Here is a list of all files with brief descriptions:

[detail level 1234]

▼ docs
► doxygen
► examples
bft_error_example.c
cavitation.h
cs_f_user_parameters.h
cs_head_losses.h
cs_lagrangian_particle_tracking_module.h
cs_porosity.h
cs_remarks.h
cs_user_boundary_conditions_ale.h
cs_user_boundary_conditions_examples.h
cs_user_extra_operations-nusselt_calculation.h
cs_user_extra_operations_examples.h
cs_user_initialization.h
cs_user_les_inflow.h
cs_user_mass_source_terms.h
cs_user_parameters.h
cs_user_physical_properties.h
cs_user_radiative_transfer.h
cs_user_source_terms-scalar_in_a_channel.h
cs_user_source_terms.h
cs_user_tabs.h
cs_var_dico.h
drift_coal_scalars.h
drift_scalars.h
richards.h
mainpage.h
▼ src
► alge
bilsca.f90	Wrapper to the function which adds the explicit part of the convection/diffusion terms of a transport equation of a scalar field $\varia$
bilscts.f90	Wrapper to the function which adds the explicit part of the convection/diffusion terms of a transport equation of a tensor field $\tens{\varia}$
bilscv.f90	Wrapper to the function which adds the explicit part of the convection/diffusion terms of a transport equation of a vector field $\vect{\varia}$
cs_balance_by_zone.c
cs_balance_by_zone.h
cs_benchmark.c
cs_benchmark.h
cs_blas.c
cs_blas.h
cs_bw_time_diff.c
cs_convection_diffusion.c
cs_convection_diffusion.h
cs_divergence.c
cs_divergence.h
cs_face_viscosity.c
cs_face_viscosity.h
cs_gradient.c
cs_gradient.h
cs_gradient_perio.c
cs_gradient_perio.h
cs_grid.c
cs_grid.h
cs_matrix.c
cs_matrix.h
cs_matrix_building.c
cs_matrix_building.h
cs_matrix_default.c
cs_matrix_default.h
cs_matrix_priv.h
cs_matrix_tuning.c
cs_matrix_tuning.h
cs_matrix_util.c
cs_matrix_util.h
cs_multigrid.c
cs_multigrid.h
cs_sles.c	Sparse linear equation solver driver
cs_sles.h
cs_sles_default.c
cs_sles_default.h
cs_sles_it.c
cs_sles_it.h
cs_sles_pc.c
cs_sles_pc.h
cs_sles_petsc.c	Handling of PETSc-based linear solvers
cs_sles_petsc.h
visort.f90
► apps
cs_check_syntax.c
cs_io_dump.c
cs_solver.c
► atmo
atchem.f90	Module for chemistry in the atmospheric module
atimbr.f90	Atmospheric Imbrication module. This module contains the data structure and subroutines to perform atmospheric imbrication or nesting of a CFD domain within a large scale meteorological field. Starting from a set of large scale meteological profiles (in the format of meteo files) an interpolation is performed for each boundary face both spatially and temporally (using Cressman method)
atincl.f90	Module for atmospheric models - main variables
atini0.f90	Initialisation of variable options for Code_Saturne atmospheric module in addition to what is done previously in iniini function
atini1.f90	Initialisation of variable options for the atmospheric module in addition to what is done in usipsu function
atiniv.f90	Initialisation of calculation variables for the atmospheric module, it is the counterpart of usiniv.f90. Initialise for example the meteorological field for each cell of the domain by interpolation of the data from the meteo file
atleca.f90	Reads initial aerosol concentration and number
atlecc.f90	Reads the chemistry profile data for the atmospheric chemistry
atlecm.f90	Reads the meteo profile data for the atmospheric module
atmcls.f90	Compute u*, q0, e0, (momentum, sensible heat and latent heat fluxes) for a non neutral atmospheric surface layer using the explicit formula developed for the ECMWF by Louis (1982)
atmsol.f90	Build constants and variables to describe the ground model
atmstd.f90	Compute standard atmospheric profile
atphyv.f90	Functions that compute physical variables for each cell for the atmospheric module
atprke.f90	Modify the $k-\varepsilon$ turbulence model formulation (cf.: turbke) for the atmospheric module
atprop.f90	Add if needed the variables fields for temperature and liquid water
atr1vf.f90	1D Radiative scheme - Compute radiative fluxes
atsoil.f90	Module for the atmospheric soil model adapted to the IGN "land use" file format
attssc.f90	Additional right-hand side source terms for scalar equations taking into account dry and humid atmospheric variables
attycl.f90	Automatic boundary conditions for atmospheric module (based on meteo file)
atvarp.f90	ATMOSPHERIC AEROSOL CHEMISTRY MODULE add necessary variables
chem_luscheme1.f90	Routines for atmospheric chemical scheme 1
chem_luscheme2.f90	Routines for atmospheric chemical scheme 2
chem_luscheme3.f90	Routines for atmospheric chemical scheme 3
chem_luscheme_siream.f90	Routines for atmospheric chemical and aerosols scheme 3
chem_solvelu.f90	Solver of AX=B with LU decomposition of A for atmospheric chemical systems
chem_source_terms.f90	Computes the explicit chemical source term for atmospheric chemistry in case of a semi-coupled resolution
compute_gaseous_chemistry.f90	Calls the rosenbrock resolution for atmospheric chemistry
compute_siream.f90	Computation of atmospheric aerosol chemistry
cs_at_plugin.c	Plugin to dynamically load(*.so) the aerosol model (SIREAM)
cs_at_plugin.h	Plugin to get aerosol and compute_coagulation_coefficient functions from SIREAM library (ENPC - INRIA - EDF R&D)
etheq.f90	Atmospheric module - humid atmosphere variables
intprf.f90	Temporal and z-axis interpolation for meteorological profiles
kinrates.f90	Calls the computation of reaction rates for atmospheric chemistry
nuclea.f90	Atmospheric module - humid atmosphere - cloud droplet nucleation
rayigc.f90	1D Radiative scheme - IR CO2 + O3 absorbtion
rayir.f90	1D Radiative scheme - IR flux divergence profile and downward flow to the ground
rayive.f90	1D Radiative scheme - IR H20 and dimere absorption
rayso.f90	1D Radiative scheme - Solar flux
raysze.f90	1D Radiative scheme - Solar data + zenithal angle)
roschem.f90	Rosenbrock solver for atmospheric chemistry
satfun.f90	Computes the saturation mixing ratio (kg/kg) of water in the atmosphere
siream.f90	Module for atmospheric aerosol chemistry in the atmospheric module
solcat.f90	Atmo. - Ground level parameters computed from a "Land use" file
soliva.f90	Atmospheric soil module - soil variables initialisation
solmoy.f90	Atmospheric soil module - Initialize ground level parameters from land use
solvar.f90	Atmospheric soil module - Compute ground level variables
spefun.f90	Atmospheric module - Module for specific math functions
► base
addfld.f90	Add additional fields based on user options
alaste.f90	Module for ALE with Code_Aster coupling
albase.f90	Module for Arbitrary Lagrangian Eulerian method (ALE)
alelav.f90	This subroutine performs the solving of a Poisson equation on the mesh velocity for ALE module
alemav.f90	This subroutine updates the mesh in the ALE framework
alstru.f90	Module for ALE structure movement with internal coupling
altycl.f90	Boundary condition code for the ALE module
b_h_to_t.f90
b_t_to_h.f90	Convert enthalpy to temperature at boundary
c_h_to_t.f90	Convert enthalpy to temperature at cells
calhyd.f90	Poisson equation resolution for hydrostatic pressure: $\divs ( \grad P ) = \divs ( f )$
caltri.f90
catsma.f90	Implicit and explicit sources terms from sources mass computation
catsmt.f90	Compute explicit and implicit source terms coming from mass source
catsmv.f90	Compute explicit and implicit source terms coming from mass source
cavitation.f90	Module for cavitation modeling
clca66.f90
clpsca.f90	This subroutine clips the values of a given scalar or variance
clptrg.f90	Boundary conditions for rough walls (icodcl = 6)
clptur.f90	Boundary conditions for smooth walls (icodcl = 5)
clsyvt.f90	Symmetry boundary conditions for vectors and tensors
codits.f90	This function solves an advection diffusion equation with source terms for one time step for the variable
coditts.f90	This function solves an advection diffusion equation with source terms for one time step for the symmetric tensor variable $\tens{\variat}$
coditv.f90	This function solves an advection diffusion equation with source terms for one time step for the vector variable $\vect{a}$
condensation_source_terms.f90	Explicit sources terms from sources condensation computation
condli.f90	Translation of the boundary conditions given by cs_user_boundary_conditions in a form that fits to the solver
copain_model.f90	The COPAIN correlations used to approximate the condensation source term and the thermal exchange coefficient to impose at the wall where condensation occurs
cou1di.f90
cou1do.f90
coupbi.f90
coupbo.f90
covofi.f90	This subroutine performs the solving the convection/diffusion equation (with eventually source terms and/or drift) for a scalar quantity over a time step
cplsat.f90	Module for code/code coupling
cptssy.f90
cpvosy.f90
cregeo.f90
cs_ale.c
cs_ale.h
cs_all_to_all.c
cs_all_to_all.h
cs_array_reduce.c
cs_array_reduce.h
cs_assert.h
cs_ast_coupling.c
cs_ast_coupling.h
cs_base.c
cs_base.h
cs_base_fortran.c
cs_base_fortran.h
cs_block_dist.c
cs_block_dist.h
cs_block_to_part.c
cs_block_to_part.h
cs_boundary_conditions.c
cs_boundary_conditions.h
cs_c_bindings.f90	Definition of C function and subroutine bindings
cs_calcium.c
cs_calcium.h
cs_control.c
cs_control.h
cs_coolprop.cxx
cs_coupling.c
cs_coupling.h
cs_crystal_router.c
cs_crystal_router.h
cs_defs.c
cs_defs.h
cs_eos.cxx
cs_ext_neighborhood.c
cs_ext_neighborhood.h
cs_f_interfaces.f90	Definition of explicit interfaces for Fortran functions
cs_fan.c
cs_fan.h
cs_field.c
cs_field.h
cs_field_operator.c
cs_field_operator.h
cs_field_pointer.c
cs_field_pointer.h
cs_file.c
cs_file.h
cs_fp_exception.c
cs_fp_exception.h
cs_gas_mix_initialization.f90	Initialization of calculation variables for gas mixture modelling in presence of the steam gas or another gas used as variable deduced and not solved
cs_gas_mix_physical_properties.f90	This subroutine fills physical properties which are variable in time for the gas mixtures modelling with or without steam inside the fluid domain. In presence of steam, this one is deduced from the noncondensable gases transported as scalars (by means of the mass fraction of each species)
cs_halo.c
cs_halo.h
cs_halo_perio.c
cs_halo_perio.h
cs_interface.c
cs_interface.h
cs_io.c
cs_io.h
cs_log.c
cs_log.h
cs_log_iteration.c	Log field and other array statistics at relevant time steps
cs_log_iteration.h
cs_log_setup.c	Setup info at the end of the setup stage
cs_log_setup.h
cs_map.c
cs_map.h
cs_math.c
cs_math.h
cs_measures_util.c
cs_measures_util.h
cs_mesh_tagmr.f90	The subroutine is used to generate the 1-D mesh and initialize the temperature field of the thermal model coupled with condensation model
cs_metal_structures_tag.f90	The 0-D thermal model to compute the temperature at the metal structures wall and pass to the volume condensation modelling to be able to model the metal structures effects. This metal structures temperature computed is passed to the volume condensation model to estimate the heat flux at the metall structures wall where the condensation occurs
cs_numbering.c
cs_numbering.h
cs_nz_condensation.f90	Module for parameters options and physical properties of the condensation model using specific zones with different wall temperatures and material properties
cs_nz_tagmr.f90	Module for parameters options, numerical and physical properties of the thermal 1D model for each specific zone with condensation on the wall. The zones number is defined by the user with the subroutine : cs_user_nzones_boundary_mass_source_terms
cs_opts.c
cs_opts.h
cs_order.c
cs_order.h
cs_parall.c
cs_parall.h
cs_paramedmem_coupling.cxx
cs_parameters.c
cs_parameters.h
cs_part_to_block.c
cs_part_to_block.h
cs_physical_constants.c
cs_physical_constants.h
cs_physical_properties.c
cs_physical_properties.h
cs_post.c	Post-processing management
cs_post.h
cs_post_default.c
cs_post_default.h
cs_preprocess.c
cs_preprocess.h
cs_preprocessor_data.c
cs_preprocessor_data.h
cs_prototypes.h
cs_renumber.c
cs_renumber.h
cs_resource.c
cs_resource.h
cs_restart.c
cs_restart.h
cs_restart_default.c
cs_restart_default.h
cs_rotation.c
cs_rotation.h
cs_sat_coupling.c
cs_sat_coupling.h
cs_search.c
cs_search.h
cs_selector.c
cs_selector.h
cs_selector_f2c.f90
cs_sort.c
cs_sort.h
cs_stokes_model.c
cs_stokes_model.h
cs_syr4_coupling.c
cs_syr4_coupling.h
cs_syr_coupling.c
cs_syr_coupling.h
cs_system_info.c
cs_system_info.h
cs_tagmr.f90	Module for parameters options and physical properties of the 1-D thermal model coupled with condensation
cs_tagmri.f90	The 1D thermal model to compute the temperature to impose at the cold wall. This one is used by the COPAIN model to estimate the heat flux at the wall where the condensation occurs
cs_tagmro.f90	The 1D thermal model to compute the temperature to impose at the cold wall. This one is used by the COPAIN model to estimate the heat flux at the wall where the condensation occurs
cs_tagms.f90	Module for parameters options and physical properties of the 0-D thermal model used by the metal mass structures modelling coupled with specific condensation correlations
cs_thermal_model.c
cs_thermal_model.h
cs_time_moment.c	Temporal moments management
cs_time_moment.h
cs_time_plot.c
cs_time_plot.h
cs_time_step.c
cs_time_step.h
cs_timer.c
cs_timer.h
cs_timer_stats.c
cs_timer_stats.h
cs_tpar1d.c
cs_tpar1d.h
cs_turbomachinery.c
cs_turbomachinery.h
cs_wall_functions.c
cs_wall_functions.h
csc2cl.f90	Translation of the "itypfb(, ) = icscpl" condition
csc2ts.f90	Code-code coupling with source terms
csccel.f90	Exchange of coupling variables between to times of Code_Saturne thanks to boundary faces
cscfbr.f90	Exchange of variables for coupling two Code_Saturne intances with boundary faces
cscini.f90	Initialization of main variables for code_saturne / code_saturne coupling
csclli.f90
cscloc.f90	Coupling interfaces localization (with FVM)
cscpce.f90	Preparation of sending velocity variables for coupling between two instances of Code_Saturne via boundary faces. Received indformation will be transformed into boundary condition in subroutine csc2cl
cscpfb.f90	Preparation of sending variables for coupling between two instances of Code_Saturne via boundary faces. Received indformation will be transformed into boundary condition in subroutine csc2cl
csinit.f90
csopli.f90
csprnt.f90
cstnum.f90	Module for numerical constants
cstphy.f90	Module for physical constants
diffst.f90
dimens.f90	Module for dimensions
distpr.f90	Compute distance to wall by solving a 3d diffusion equation. Solve $\divs ( \grad \varia ) = -1$ with:
distpr2.f90	Compute distance to wall by a brute force geometric approach (serial only)
distyp.f90	This subroutine computes the dimensionless distance to the wall solving a transport equation
driflu.f90	Compute the modified convective flux for scalars with a drift
dttvar.f90	Compute the local time step and add the Courant and Fourier number to
dvvpst.f90	Standard output of variables on post-processing meshes (called after cs_user_extra_operations)
ecrava.f90
ecrhis.f90	Write plot data
ecrlis.f90
entsor.f90	Module for input/output
field.f90	Module for field-related operations
field_operator.f90	Module for field-based algebraic operations
findpt.f90	This subroutine looks for the nearest element to the position (xx, yy, zz) among the element of xyzcen array
fldini.f90
fldprp.f90	Properties definition initialization, according to calculation type selected by the user
fldtri.f90
fldvar.f90	Variables definition initialization, according to calculation type selected by the user
haltyp.f90
idrbla.f90
ihmpre.f90	Module for GUI parameter file flag We could avoid this module by querying a C structure
impini.f90
iniini.f90	Commons default initialization before handing over the user
initi1.f90	Commons initialization
initi2.f90	End of commons initialization
iniusi.f90
iniva0.f90	Computed variable initialization. The time step, the indicator of wall distance computation are also initialized just before reading a restart file or use the user initializations
inivar.f90	Initialization of calculation variables, time step and table that stores distance to the wall by the user (after reading a restart file)
iprbla.f90
lecamo.f90	Reading of restart file
lecamp.f90	Reading of main restart file
lecamx.f90	Reading of auxiliary restart file
majgeo.f90
memfin.f90
mesh.f90	Module for mesh-related arrays
metal_structures_copain_model.f90	The COPAIN modelling to estimate the heat and mass transfer associated to the steam condensation phenomena at each cell corresponding to the metal structures volume identified by geometric criteria
mmtycl.f90
modini.f90	Modify calculation parameters after user changes (module variables)
navstv.f90	Solving of NS equations for incompressible or slightly compressible flows for one time step. Both convection-diffusion and continuity steps are performed. The velocity components are solved together in once
newmrk.f90
numvar.f90	Module for variable numbering
optcal.f90	Module for calculation options
parall.f90	Module for basic MPI and OpenMP parallelism-related values
paramx.f90	Module for definition of general parameters
period.f90	Module for periodicity flags
phyvar.f90	This subroutine fills physical properties which are variable in time (mainly the eddy viscosity)
pointe.f90	Module for pointer variables
post.f90	Module for post-processing related operations
post_util.f90
precli.f90	Preparation of boudary conditions determination Boundary faces of precedent step are used. Except at first time step, where arrays itypfb and itrifb are undefined
predfl.f90	Update the convective mass flux before the Navier Stokes equations (prediction and correction steps)
predvv.f90	This subroutine performs the velocity prediction step of the Navier Stokes equations for incompressible or slightly compressible flows for the coupled velocity components solver
prehyd.f90	Compute an "a priori" hydrostatic pressure and its gradient associated before the Navier Stokes equations (prediction and correction steps navstv.f90)
prmoy0.f90
pthrbm.f90	Update the density $\rho^{n+1}$ with the $\rho^{n-\frac{1}{2}}$ density with the state law and a thermodynamic pressure $p_{ther}^{n+1} estimated from the integral over the total fluid domain of the mass conservation equation.$
ptrglo.f90
resopv.f90	This subroutine performs the pressure correction step of the Navier Stokes equations for incompressible or slightly compressible flows for the coupled velocity components solver
resvoi.f90	Solving the void fraction $\alpha$ for cavitation model
rotation.f90	Module for physical constants
scalai.f90	Resolution of source term convection diffusion equations for scalars in a time step
schtmp.f90
stdtcl.f90
strdep.f90
strhis.f90
strini.f90
strpre.f90
tdesi1.f90
tridim.f90	Resolution of incompressible Navier Stokes and scalar transport equations for a time step
tspdcv.f90
turbomachinery.f90
typecl.f90	Handle boundary condition type code (itypfb)
undscr.f90
varpos.f90	Variables location initialization, according to calculation type selected by the user
vericl.f90	Check boundary condition code
verini.f90
verlon.f90
vert1d.f90
visecv.f90	Computes the secondary viscosity contribution $\kappa -\dfrac{2}{3} \mu$ in order to compute: $\grad\left( (\kappa -\dfrac{2}{3} \mu) \trace( \gradt(\vect{u})) \right)$ with:
zufall.f90
► bft
bft_backtrace.c
bft_backtrace.h
bft_error.c
bft_error.h
bft_mem.c
bft_mem.h
bft_mem_usage.c
bft_mem_usage.h
bft_printf.c
bft_printf.h
► cdo
cs_advection_field.c
cs_advection_field.h
cs_cdo.c
cs_cdo.h
cs_cdo_bc.c
cs_cdo_bc.h
cs_cdo_connect.c
cs_cdo_connect.h
cs_cdo_main.c
cs_cdo_main.h
cs_cdo_quantities.c
cs_cdo_quantities.h
cs_cdo_toolbox.c
cs_cdo_toolbox.h
cs_cdofb_scaleq.c
cs_cdofb_scaleq.h
cs_cdovb_advection.c	Build discrete advection operators for CDO vertex-based schemes
cs_cdovb_advection.h
cs_cdovb_diffusion.c	Build discrete stiffness matrices and handled boundary conditions diffusion term in CDO vertex-based schemes
cs_cdovb_diffusion.h
cs_cdovb_scaleq.c
cs_cdovb_scaleq.h
cs_domain.c
cs_domain.h
cs_equation.c
cs_equation.h
cs_equation_priv.h
cs_evaluate.c
cs_evaluate.h
cs_groundwater.c
cs_groundwater.h
cs_hodge.c	Build discrete Hodge operators
cs_hodge.h
cs_param.c
cs_param.h
cs_property.c
cs_property.h
cs_quadrature.c
cs_quadrature.h
cs_reco.c
cs_reco.h
cs_sla.h
cs_sla_matrix.c
cs_walldistance.c
cs_walldistance.h
► cfbl
cfdivs.f90
cfdttv.f90
cfener.f90	Perform the solving of the convection/diffusion equation (with eventual source terms) for total energy over a time step. It is the third step of the compressible algorithm at each time iteration
cffana.f90	Computes the analytical flux at the boundary for Euler and Energy
cfini1.f90
cfiniv.f90	Initialisation of the variables if the compressible flow model is enabled
cfmsfp.f90
cfmspr.f90	Update the convective mass flux before the velocity prediction step. It is the first step of the compressible algorithm at each time iteration
cfphyv.f90	Computation of variable physical properties for the specific physics compressible
cfpoin.f90	Module for fuel combustion
cfprop.f90	Properties definition initialization for the compressible module, according to calculation type selected by the user
cfrusb.f90
cfvarp.f90	Variables definition initialization for the compressible module, according to calculation type selected by the user
cfxtcl.f90	Handle boundary condition type code (itypfb) when the compressible model is enabled
cs_cf_bindings.f90	Definition of C functions and subroutine bindings for compressible flow module
cs_cf_thermo.c
cs_cf_thermo.h
► cogz
coincl.f90	Module for gas combustion
coini1.f90
colecd.f90
coprop.f90
cothht.f90
covarp.f90
d3phst.f90	Specific physic subroutine: diffusion flame
d3pini.f90
d3pint.f90	Specific physic subroutine: diffusion flame
d3pphy.f90	Specific physic subroutine: diffusion flame
d3ptcl.f90
d3pver.f90
ebuini.f90
ebuphy.f90
ebutcl.f90
ebutss.f90
ebuver.f90
lwcgfu.f90
lwcini.f90
lwcphy.f90
lwctcl.f90
lwctss.f90
lwcurl.f90
lwcver.f90
pdflwc.f90
pdfpp3.f90
pdfpp4.f90
sootsc.f90	Specific physic subroutine: two equations soot model
yg2xye.f90	Compute molar and mass fractions of elementary species Ye, Xe (fuel, O2, CO2, H2O, N2) from global species Yg (fuel, oxidant, products)
► comb
cpincl.f90	Module for pulverized coal combustion
cplin1.f90
cplini.f90
cplph1.f90
cplphy.f90
cplpro.f90
cpltcl.f90
cpltss.f90
cpltsv.f90
cplvar.f90
cplver.f90
cplym1.f90
cppdf4.f90
cppdfr.f90
cpteh1.f90
cpthp1.f90
cs_coal_bcond.f90	Automatic boundary condition for pulverized coal combution
cs_coal_fp2st.f90
cs_coal_htconvers1.f90	Calculation of gas temperature Function with gas enthalpy and concentrations if mode = 1
cs_coal_htconvers2.f90	Calculating temperature of particles Function with enthalpy and concentrations if imode = 1
cs_coal_incl.f90	Module for coal combustion
cs_coal_masstransfer.f90	Calculation of the terms of mass transfer between the continous phase and the dispersed phase
cs_coal_noxst.f90
cs_coal_param.f90
cs_coal_physprop.f90	Specific physics routine: combustion of pulverized coal Calculation of $\rho$ of the mixture
cs_coal_physprop1.f90	Calculation of the physic propeties in gaseous phase
cs_coal_physprop2.f90	Calculation of the physical properties of the dispersed phase (classes of particules)
cs_coal_prop.f90	Purpose:
cs_coal_radst.f90
cs_coal_readata.f90
cs_coal_scast.f90	Specific physic routine: pulverized coal flame Souce terms have to be precised for a scalar PP on a step of time
cs_coal_thfieldconv1.f90	Calculation of the gas temperature Function with gas enthalpy and concentrations
cs_coal_thfieldconv2.f90	Calculation of the particles temperature Function with the solid enthalpy and concentrations
cs_coal_varini.f90
cs_coal_varpos.f90
cs_coal_verify.f90
cs_fuel_bcond.f90	Automatic boundary conditions Fuel combustion
cs_fuel_fp2st.f90
cs_fuel_htconvers1.f90	Calculation of the gas enthalpy. Function with gaz enthalpy and concentrations, if mode = 1
cs_fuel_htconvers2.f90	Calculation of the temperature of particles Function with enthalpy and concentrations if imode = 1
cs_fuel_incl.f90	Module for heavy fuel oil combustion
cs_fuel_masstransfer.f90	Calcultaion of mass transfer terms between the contineous phase and the dispersed phase
cs_fuel_noxst.f90
cs_fuel_param.f90
cs_fuel_physprop.f90	Specific physic routine: pulverized coal combustion. Calculation of $\rho$ of the mixture
cs_fuel_physprop1.f90	Calculation of physic properties of the gaseous phase
cs_fuel_physprop2.f90	Calculation of the physical properties of the dispersed phase
cs_fuel_prop.f90	Define state variables for fuel combustion
cs_fuel_radst.f90
cs_fuel_readata.f90
cs_fuel_scast.f90	Specific physic routine: fuel oil flame. We indicate the source terms for a scalar PP on a step time
cs_fuel_thfieldconv1.f90	Calculation of the gas temperature Function with the gas enthalpy and concentrations
cs_fuel_thfieldconv2.f90	Calculation of the particles temperature Fonction with the fuel enthalpy and concentrations
cs_fuel_varini.f90
cs_fuel_varpos.f90
cs_fuel_verify.f90
cs_gascomb.f90
cs_physical_properties_combustion_drift.f90	Definition of physical variable laws for combustion with a drift
► ctwr
cs_ctwr.c
cs_ctwr.h
cs_ctwr_air_props.c
cs_ctwr_air_props.h
cs_ctwr_f2c.f90
cs_ctwr_halo.c
cs_ctwr_halo.h
cs_ctwr_mesh.c
cs_ctwr_mesh.h
ctincl.f90
ctini1.f90
ctiniv.f90
ctphyv.f90
cttssc.f90
ctvarp.f90
► darc
daini1.f90	Initialize global settings for darcy module
darcy_module.f90	Module for Darcy calculation options
richards.f90	This routine solves the Richards equation, then compute the new velocities deducted from the gradients of hydraulic head and from the permeability. These velocities are used for post-processing, calculation of dispersion coefficients, convergence criterion of Newton scheme... but not for transport. In order to ensure the exact conservation of mass, the mass fluxes are computed following the procedure of the standard subroutine resopv (see theory guide)
► elec
cs_elec_bcond.f90
elflux.f90
elincl.f90	Module for electric arcs
elini1.f90
eliniv.f90
ellecd.f90
elphyv.f90
elprop.f90
elreca.f90
elthht.f90
eltssc.f90
elvarp.f90
elveri.f90
► fvm
fvm_box.c
fvm_box.h
fvm_box_priv.h
fvm_box_tree.c
fvm_box_tree.h
fvm_convert_array.c
fvm_convert_array.h
fvm_defs.c
fvm_defs.h
fvm_group.c
fvm_group.h
fvm_hilbert.c
fvm_hilbert.h
fvm_io_num.c
fvm_io_num.h
fvm_morton.c
fvm_morton.h
fvm_neighborhood.c
fvm_neighborhood.h
fvm_nodal.c
fvm_nodal.h
fvm_nodal_append.c
fvm_nodal_append.h
fvm_nodal_extract.c
fvm_nodal_extract.h
fvm_nodal_extrude.c
fvm_nodal_extrude.h
fvm_nodal_from_desc.c
fvm_nodal_from_desc.h
fvm_nodal_order.c
fvm_nodal_order.h
fvm_nodal_priv.h
fvm_nodal_project.c
fvm_nodal_project.h
fvm_nodal_triangulate.c
fvm_nodal_triangulate.h
fvm_periodicity.c
fvm_periodicity.h
fvm_point_location.c
fvm_point_location.h
fvm_selector.c
fvm_selector.h
fvm_selector_postfix.c
fvm_selector_postfix.h
fvm_tesselation.c
fvm_tesselation.h
fvm_to_catalyst.cxx
fvm_to_catalyst.h
fvm_to_ccm.c
fvm_to_ccm.h
fvm_to_cgns.c
fvm_to_cgns.h
fvm_to_ensight.c
fvm_to_ensight.h
fvm_to_ensight_case.c
fvm_to_ensight_case.h
fvm_to_med.c
fvm_to_med.h
fvm_to_medcoupling.cxx
fvm_to_medcoupling.h
fvm_trace.c
fvm_trace.h
fvm_triangulate.c
fvm_triangulate.h
fvm_writer.c
fvm_writer.h
fvm_writer_helper.c
fvm_writer_helper.h
fvm_writer_priv.h
► gui
cs_gui.c
cs_gui.h
cs_gui_boundary_conditions.c
cs_gui_boundary_conditions.h
cs_gui_conjugate_heat_transfer.c
cs_gui_conjugate_heat_transfer.h
cs_gui_mesh.c
cs_gui_mesh.h
cs_gui_mobile_mesh.c
cs_gui_mobile_mesh.h
cs_gui_output.c
cs_gui_output.h
cs_gui_particles.c
cs_gui_particles.h
cs_gui_radiative_transfer.c
cs_gui_radiative_transfer.h
cs_gui_specific_physics.c
cs_gui_specific_physics.h
cs_gui_util.c
cs_gui_util.h
cs_gui_variables.h
► lagr
cs_lagr_clogging.c
cs_lagr_clogging.h
cs_lagr_dlvo.c
cs_lagr_dlvo.h
cs_lagr_extract.c	Extract information from lagrangian particles
cs_lagr_extract.h
cs_lagr_perio.c
cs_lagr_perio.h
cs_lagr_restart.c
cs_lagr_restart.h
cs_lagr_roughness.c
cs_lagr_roughness.h
cs_lagr_tracking.c
cs_lagr_tracking.h
cs_lagr_utils.c
cs_lagr_utils.h
diverv.f90
lagadh.f90
lagaff.f90
lagcar.f90
lagcli.f90
lagcou.f90
lagdcl.f90
lagdep.f90
lagdif.f90
lagdim.f90	Module for Lagrangian dimensions
lageje.f90
lagent.f90
lageqp.f90
lages1.f90
lages2.f90
lagesd.f90
lagesp.f90
laggeo.f90
laggra.f90
laghis.f90
laghlo.f90	Define Head losses to take into account deposit in the flow
lagich.f90
lagidp.f90
lagimp.f90
lagini.f90
lagipn.f90
lagitf.f90
lagitg.f90
lagitp.f90
laglec.f90
laglis.f90
lagnew.f90
lagopt.f90
lagout.f90
lagpar.f90	Module for Lagrangian model (parameters)
lagphy.f90
lagpoi.f90
lagprj.f90
lagran.f90	Module for Lagrangian model
lagres.f90
lagrus.f90
lagsec.f90
lagsta.f90
lagstf.f90
lagswe.f90
lagtmp.f90
lagune.f90
porcel.f90	This routine permits to calculate the porosity in wall-normal cells from the mean deposit height (which is only known at the boundary faces)
precdi.f90	Management of the injection of particles formed by precipitation
precst.f90
► mei
mei_evaluate.c	Build an interpreter for a mathematical expression
mei_evaluate.h	Build an interpreter for a mathematical expression
mei_hash_table.c	Hash table, intended to provide a symbol table
mei_hash_table.h	Hash table, intended to provide a symbol table
mei_math_util.c	Provides mathemathical functions facilities
mei_math_util.h	Provides mathemathical functions facilities
mei_node.c	Nodal structure of the interpreter
mei_node.h	Nodal structure of the interpreter
mei_parser.c
mei_parser.h
mei_parser_glob.c	Define global variables useful for the mathematical expression parsing
mei_parser_glob.h	Define global variables useful for the mathematical expression parsing
mei_scanner.c
► mesh
cs_join.c
cs_join.h
cs_join_intersect.c
cs_join_intersect.h
cs_join_merge.c
cs_join_merge.h
cs_join_mesh.c
cs_join_mesh.h
cs_join_perio.c
cs_join_perio.h
cs_join_post.c
cs_join_post.h
cs_join_set.c
cs_join_set.h
cs_join_split.c
cs_join_split.h
cs_join_update.c
cs_join_update.h
cs_join_util.c
cs_join_util.h
cs_mesh.c
cs_mesh.h
cs_mesh_bad_cells.c
cs_mesh_bad_cells.h
cs_mesh_builder.c
cs_mesh_builder.h
cs_mesh_coherency.c
cs_mesh_coherency.h
cs_mesh_connect.c
cs_mesh_connect.h
cs_mesh_from_builder.c
cs_mesh_from_builder.h
cs_mesh_halo.c
cs_mesh_halo.h
cs_mesh_location.c
cs_mesh_location.h
cs_mesh_quality.c
cs_mesh_quality.h
cs_mesh_quantities.c
cs_mesh_quantities.h
cs_mesh_save.c
cs_mesh_save.h
cs_mesh_smoother.c
cs_mesh_smoother.h
cs_mesh_thinwall.c
cs_mesh_thinwall.h
cs_mesh_to_builder.c
cs_mesh_to_builder.h
cs_mesh_warping.c
cs_mesh_warping.h
cs_partition.c
cs_partition.h
► pprt
ppcabs.f90
ppcpfu.f90	Module for specific physics common variables between combustion of pulverized coal and heavy fuel
ppincl.f90	General module for specific physics
ppini1.f90
ppinii.f90
ppiniv.f90
ppinv2.f90
pplecd.f90
pppdfr.f90	Specific physic subroutine: Calculation of rectangle-Dirac pdf parameters
ppphyv.f90	These subroutineS fill physical properties which are variable in time for the dedicated physics modules (BEFORE and AFTER the user surbroutines)
ppppar.f90	General module for specific physics containing common parameters
ppprcl.f90
ppprop.f90
pptbht.f90
ppthch.f90	Module for specific physics thermophysical data
pptssc.f90
pptycl.f90	Boundary conditions for specific physics modules
ppvarp.f90
► rayt
cs_radiation_solver.c
cs_radiation_solver.h
radf08.f90	Subroutine of the ADF radiation model
radf50.f90	Subroutine of the ADF radiation model
radiat.f90	Module for Radiation
rafsck.f90	This subroutine is part of the FSCK radiation model
raycli.f90	Compute wall temperature for radiative transfer, and update BCs
raycll.f90
raydak.f90
raydir.f90
raydom.f90
raylec.f90
rayopt.f90
rayout.f90
raypar.f90
rayprp.f90	Properties definitions for radiative model
raypun.f90
raysca.f90
raysol.f90
rmodak.f90
► turb
clipke.f90
clipsa.f90
clpalp.f90	Clipping of alpha in the framwork of the Rij-EBRSM model
clprij.f90
clpv2f.f90
cs_les_filter.c
cs_les_filter.h
cs_les_inflow.c
cs_les_inflow.h
cs_turbulence_bc.c
cs_turbulence_bc.h
cs_turbulence_model.c
cs_turbulence_model.h
divrit.f90	This subroutine perform add the divergence of turbulent flux to the transport equation of a scalar
resalp.f90	Solving the equation on alpha in the framwork of the Rij-EBRSM model. (written from the equation of $\overline{f})$
reseps.f90	This subroutine performs the solving of epsilon in $R_{ij} - \varepsilon$ RANS turbulence model
resrij.f90	This subroutine performs the solving of the Reynolds stress components in $R_{ij} - \varepsilon$ RANS (LRR) turbulence model
resrij2.f90	This subroutine performs the solving of the coupled Reynolds stress components in $R_{ij} - \varepsilon$ RANS (LRR) turbulence model
resrit.f90	This subroutine perform the solving of the transport equation of the turbulent heat fluxes
resssg.f90	This subroutine performs the solving of the Reynolds stress components in $R_{ij} - \varepsilon$ RANS (SSG) turbulence model
resssg2.f90	This subroutine performs the solving of the Reynolds stress components in $R_{ij} - \varepsilon$ RANS (SSG) turbulence model
resv2f.f90	Resolution of source convection diffusion equations for $\phi$ and diffusion for $\overline{f}$ as part of the V2F phi-model
rijech.f90	Terms of wall echo for R_{ij} $var = R_{11} \: R_{22} \: R_{33} \: R_{12} \: R_{13} \: R_{23}$ $isou = 1 \: 2 \: 3 \: 4 \: 5 \: 6$
rijthe.f90	Gravity terms For $R_{ij}$ and $\epsilon$ $var = R_{11} \: R_{22} \: R_{33} \:R_{12} \:R_{23} \:R_{13} \:\varepsilon$
rijthe2.f90	Gravity terms For $R_{ij}$ $var = R_{11} \: R_{22} \: R_{33} \:R_{12} \:R_{23} \:R_{13}$
rotcor.f90	Computing rotation/curvature correction for eddy-viscosity models. The subroutine is called for the linear eddy viscosity RANS models, when the option irccor = 1 is verified
tsepls.f90	Calculation of the E term of the $\varepsilon$ equation (BL-V2/K model)
turbke.f90	Solving the $k - \epsilon$ for incompressible flows or slightly compressible flows for one time step
turbkw.f90	Solving the $k - \omega$ SST for incompressible flows or slightly compressible flows for one time step
turbsa.f90	Solving op the equation of $\tilde{\nu}$ , which is the scalar quantity defined by the Spalart-Allmaras model for 1 time-step
turent.f90	Calculation of turbulent inlet conditions for a circular duct flow with smooth wall
turrij.f90	Solving the $R_{ij} - \epsilon$ for incompressible flows or slightly compressible flows for one time step
vandri.f90	Imposition of an amortization of Van Driest type for the LES. $\nu_T$ is absorbed by $(1-\exp(\dfrac{-y^+}{d^+}))^2$ where is set at 26
visdyn.f90	Calculation of turbulent viscosity for a dynamic Smagorinsky LES model
vislmg.f90	Calculation of turbulent viscosity for a model of length of simple mixture
vissma.f90	Calculation of turbulent viscosity for a Smagorinsky LES model
vissst.f90	Calculation of turbulent viscosity for the $k - \omega$ SST model
visv2f.f90	Calculation of turbulent viscosity for the V2F-BL model
viswal.f90	Compute the turbulent viscosity for the WALE LES model
vor2cl.f90
vordep.f90
vorimp.f90
vorin0.f90
vorinc.f90	Module for vortex method for LES boundary conditions
vorini.f90
vorlgv.f90
vorpre.f90
vortex.f90
vorver.f90
vorvit.f90
► user
cs_user_atmospheric_model.f90
cs_user_boundary_conditions.f90	User subroutine which fills boundary conditions arrays (`icodcl`, `rcodcl`) for unknown variables
cs_user_boundary_conditions_ale.f90	User subroutine dedicated the use of ALE (Arbitrary Lagrangian Eulerian) Method:
cs_user_boundary_mass_source_terms.f90	Source terms associated at the boundary faces and the neighboring cells with surface condensation
cs_user_cdo.c	Set main parameters for the current simulation when the CDO kernel is used
cs_user_cdo_extra_op.c	Additional user-defined post-processing and analysis functions
cs_user_cdo_numerics.c	Set advanced parameters about the numerical schemes for each equation to solve. Useful to change the default behaviour
cs_user_coupling.c
cs_user_extra_operations.c
cs_user_extra_operations.f90	This function is called at the end of each time step, and has a very general purpose (i.e. anything that does not have another dedicated user subroutine)
cs_user_fluid_structure_interaction.f90
cs_user_head_losses.f90	Define Head losses
cs_user_initialization.f90	Initialize variables
cs_user_les_inflow.f90	Generation of synthetic turbulence at LES inlets
cs_user_mass_source_terms.f90	Mass source term user subroutine
cs_user_mesh.c
cs_user_metal_structures_source_terms.f90
cs_user_modules.f90	User-defined module: it allows to create any user array
cs_user_parameters.c
cs_user_parameters.f90
cs_user_particle_tracking.f90
cs_user_performance_tuning.c
cs_user_physical_properties.f90	Definition of physical variable laws
cs_user_porosity.f90	This function computes the porosity (volume factor $\epsilon$ when porosity module is activated (iporos = 1 in cs_user_parameters.f90)
cs_user_postprocess.c
cs_user_postprocess_var.f90	Output additional variables on a postprocessing mesh
cs_user_radiative_transfer.f90
cs_user_radiative_transfer_bcs.f90	User subroutine for input of radiative transfer parameters: boundary conditions
cs_user_solver.c
cs_user_source_terms.f90	Additional right-hand side source terms
cs_user_turbomachinery.c
usatch.f90	Routines for user defined atmospheric chemical scheme
usctdz.f90
uselrc.f90
ushist.f90
uslaen.f90
uslag1.f90
uslag2.f90
uspt1d.f90
usthht.f90
usvort.f90
usvosy.f90

Purpose: