or trajectories\\
useful only if \texttt{iphyla} = 2}

\motcleb{ivisck}{i}{0, 1}{0}{O}{L1}
{associates (=1) or not (=0) the variable ``mass of coal of the
coal particles'' with the output of particles or trajectories\\
useful only if \texttt{iphyla} = 2}

%==================================================
\subsubsection{Display of the particle/boundary interactions and the statistics at the boundaries}
%==================================================

\motcleb{iensi3}{i}{0, 1}{0}{C}{L1}
{activates (=1) or not (=0) of the recording of the particle/boundary
interactions in  \texttt{parbor\index{parbor}}, and of the calculation of the
statistics at the corresponding boundaries, for post-processing
(\textit{EnSight6} format)\\
By default, the statistics are unsteady (reset to zero at every
Lagrangian iteration). They may be steady if \texttt{isttio}=1 ({\em i.e.}
calculation of a cumulated value over time, and then calculation of an
average over time or over the number of interactions with the boundary)\\
always useful}

\motcleb{nstbor}{i}{strictly positive integer}{1}{O}{L1}
{number of absolute Lagrangian iterations (including the restarts)
after which the statistics at the boundaries are considered steady and are
averaged (over time or over the number of interactions)\\
If the number of absolute Lagrangian iterations is less than \texttt{nstbor},
or if \texttt{isttio}=0, the statistics are reset to zero at every
Lagrangian iteration (unsteady statistics)\\
useful if \texttt{iensi3}=1 and \texttt{isttio}=1}

\motcleb{seuilf}{r}{positive real number}{0}{O}{L1}
{every boundary face of the mesh undergoes a certain number of
interactions with particles, expressed in term of statistical weight
(sum of the statistical weights of all the particles which have
interacted with the boundary face). \texttt{seuilf} is
the limit statistical weight value, below which the contribution of the
face is not taken into account in the
statistics at the boundaries for post-processing\\
useful if \texttt{iensi3}=1}

\motcleb{inbrbd}{i}{0, 1}{1}{O}{L1}
{activates (=1) or not (=0) of the recording of the number of particle/boundary
interactions, and of the calculation of the associated boundary statistics.\\
\texttt{inbrd} = 1 is a compulsory condition to use the particulate average
\texttt{imoybr} = 2\\
useful if \texttt{iensi3}=1}

\motcleb{iflmbd}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the recording of the particulate mass flow
related to the particle/boundary interactions, and of the calculation of
the associated boundary statistics\\
\texttt{inbrd} = 1 is a compulsory condition to use \texttt{iflmbd}=1\\
useful if \texttt{iensi3}=1 and \texttt{inbrbd}=1}


\motcleb{iangbd}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the recording of the angle between a
particle trajectory and a boundary face involved in a particle/boundary
interaction, and of the calculation of the associated boundary statistics\\
useful if \texttt{iensi3}=1}

\motcleb{ivitbd}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the recording of the velocity of a particle
involved in a particle/boundary interaction, and of the calculation of
the associated boundary statistics\\
useful if \texttt{iensi3}=1}

\motcleb{iencbd}{i}{0, 1}{0}{O}{L1}
{activates (=1) or not (=0) of the recording of the mass of coal particles
stuck to the wall due to fouling, on the boundary faces of the \texttt{iencrl}
interaction type\\
useful if \texttt{iensi3}=1, \texttt{iphyla}=2, \texttt{iencra}=1, and if
there is at least one boundary face of the \texttt{iencrl} interaction
type}

\motcleb{nusbor}{i}{positive integer}{0}{O}{L1}
{number of additional user data to record for the calculation
of additional boundary statistics in \texttt{parbor\index{parbor}}\\
useful if \texttt{iensi3}=1}

\motcleb{nombrd}{ca}{string of less than 50 characters}{see
\texttt{uslag1}}{O}{L1}
{name of the boundary statistics, displayed in the listing
and the post-processing files\\
useful if \texttt{iensi3}=1\\
{\em Warning: this name is also used to reference information in the restart file
\mbox{(\texttt{isuist} =1)}. If the name of a variable is changed between two
calculations, it will not be possible to read its value from the restart file}}

\motcleb{imoybr}{ia}{0, 1, 2}{0 , 1 or 2}{O}{L1}
{the recordings in \texttt{parbor} at every particle/boundary interaction are
cumulated values (possibly reset to zero at every iteration in the
unsteady case). They must therefore be divided by a quantity to
get boundary statistics. The user can choose between two average types:\\
\hspace*{1.3cm} = 0: no average is applied to the recorded cumulated values\\
\hspace*{1.3cm} = 1: a time-average is calculated. The cumulated value
is divided by the physical duration in the case of steady
averages (\texttt{isttio}=1). The cumulated value is divided by the value of
the last time step in the case of unsteady averages (\texttt{isttio}=0),
and also in the case of steady averages while the
absolute Lagrangian iteration number is inferior to \texttt{nstbor}\\
\hspace*{1.3cm} = 2: a particulate average is calculated. The cumulated
value is divided by the number of particle/boundary interactions (in terms of
statistical weight) recorded in \texttt{parbor(nfabor,inbr)}. This average
can only be calculated when \texttt{inbrbd}=1. The average is calculated if
the number of interactions (in statistical weight) of the considered
boundary face is strictly higher than \texttt{seuilf}, otherwise the average
at the face is set to zero\\
only the cumulated value is recorded in the restart file\\
useful if \texttt{iensi3}=1}

\motcle{npstf}{i}{positive integer}{0}{O}{L3}
{number of iterations during which steady boundary statistics have
been cumulated\\
useful if \texttt{iensi3}=1, \texttt{isttio}=1 and \texttt{nstbor} less than
or equal to the current Lagrangian iteration\\
\texttt{npstf} is initialised and updated automatically by the code,
its value is not to be modified by the user}

\motcle{npstft}{i}{positive integer}{0}{O}{L3}
{number of iterations during which boundary statistics have
been calculated
(the potential iterations during which unsteady
statistics have been calculated are counted in \texttt{npstft})\\
useful if \texttt{iensi3}=1\\
\texttt{npstft} is initialised and updated automatically by the code,
its value is not to be modified by the user}

\motcle{tstatp}{r}{positive real number}{\texttt{dtp}}{O}{L3}
{if the recording of the boundary statistics is steady, \texttt{tstatp}
contains the cumulated physical duration of the recording of the boundary
statistics\\
if the recording of the boundary statistics is unsteady, then
\texttt{tstat=dtp\index{dtp}} (it is the Lagrangian time step, because the
statistics are reset to zero at every time step)\\
useful if \texttt{iensi3}=1}
