
Release 4.2.0 (Dec 23 2015)
===========================

User changes
------------

 - Automatic initialization of the Turbulence for EBRSM and k-omega models.
   From a reference velocity (uref), the turbulence profiles are reset
   after the first iteration. The velocity magnitude is also changed
   so that the Reichard profile is imposed next to walls.
   Activate it with reinit_turb=1 (in usipsu).

 - Merge the bad cell and the mesh quality criterion for offsetting.

 - Merge general boundary temperature handling with the radiative
   "wall temperature", for unified logging and post-processing.

 - Added optional saving of scalar variable boundary values as fields
   (also done for temperature when a property).

 - GUI: "check mesh" option is replaced by a new "preprocessor view": when
   building a new case, the GUI only shows sections relative to mesh
   selection and preprocessing, showing only the steps necessary up to
   preprocessing. "Tools"  menu entries and toolbar icons allow switching
   from the preprocessing mode to the computation mode.
   This new view encourages users to use the "preprocessing" run type,
   which was previously available at the end of the GUI options,
   instead of the "check mesh" option, which did not handle batch runs
   or user subroutines.

 - Add boundary cell thickness computation to mesh quality criteria.

Physical modelling
------------------

 - Add gas mix thermo. and fix mass source term with the compressible module
   (internship of A. Menasria):
    * allow to select both gas mix (igmix) specific physics with compressible
      (icompf) spec. physics
    * add property field for deduced mass fraction (iddgas) and mixture molar
      mass (igmxml)
    * add a field pointer mapping for gas mix (mapping mix molar mass field)
    * add mapping of specific heat at constant volume field pointer
    * add one gas mix composed of helium, N2 and O2 (i.e. Helium+Air), O2 is the
      deduced species
    * add Sutherland behavior law for viscosity and thermal conductivity of
      gas mix (ivsuth option)
    * move setting of ieos from uscfx1 to usppmo
    * add thermo. relations for perfect gas mix in compressible thermo.
      (also for BCs),
    * igmix specific physics triggers switch of ieos to 3
    * treat conduction term in total energy equation correctly in gas mix
      (Cv depends on species)
    * fix mass source term in compressible (momentum source term coming from
      added mass has to be accounted for in simplified momentum equation during
      mass balance step).

 - Add precipitation/dissolution modeling for particle tracking.

 - Add the added-mass term in Lagrangian particle tracking (activate it
   with iadded_mass=1).

 - Add FSCK radiative model for coal combustion.
   Activate it in cs_user_parameters.f90 with imfsck=1.

 - Add a wall function for the velocity based on scalable wall function
   which is valid for both rough and smooth walls (activate it with
   iwallf = 6 in cs_user_parameters.f90).
   Moreover, the continuous wall function based on Van Driest (iwallf=5)
   is extended to Eddy Viscosity Models, and the use of roughness is allowed.
   For both wall functions, roughness must be specified in the field nammed
   "boundary_roughness" in cs_user_boundary_conditions.f90 for instance.

Numerics
--------

 - Add new preconditioning management layer to allow for use of multigrid
   as a preconditioner.

 - Extend weighted coefficients for lsq gradient calculation in case of
   anisotropic diffusion (this option can be enabled with the option
   iwgrec(ivar) = 1).

 - Add a coupled component solver for symmetric tensors for the Reynolds
   stress model (irijco=1).
   * convection diffusion brick for tensors
   * add a gradient of a tensor field
   * only iterative methode up to now, least square gradients not yet
     available
   * add the advection/diffusion matrix for a tensor field
   * adapt matrix tuning fill and Jacobi and other linear solvers
   * update rotation functions
   * restart from an uncoupled Rij tensor is possible
   * Daly Harlow and Shir models are available

 - CDO module:
   * Add reaction term to CDO module.
     Improve the computation of discrete Hodge op. when using
     conforming reconstruction function.
     Adapt the computation of the source term when using this kind of discrete
     Hodge operator.
   * Add time scheme and make some factorizations in vertex-based schemes.
     Add functionalities to cs_locmat_t structure.
   * Add convection for CDO vertex-based schemes.
     Add advection field along with its post-processing.
     Two advection operators are available related to the conservative or
     non-conservative form of the advection operator.
     Add post-processing of an equation (i.e. that of the related field).
   * Add different ways to enforce boundary conditions for CDO vertex-based
     schemes. Weak (Nitsche) enforcement, penalization and strong enforcement.
   * Add a domain and an equation structures
     Move cs_param_eq_t structure as a member of the cs_equation_t structure
   * Add the computation of the wall distance for CDO vertex-based schemes
   * Add the computation of the wall distance for face-based CDO schemes
   * Change the way user sets the paramters of a computation
   * Integrate PETSc solver calls
   * Add face-based CDO schemes for pure diffusion problem.

Architectural changes
---------------------

 - Add --compute-build option to "code_saturne run" command to allow choosing
   one of several compute builds at runtime.

 - Add "code_saturne submit" command to submit a batch job.
   The GUI now uses this to prepare data upon submission.

 - Some renames and simplifications in matrix fill types:
   * to make things more generic, CS_MATRIX_33_BLOCK* is replaced by
     CS_MATRIX_BLOCK*
   * tuning for blocks assumes 3x3 blocks, but a specific CS_MATRIX_BLOCK_D_66
     type is added (as a subcase of CS_MATRIX_BLOCK_D) to allow for specific
     tuning for RSM coupled component matrixes.

 - When using old (non-parallel) algorithm to compute wall distance, save
   distance in same array as for main algorithm.

 - Implement handling of point and element tags so as to ignore location
   on elements sharing tag.

 - Simplify Lagrangian particle tracking, removing a linked list.
   This is transparent for the user, except for a possible differences
   in particle numbering.

 - Major changes to all_to_all API, so as to make its usage easier.
  * new API is similar to cs_part_to_block / cs_block_to_part, so
    as to be aligned more with sparse or neighborhod collectives
    then Crystal Router in the future.
  * place Crystal Router code in separate files from cs_all_to_all,
    to allow lower-level use. Also simplify its usage, and make its
    data access logic higher level.

- Added cs_debug_wrapper.py debugger wrapper, to assist in running the code
  under a gdb-based debugger, under Valgrind, or a combination of the two.
  * replaces the "valgrind" only debug in the GUI advanced options for execution.
  * may also be used in standalone mode.

- Do not build with BLAS by default, as only MKL is used outside of unit tests, and
  using it requires providing its path to "--with-blas" anyways.


Release 4.1.0 (July 31 2015)
============================

User changes
------------

 - Renamed 'efforts' to 'stress', which should be less confusing.

 - Add simple fan effects modeling as explicit momentum source term in
   regions defined by fan characteristics.

 - Add a code icodcl=11, allowing to easily impose a boundary value
   consisting in an affine function of the next cell value
   (used at wall faces in the compressible module).

 - Add timer statistics and plots for different stages and operators.
   * Base timers for each time step (with initialization as time step 0)
     are now available in the timer_stats.csv file (or timer_stats.dat
     if the default format is changed).
   * Final performance data is also moved from listing to performance.log.

 - Allow condensation model to use zone-based definitions. The examples
   are updated so as to recommend the zone-based setup, though previous
   single-zone setups definitions remain compatible.

 - Add "--import-only" option to "code_saturne create" command so as to
   rebuild SaturneGUI and runcase scripts for a case which was copied
   from a different system.

 - Add higher level functions for turbulent boundary condition settings.
   This allows moving tests on the current turbulence model inside
   the user-callable functions, for more concise and safer programming.

Physical modelling
------------------

 - Add 2-scales wall function (with V. Driest mixing length) and its consistant
   wall function on scalars (keyword iwallf in the doc.).

 - Changes in Lagrangian Particle tracking.
   * modification of multi-layer model (iclogst = 1)
   * compute porosity in each cell based on mean deposition height only
     at boundary faces (porcel.f90)
   * influence of deposited layers on the flow (iflow = 1 option); addition of
     laghlo.f90 to compute the head loss due to deposition based on porosity)
   * remove lagbar.f90 (energy barrier now computed by cs_lagr_barrier for
     smooth wall/irough = 0, and cs_lagr_roughness_barrier for rough wall/
     irough = 1).

 - Add stiffened gas thermodynamic law for the compressible module (ieos=2).
   Two new parameters are accessible in the user subroutine uscfx2:
   gammasg ("pseudo" specific heat ratio) and psginf (infinite pressure).

 - Add ADF models for radiative transfers.

Numerics and linear solvers
---------------------------

 - Add vertex-based CDO (Compatible Discrete Operator) numerical scheme
   for diffusion problems. This is a first step, and does not handle
   parallelism yet. Integration with the rest of the code will be improved
   progressively.

 - Change multigrid default settings based on recent performance benchmarks.

 - Add 3-layer conjugate directions (residual) algorithm for non-symmetric
   linear systems (this algorithm was used in older EDF codes, and is
   different from the "standard" conjugate residual, which is limited to
   Hermitian matrixes).

 - Add support for using PETSc in linear solvers.

 - Convergence of linear solvers may now be plotted using CSV files.
   When solver verbosity is high, residues are not printed anymore
   (except in case of non-convergence), as plotting provides the same
   info in a more usable manner.

Architectural changes
---------------------

 - Add --sig-defaults option to cs_solver executable to allow use of
   default signal handlers.

 - Only trap floating-point exceptions by default for code compiled in
   debug mode, to avoid interfering with optimizer speculation.
   Exception trapping can be enabled or disabled locally using the
   cs_fp_exception_...() functions.

- Remove support for some older MPI libraries or process managers
  (which can still be used if needed using post-install settings).

- Complete Python 3 compatibility, except for builds with SALOME support
  (as the SALOME platform is not yet Python-3 compatible).

- Refactor EnSight, MED and CGNS output, replacing slice by block logic.
  The fvm_gather_...(*) API is now removed, and using parallel APIs
  for MED and CGNS should now be relatively straightforward.


Release 4.0.0 (April 30 2015)
=============================

Changes
-------

- Added boundary condition to flow mapping (feedback) functionnality
  (see boundary_conditions_map and boundary_conditions_mapped_set functions).

- By default, do not force use of an iterative gradient reconstruction method
  for pressure gradients, or other gradients deriving from a potential.
  To force it, a negative value of the IMRGRA keyword may be used.

- Coprocessing: if the main (default) writer uses Catalyst output, ignore
  joining output and use EnSight Gold format for joining and error writers
  if no matching Python script is found, to avoid uneeded abort.

- Turbomachinery modeling:
  * enable multiple rotors for rotor-stator model based on mesh joining.

- Generalize double backward implicit Euler time scheme for all variables.
  It can be activated with the keyword ibdtso(ivar) = 1.

- Add a "slope_test_upwind_id" field keyword, allowing postprocessing output
  of the contribution of slope tests to convected variables.

- Add a new dilatable (non conservative) algorithm for fire modelling.
  Activate it with idilat=4 (the formulation is in div(u) instead of
  div(rho u)). You can access to the previous dedicated algorithm by
  setting idilat to 5.

- Add L2 time normalized residual to the log.

- Major changes for solvers:
  * Unify handling of linear solvers, so as to allow finer user control, and
    enable future additions of solver options and user-defined or external
    solvers.
  * Add Block Gauss-Seidel linear solver, which may be accelerated for "upwind"
    type systems by a matrix line ordering. This is used (by default) for the
    DOM radiation module, using the ordering defined by the radiation direction,
    and leads to a factor of 2 to 4 improvement over the Jacobi solver for this
    case (tested on a small number of MPI ranks).
  * Single-reduction conjugate gradient is now an option rather than a separate
    solver. This allows switching automatically from one to the other based on
    computation vs. communication cost.
  * Add BiCGstab2 linear solver.
  * Change default solver for pure diffusion problems (from Conjugate gradient to
    multigrid solver).

- Add a new experimental module for Darcy flows. It can be
  activated with the keyword usppmo(idarcy) = 1.
  This path includes new developments to improve reconstruction gradient
  calculation with heterogeneous diffusion coefficients. This feature is only
  available for standard LSQ gradients and can be activated with
  the keyword iwgrec(ivar) = 1.

- Add drift modelling for coal combustion, and clean up the module:
  * Now, the enthalpy of the continuous phase (gas phase, h1) is transported
    rather than deduced (to be precises, X1.h1 is transported)
  * The convective flux for the gas phase is deduced from the convective fluxes
    of the particle classes and the convective flux of the bulk: therefore, the
    algorithm is fully conservative over time and space.
    (Note that the conservatism is obtained mainly due to having upwind schemes;
     transport equation on X1 with convective field V1 and
     transport equation on h1 with convective field X1.V1
     is equivalent to transport equation of X1.h1 with convective field V1...)
  * Some coal combustion fields are renamed
  * A model with a transported particle velocity per class is added (in fact,
    this velocity is handled as 3 scalars).
  * Correct cs_user_initialization-unified_combustion_coal.f90 user example.

- Add a condensation wall model.

- Added cell and face renumbering options to try to improve performance.

Architectural changes
---------------------

- New PLE (parallel location and exchange) library API, allowing new locator
  features and algorithm versioning. This requires an update on the Syrthes
  side for conjugate heat transfer.

- The preprocessor now uses integers of the same size as the kernel's
  global numbers (cs_gnum_t). This allows handling of meshes above
  200 million cells, at the cost of about 50% higher memory usage for
  this stage (unlesss the code is configured  with --disable-long-gnum).

- Remove rtp and rtpa arrays. Variables are stored with field
  structure owning its value arrays.

- Rename and merge user subroutines:
  * User scalars are not declared in usinsc (in cs_user_parameters.f90) anymore,
    but in cs_user_model (in cs_user_parameters.c). They are not named based
    on their number, but both their name and label is determined by the user.
    This should make it easier to combine data setups.
  * Remove the cs_user_field_parameters subroutine from cs_user_parameters.f90.
    user code in that subroutine may now be placed in usipsu or usipes.
    The usipsc subroutine is also removed, and scalar variable diffusivity
    behavior may be activated through usipsu.
  * merge (usebu1, uslwc1, usd3pt1, uscpl1, user_coal_ini1, user_fuel_ini1)
          in cs_user_combustion (in cs_user_paramters.f90)
  * split and rename usray1 in cs_user_radiative_transfer
    (in cs_user_parameters.f90)
          (Note that the declaration of the use of radiative transfer is in
                usppmo, as the other specific physics models)
  * rename usray2 in cs_user_radiative_transfer_bcs
  * merge usalin into usipph (in cs_user_parameters.f90)
  * rename ustsma into cs_user_mass_source_terms
  * rename uskpdc into cs_user_head_losses
  * remove the usipgl subroutine from cs_user_parameters.f90.
    Specific, model oriented options are defined in usipph, general options
    in usipsu.

- Lagrangian particle data is now shared between Fortran and C parts.
  Fortran arrays have been replaced by pointers, which map to the C data.
  arrays itepa, tepa, ettp, and ettpa are replaced respectively by pointers
  ipepa, pepa, eptp, eptpa, which use interleaved data; for example, the
  equivalent of itepa(np,jisor) would now be ipepa(jisor,np).
  Allocation is automatic, and npmabs is no more.

- When building with both lib CCM-IO and CGNS, do not try to use CGNS's ADF
  library for CCM-IO. This used to work in the past, but now leads to failure
  opening CCM files. The change might lead to issues for such builds when using
  ADF output for CGNS files, but HDF5 is now the default for CGNS (where
  available), and the hdf2adf and adf2hdf tools of the CGNS library suite allow
  conversion, so this should not be an issue. Builds with both libraries with
  linkers not allowing or configured to allow multiple definitions might be
  an issue.

- Restart files now use a new section naming scheme, at least for field data.
  this allows more automated handling of variables and properties in
  checkpoint/restart.

- Major indexing change: the mesh connectivity arrays (in cs_mesh_t
  structures, i_face_cell, b_face_cell, i_face_vtx_idx, i_face_vtx_lst,
  b_face_vtx_idx, and b_face_vtx_lst) now use 0-based indexing.
  This simplifies expressions in C code, but may break existing C code
  referencing those arrays. On the Fortran side, ifacel, ifabor, ipnfac,
  nodfac, ipnfbr, and nodfbr are no longer arrays, but elemental functions,
  which add 1 to the C array values, so as to make this transparent to the
  user. As most accesses are now in C, and the ifacel and ifabor functions are
  defined as "elemental pure" in the mesh module, the performance impact
  should not be significant.

- Some arrays for which there is a field keyword equivalent, such as ivarpr,
  are replaced by functions, which allow similar read-only access, but not
  modification, which must be done through the field API.

Bug fixes
---------

- Face mean secondary viscosity is now computed consistantly with face mean
  viscosity (namely harmonic if imvisf equal to 1).

- Fix bug introduced in rev. 4491 (before release of 3.0.0):

  - in rev 4491, the call to specific physics laws was moved from BEFORE
    the user call to AFTER the user call, which was only needed for the
    compressible module, whereas it impinges ALL the specifics physics.
  - therefore ppphyv is split into two.
  - WARNING: this change MAY impige all the specific physics
    (Atmospheric, Electric Arcs, Combustion, etc.)

- Many more bug changes (see ChangeLog for details)


Release 3.3.0 (16 May 2014)
===========================

Changes
-------

- Add 2 order backward Euler scheme in time for velocity prediction.
  Set ibdtso = 2 in usipsu to activate it.

- Add cavitation models. See the documentation (theory, user, Doxygen) for more details.
  You can activate it in cs_user_parameters.f90 with icavit=1.

- Add the Shir model for the turbulent diffusion of the second moment turbulence models
  (Rij and epsilon, isotropic diffusion). Available with the idirsm=0.

- Enable use of sparse matrix-vector tuning mechanism in regular calculations.
  Automatic tuning or variant selection may be done using the
  cs_user_matrix_tuning() function, in cs_user_performance_tuning.c.

- For non-batch systems, handling of the number of MPI ranks is
  based on a "code_saturne run" option, --nprocs, and is set in the
  runcase file, not in the XML file anymore.

- For couplings, runcase_coupling is replaced by a standard runcase,
  mechanism, using "code_saturne run --coupling coupling_parameters.py",
  where coupling_parameters.py contains the domains dictionnary previously
  in runcase_coupling. This allows unifying the handling of "code_saturne run"
  options.

- Rewrite of temporal moments handling. Moments handling is now more modular,
  and allows for variances in addition to means. Also, numerically stable recurrence
  relations are used to update moments, whose values are now directly usable at any
  given time. Weight accumulators are handled inside the module, and not seen as
  fields anymore. Also, support for user functions is added.
  Currently, this is mapped to the legacy data setup, and tested only in this
  context, but the added functionality will be exposed with future changes in
  case setup.

- Lagrangian module: Improvements in roughness and resuspension models
   * added a user keyword 'irough' for roughness surface (calculation of the
     energy barrier in the case of rough wall)
   * consideration of the electrostatic force in the adhesion force
     for the resuspension
   * mass flux update for particles rolling on the wall

- Ensure postprocessing of symmetric tensors for EnSight and Catalyst is consistent
  with {xx, yy, zz, xy, yz, xz} internal component representation.

- Update some external package versions for automatic installer.

Architectural changes
---------------------

- Remove rtp, rtpa and propce in user subroutines API. The access to the
  variables and the properties is carry out using field structure.

- Velocity field is now created as "owner field" in C (removed from rtp
  and rtpa). Velocity is now fully interleaved.

- Ensure only platform-independent files are installed to datarootdir
  (either as defined by ${prefix}/share or as ${datarootdir}. Files
  which contain install-related paths are now installed in sysconfdir.

- Fields representing variables are now declared in fldvar, previously call 1 of varpos.
  Fields representing properties are now declared in fldprp, previously call 2 of varpos.
  Fields for the radiation model are now declared in rayprp, previously call 4 of varpos.
  The only remaining call of varpos matches previous call 3.
  The nomvar array is replaced by field labels for fields, and nomva0 for temporaries.
  Field pointers for all variables are accessible from C using the macros in
  cs_field_pointer.h. The ichrvr, ilisvr, scamin and scamax arrays are also replaced by
  field keywords.

- Lagrangian module: for tracking, particle structure is replaced by raw data
  mapped at run-time, allowing for allocation only of useful data.

- Remove support for obsolete LAM and MPICH1 MPI libraries.

- Finalized cleanup of handling of boundary condition coefficients. Fields now allocate
  their coefficients, rather than map them from a common array.

Bug fixes
---------

 - Fix bug in the Generalized Gradient Diffusion Hypothesis (GGDH).
      - swich between two components (R13 and R23): this is not impacting the validation
        database because this model is only validated on 2D test cases
        where the R13 and R23 components are both 0.
      - from version 3.1, it is impacting all the Rij-epsilon calculations
        because from this version, the Daly Harlow model is passed by default on Rij
        (this model induces a GGDH on Rij and epsilon).


Release 3.2.0 (4 Dec 2013)
==========================

Changes
-------

- Documentation:
   * moved tutorials outside the codebase, and into a separate base.
     This allows looser synchronization with the code base, as tutorials may be
     updated somewhat less frequently.
   * complete the Doxygen documentation of
     - Fortran modules
     - user examples
     - Fortran routines
   * install Doxygen documentation from tarball (as built by "make dist").

- Remove deprecated uncoupled velocity solver (ivelco=0).

- Thermal model:
   * the thermal model is now defined by the "itherm" keyword/variable, which
     replaces iscsth(iscalt). In the case of temperature, the scale used is
     defined by a separate variable (itpscal). For additional user scalars,
     a new array iscacp is defined, such that iscacp(iscal) defines whether the
     scalar behaves like a temperature, so the possibility of modeling multiple
     passive "temperatures" is not lost.
     This change allows for better consistency between the standard and specific
     physics, as the thermal variable is now always a "model" scalar, and user
     scalars remain separate. It also allows querying the thermal model with one
     less indirection.
- Atmospheric module:
   * add gaseous chemistry models.
   * plug the SIze REsolved Aerosol Model (SIREAM).

- Turbomachinery modeling:
   * added a rotor-stator model based on mesh joining.

- Particle tracking module:
   * add a modeling of the drying phase of the coal particle combustion
   * add a new boundary condition to simulate coal fouling mechanism
   * bug fixes related to radiative transfer
   * implementation of a particle discretization in the coal combustion model:
     - backwards compatibility is ensured (set nlayer = 1)
     - computation of intra-particle thermal gradients
     - adaptation of chemical source terms to temperature discretization
     - reworked of the particle injection for coal (clear difference between standard
       and user-defined coal composition)
     - adapted the particles and trajectories export routines to be able to output variable
       information for a specific layer.

- Compressible module:
   * change the compressible algorithm from a density formulation to a pressure formulation
   * merge the compressible algorithm with the coupled velocity components algorithm
   * adapt standard bricks (codits, bilsc*) in order to make them compatible with the
     compressible algorithm
   * implement analytical flux boundary condition
     (plus a new total enthalpy / total pressure boundary condition with a fixed point algo,
      generalization of the subsonic outlet)
   * creation of a new set of BC coefficient for the convection operator for compressible flows
   * remove density in the variables array (rtp) and keep it only in the properties array.

- Coal combustion module:
  - added new NOx model for coal combustion;
  - introduction of the coal thermal conductivity
    (for the calculation of intra particle gradients in particle-tracking module)

- Boundary conditions:
   * Fix in the wall boundary conditions for the viscous boundary term
     (the viscous boundary term is not always parallel to the wall). This is
     mainly impactant for verification testcases.
   * add a new Boundary Condition type for free inlet,
     - this BC can be used for natural convective flows in free atmosphere for
       instance (plumes, flame, etc.).

- Turbulence:
   * Major change in Rij-epsilon models:
     - the Daly Harlow model on the diffusive term is now by default for SSG
     - the GGDH brick is used for all the models (LRR, SSG, EBRSM)
     - the "diffusivity_tensor" is added as a field key word
     - Rij-epsilon routines are cleaned up and doxygened.

Architectural changes
---------------------

- For CFDSTUDY, use PARAVIS instead of VISU.

- Only search for SCOTCH/PT-SCOTCH, Metis/ParMetis, Catalyst, and EOS
  if explicitely required to avoid detection of incorrect versions
  on clusters.

- Added cs_c_bindings.f90 module for general definitions of C bindings.
  For large modules, it is recommended to use separate files (see field.f90
  and post.f90 for example), but for smaller modules, this avoids requiring
  the definition of specific module files.

- Added cs_field_pointer API for quick access to main fields from C.

- Added experimental ParaView Catalyst co-processing output option.

- Added new all-to-all infrastructure, allowing alternative algorithms such as
  Crystal Router to MPI_Altoall/MPI_alltoallv as an option.

- Move the convection-diffusion balance (bilsc2.f90) to C.

Bug fixes
---------

- Fixes in the wall boundary conditions (validation cases re-run for safety,
  and were not impacted by these changes)
  - for the velocity, when the wall velocity condition is non-zero,
    the gradient BC was wrong.
  - for the scalars, a term (proportional to the wall value) was missing
    in the gradient BC
  - for scalars with small molecular Prandtl number, the value in the viscous
    sub-layer was not consistent between the gradient BC and the flux BC.

- Many bug fixes (see ChangeLog for details).


Release 3.1.0 (11 Jun 2013)
===========================

Changes
-------

- Many documentation updates

- Documentation: correction of the wall functions provided by D. Laurence,
  description of the BL-v2-k model provided by F. Billard.

- Improve k-omega robustness when yplus is low.

- Use field structure for the scalar with drift and add a drift
  model for coal combustion.

- New key words are added to the field structure:
  * scalar_id (inverse of the array isca(iscal))
  * scalar_class (class of the scalar which belongs to, in particular sharing
    the convective mass flux)
  * inner_mass_flux_id (index of the convective field at inner faces)
  * boundary_mass_flux_id (index of the convective field at boundary faces)
  * drift_scalar_model (type of model for drift scalar:
    0 no drift, > 0 with drift)
  The different models may be activated in cs_user_parameters
  (user_field_parameters)), and one example is available in src/user_examples
  and documented with Doxygen.

- Lagrangian module: implement a zero-flux particle boundary condition to be
  applied with eulerian symmetries.

- Lagrangian module with combustion: use of a formulation of the coal density
  local to a particle and improve the numerics.

- Lagrangian module: add a particle resuspension model.

- Lagrangian module: implementation of a wall law for fluid velocity, k and
  epsilon for the deposition sub-model

- Radiative model: fix existing T2 and T4 quadratures, and add new
  S4 S6 S8 and Tn quadratures .

- Add numbering options for threads.

- Use relative paths when possible in execution script.

- Lagrangian deposition sub-model: improvement of the initialization of the
  particle state vector.

- Increase max coal number to 5.

- Add coke composition for coal combustion.

- Remove old coal combustion model

- Implementation of a Lagrangian boundary condition based on the DLVO theory

GUI changes
-----------

- If the GUI is launched through SALOME, update the object browser in order to
  display the results.

- Possible activation of the Lagrangian particle deposition sub-model
  through the GUI.

- Add new case creation capability by GUI.

- CFD_STUDY: display the listing in the standard dialog window.

User and pre/post processing changes
------------------------------------

- Lagrangian model: full rewrite of the postprocessing output,
  which is now usable in parallel.

- Add handling of white-space in paths.

- GUI and CFD_STUDY: display the monitoring points on the SALOME VTK viewer.

AutoVnV changes
---------------

- Allow to call Code_Saturne GUI functions in external preprocessing scripts
 (automatically set the PYTHONPATH variable).

- Add file input feature to the postprocessing environment in autovnv.

- Add use Agg and suppress usetex to run autovnv on cluster with no X server.

- Merge the preprocessing and case running steps (update documentation example).

- Add the possibility to apply a global post-processing to a study composed
  of several cases.

- Add the possibility to run the same case several times and to prescribe
  impose the name of results directory.

Architectural changes
---------------------

- Automatic installer changes. The installer is now in the top-level directory,
  and does not download Code_Saturne anymore. The setup file template is
  generated by a first call to install_saturne.py. MPI should now be installed
  upstream, but PT-SCOTCH and ParMetis are now handled.

- Improve robustness of SALOME detection for YAMM builds. Sourcing the SALOME
  environment should not be required anymore when the --with-salome configure
  option is used with a YAMM salome build (which incluides its own Python
  interpreter by default).

- To simplify current and future tests, a build-aux/cs_config_test.py
  file was added to allow writing of configuration tests in Python.

- Improve MPI variant detection.

- Add EOS detection and support.

- Add MPMD support for Blue Gene/Q.

- Remove support for legacy (version 1-1 to 1.3) restart files, simplifying code.

- Remove support for obsolete METIS 4/ParMETIS 3 versions.

- Add "flush" stage times to postprocessing writer.

- Add CS_LOG_DEFAULT type to use logging API to listing file.

Bug fixes
---------

- Many bug fixes (see ChangeLog for details).


Release 3.0.0 (22 Mar 2013)
===========================

Changes
-------

- Many documentation updates.

- Lagrangian deposition submodel: improved parallel handling of the
  deposition submodel.

- Always perform the first iteration of the iterative processes (to prevent
  problems if the user set a too large value for the solver precision)

- LES: restore the wall shear stress in the velocity components coupled
  solver (ivelco = 1) when the first cell is in the viscous sub-layer.

- Compressible module is now usable again.

- Lagrangian module: forbid the use of the broken trajectory and displacement
  post-processing in parallel mode.

- Allow user selection of single reduction congugate gradient algorithm.

- Add a Boundary type to vectors (generalized symmetry) where a Dirichlet
  is imposed on the normal component and a flux is imposed on the tangential
  ones (icodcl=14). Needed for Marangoni effect.

- MAJOR fix in Head Losses:
  - itrgpv.f90, itrmav.f90 and projtv.f90 are now adapted to anisotropic
    diffusion (same algorithm as diften.f90 for scalars) for ivelco=1
  - fix in BCs on the rpessure field for ivelco=0 with head losses.
  - the symmetric tensor K for head losses is stored as follows
    [k11, k22, k33, k12, k23, k13] instead of [k11, k22, k33, k12, k13, k23]
    to be consistent with the anisotropic diffusion operator.
  - pseudo pressure velocity coupling is also corrected.

- Replace symmetry/block flags for matrix benchmarking by fill type.
  This allows finer control and easier addition of fill types,
  such as diagonal/extradiagonal block/no block combinations,
  and possible future special block types.

- Add finer control for computation and visualization  of bad cells.

- Add parallel checkpoint/restart for particle tracking.
  (this breaks the contents compatibility for the restart content).

- Unset default "relaxation" on k-omega.

- MAJOR fix in k-omega turbulence model. Buoyancy term and -2/3divu term are
  implicit in the equation of k if they are negative.
  It prevents from clippings on k (if an upwind scheme is used and if ircflu=0).

- MAJOR change in "k-epsilon" turbulence models (iturb = 20, 21, 50, 51):
  - the time stepping on k-epsilon Linear Production (iturb=21) is revisited
    so that any negative source term is taken implicit (it could be the case of
    "-2/3*k* trace(Grad u)" or of the buoyant term). No Clipping on k or epsilon
    should now appear if the convective scheme is upwind and if there is no
    reconstruction on the diffusive term (ircflu=0).
  - The limitation done by the k-epsilon Linear Production (iturb=21) model when
    the Strain rate is big if performed on the deviatoric strain rate and not
    the strain rate itself, as proposed by the model. That was an issue because
    trace(Grad u) is not exactly 0 even for incompressible flows.
  - The subroutine turbke is partially rewritten using additional arrays making
    the code clearer. The order of the steps is then more logical.
  - The relaxation which was performed by default on k and epsilon in tridim is
    deactivated for iturb=21.
  - The negative source terms ("-2/3*k* trace(Grad u)" or the buoyant term) are
    also implicit for models iturb=50 and iturb=51.
  - The buoyant term for atmospheric flows has been adapted.

- Lagrangian module: seed the random number generator with (num_rank+1)
  to avoid statistical bias.

- Lagrangian module: reimplementation of the counter of depositing particles.

- New Fortran bindings for postprocessing, and update user output of variables
  (this breaks the previous usvpst routine, but should be clearer).

- Move definition of variables output of all physics to usipes and separate
  detailed examples.

- Add flags for condensation source terms and exchange coefficient correlation
  (icond and iwallt flags).

- Always use an iterative gradient reconstruction method for pressure gradients.
  In fact, this is done for all gradients deriving from a potential. To
  allow the previous behavior, a negative value of the IMRGRA keyword may be
  used (forcing the method matching its aboslute value).
  Iterative gradients may now also be initialized by least squares using an
  extended neighborhood.

- Set iclsyr=1 as default option (improved symmetry boundary conditions on
  Reynolds stress tensor).

- Adapt diffusive modelization of turbulent flux (T'u') to any scalar.
  This is performed using the new field structure.
  For each scalar, the user can choose 3 options:
  - iturt(iscal) = 0 SGDH (default) muT * GradT
  - iturt(iscal) = 10 GGDH, T'u' = ctheta*k/eps/Rij * GradT
  - iturt(iscal) = 20 AFM, (Alegbraic model)
  - iturt(iscal) = 30 DFM, (Transport equation on u'T').
  Note that the user BCs on u'T' are set at the end of icocl and rcodcl
  (if iturt=30).

- Add a hydrostatic pressure gradient computation (iphydr = 2).
  This allows handling the imbalance between the pressure gradient and gravity
  source term. This pressure gradient currently requires an orthogonal mesh.

- Remove limit on number of classes for Lagrangian inlets.

- Syrthes now only allows nearest-neighbor search for non-matching faces
  as an advanced option. By default, only matching faces are detected, and
  non-matching faces provoke an error. This avoids silently switching to a much
  slower algorithm, while non-matching faces are most often due to inconstitent
  coordinates between domains, rather than different mesh feature detail levels.

- Add Fortran derived types to manage arrays of pointers.

- Add several boundary postprocessing options (notably wall T+, temperature, and Nusselt).

- Add GGDH-AFM and DFM models for the thermal scalar. This options is available
  with the key word iturbt (0, 10, 20, 30).
  Warning: the transport equation on turbulent fluxes (DFM) requires changing
           the gradient boundary conditions on the thermal scalar to have the
           proper production term. It is now consistent with the gardient
           boundary conditions on the velocity.

- Improve user scripts, to add data preparation and results copying user hooks.
  An example is provided, allowing simplified successive restart handling.

- All files in case's DATA and not in subdirectories are now copied
  automatically to execution directory.

- Move initialization of IO logging to main initialization block.

- Add a soot model for gas combustion.

- Add computation of combustion source terms for the Low Mach algorithm (idilat=4).

- Change the default value for the precision of the reconstruction iterative
  process (codits, coditv): it is now by default 10 times the precision of the
  linear solver, to be consitent with resopv.f90.

- Add an extra block size to matrix (used for solving vectorial field with
  tensorial diffusion). Add bricks for tensorial diffusion for vectorial fields
  (matrvv, vistnv, diftnv).

- Modify iterative process to print the proper residual in the listing.
  That means we always compute the residual (whereas we didn't before), so
  it might be a little bit more costly.

- Adapt the dynamic relaxation to vectorial field (from codits to coditv).
  The log messages are also changed so that the normed residual in the listing
  is now the one of the iterative process (codits and coditv).
  The nuber of iterations for the solver is now the sum of iterations for the
  solver over the sweeps in codits or coditv, as it was already done in resopv.

- Add a new algorithm to solve diffusion term with anisotropic & heterogenous
  viscosity for scalars (for use with GGDH);
  to activate it set idften(ivar) = 6 (for symmetric tensor diffusion)
                                  = 1 (for standard scalar diffusion)
                                  = 3 (be for orthotropic diffusion, diagonal tensor)

- Add a new dynamic relaxation for solving the Poisson equation on the pressure;
  to activate it set iswdyn(ivar) = 1 for a relaxation with the last increment
                                  = 2 for a relaxation with the two last increments.
  should be used only for transport equation without advection.

- Replace depecrated activated() SIGNALs by triggered() ones as advised by
  the Qt documentation.

- Add rotation/curvature correction (Spalart-Shur and Cazalbou) for Eddy viscosity
  turbulence models.

- Add (exact) Coriolis terms in Rij-epsilon models (LRR, SSG and EBRSM).

- Use vector coefa/coefb for postprocessing output when applicable.

- Major Fix on Boundary conditions with the coupled velocity components algo (ivelco=1).
  - The Gradient boundary term for the velocity in k-epsilon, 2 scales of velocity was
    not computed correctly.
  - The wall shear stress in Rij-epsilon was counted twice.
    Note: The previous versions of CS for Rij didn't ensure that rho uk*uet was
          the wall shear stress.
    Note 2: The 2 scales of velocity for Rij does not work properly in a channel,
            because the scale uk is underestimated.

GUI changes
-----------

- Integration of UNDO/REDO function.

- Allow setting of RHS reconstruction sweeps for pressure.

- Add electric models.

- Change partitioning page into tab of a more complete performance tuning page.

- Add a popup for print XML function

- suppress Current species class.

User and pre/post processing changes
------------------------------------

- Change default v2f model from phi model to BL-v2k model.

- Output probe set coordinates in CSV format.

- Regroup usatsoil and usatdv user subroutines in cs_user_atmospheric_model.f90.

- Replace ficstp by control_file, with extended options. This file may now
  also be used to force postprocessing or checkpoint output.

- Introduce physical time for mesh rotation start.

- Allow using SYRTHES 4 even if matching environment is not sourced.

- Allow user definition of additional compile/link options to simplify usage of
  external libraries.

- Move some post-processing functionnality to utility functions, for easier usage.

- Add user example for visualization of space-filling curves.

- Add a starting time for the computation of moments.

- Read JANAF file from reference directory directly instead of using a local copy.

- Use reconstructed value for postprocessing of heat flux.

- Remove coefa/coefb arguments from user subroutines.
  We now encourage the use of the field API. Legacy coefa/coefb
  arguments are nonetheless kept in cs_user_extra_operations.f90,
  as we may still need to compute a gradient of a single velocity
  component even when ivelco = 1 (at least until examples are improved).

- Add CCMIO output for main volume and boundary meshes.

- Move user control of mesh warping handling to cs_user_mesh.c

- Improve defaults for cs_user_parameters and make examples more consistent.
  The "--nogui" option of "code_saturne create" is finally removed.
  Tests on "iutile" are replaced by .true. or .false. for clarity.

- Remove obsolete igghexa to MED 2.3 converter tool.

- Lagrangian module: removal of the now-useless routine uslabo.

Architectural changes
---------------------

- Move field properties from cstphy to optcal.

- Update detection of PT-SCOTCH/SCOTCH to handle new version 6.0.

- Allow definition of a user or site shell rcfile to modify the execution environment.

- Add finer control for parallel block I/O.
  Global data is now never read in a collective manner, but broadcast,
  while additional modes and hints for MPI-IO may be chosen by the user
  (control is moved from the command line to the GUI and user files).
  It is now possible to use a specific I/O communicator of smaller
  size than the main calculation communicator.
  These additions are part of a "Performance Tuning" group of user options.

- First version of the Windows port of Code_Saturne.
  This brings up the following adaptations: the installation can now be relocated
  (also available on Unix systems), the scripts (SaturneGUI, runcase,
  run_solver.sh) are now generated on the fly and depend on the underlying
  system and shell, and the interaction with NEPTUNE_CFD package is also changed
  for a correct behavior.

- Add C API for access to time step information.

- Use ISO_C_BINDINGS to improve Fortran API for fields

- Python cleanup and partial Python 3 compatibility.
  Except for Unicode and Qt4 aspects of the GUI, Python code
  should now be compatible both with Python 2 and Python 3.

- Move some base Fortran API functions from cs_base.c to cs_base_fortran.c,
  and replace CPU times by elapsed time in Fortran timings.

- Default logging mechanism may now switch between multiple modes.
  This allows combining a C stdio-based API an a Fortran IO based API,
  switching to Fortran where it is dominant (in which case bft_printf()
  uses Fortran IO, as before), and back to C where preferred.
  This removes the need for flushing of Fortran output, as bft_printf_flush()
  is used mainly by the C API, and a switch back to the C API is forced
  (with the Fortran output being closed) before error logging.

- Allow query of locale directory and package data directory from main executable.

- Rewrite gradient quality tests in C.

Bug fixes
---------

- Many bug fixes (see ChangeLog for details).


Release 2.3.0 (23 Jul 2012)
===========================

Changes
-------

- Set the coupled velocity component solver as default option (ivelco=1).

- Default turbulence model is now linear production variant of k-epsilon.

- MAJOR atmospheric/meteo addition of new features (humid atmosphere and
  soil module).
  Note: humididy, soil and 1D radiation models are experimental.

- MAJOR change: the Temperature transport equation is multiplied by
  Cp (specific Heat) so that the equation has now the dimension of energy.
  The change is expected to have NO influence when Cp is constant.
  When Cp is variable in space, this change fixes the error done on this
  equation.

- Change default values for NSWRSM.

- Add synthetic turbulence inflow methods for LES:
  - random method (Gaussian noise),
  - Batten method (based on Fourier decomposition of turbulent fluctuations),
  - Synthetic Eddy Method (SEM).

- Adapt the Multigrid algorithm to vectorial Poisson equation
  (such as mesh velocity for ALE).
  - The aggregation criterium is based on the trace of the diagonal block
    DA (3x3), but can be a changed (We could test n.DA.n),
  - The multigrid algorithm for scalars (such as the pressure field) is
    rigourously unchanged.

- Add a low Mach algorithm (semi-analitical: idilat=4).

- The subroutines codits and inimas/inimav are transparently changed:
  - codits save and return the last increment,
  - inimas/inimav can compute a velocity flux OR a mass flux regarding
    the value of itypfl.

- First stage of the implementation of the diffusion-inertia model of
  aerosol deposition. Still under development in this revision.

- Add an multi-species algorithm for low-Mach number algorithm (idilat=3).

- MAJOR changes to the formulation of boundary conditions for diffusive part.
  The changes impact the subroutines where the BCs are computed (condli,
  clptur, clptrg, clsyvt) which are rewritten (and doxygened).
  The changes should not impact the results (to the truncature error precision).
  A new boundary condition is added: convective/radiative outlet (icodcl=2).
  The radiative transfer module has been widely modified:
  - a new solved variable (in rtp) call ilum has been created,
  - the boundary coefficient are now in the same array as for the
    other variables,
  - the new Boundary condition (radiative) is used and user set BCs with
    rcodcl and icodcl
  This may have introduced bugs in the compressible module.

- Lagrangian module: removal of the 'snap_to_grid' (legacy) method of
  particle localization

- Lagrangian module: first stage of the implementation of the parallelism.

- Add bad cells detection and post-processing.

- Lagrangian module:
  - English translation of the main messages
  - Suppression of the display of the ambiguous mean values of the stats

- Clean the coupled velocity component version or the correction step
  of pressure. The loop over non orthogonalities is performed in a
  clearer manner. The updating of the mass flux is always performed so
  that the continuity equation is fullfilled exactly (at the pressure
  precision) even when the iterative process have converged.

- Pass the mass aggregation term (-div(rho u)T) directly into the linear
  system (matrix and bilsc) to be coherent with NCFD.

- Add a Low Mach compressible algorithm conservative in time for the
  momentum equation and the transport equation of any scalar.
  It adds a prediction step of the mass flux. Available with the
  key word idilat (2 or 3).

- Add a low-Mach algorithm to account for the mass equation for dilatable
  flows. It is only available for mono-species flows at the moment.
  This can be activated with the idilat keyword set to 3 (1 being the
  current default).

GUI changes
-----------

- Add handling of gas combustion model.

- Add handling of solid fuel combustion.

- Add compressible algorithm in GUI (not fully operational in this version
  yet: version 3.0 recommended).

- New presentation and use MEI to initialize scalar boundary conditions.

- Volumic initialization for meteo variables.

- Add choice for NSWRSM and IRESOL.

- Use splines to define profiles.

- Modification of min, max and initialization for scalars and variance.

- Langrangian module: modification of the oundary conditions:
  - Rename of the classical boundary conditions

- Lagrangian module: modification of the volume and boundary
  statistics management:
  - Rename of the default names
  - Names non-modifiable in the GUI
  - Post-processing or not or the default variables
  - Move of the names from uslag1 to lagopt.f90
  - Rename in lagopt to be consistent with the GUI

- Pulverized-coal model not activatable in the GUI (deprecated).

- Use MEI to initialize turbulence, velocity and thermal variables by zone.

- Add use of MEI for turbulence boundary conditions.

- Added piso and modification of control time step with
  velocity-pressure algorithm choice.

- Move hydrostatic pressure option from body forces to numerical parameters.

- Use MEI only for deformable mesh and control access view.

- Add support for Rij-epsilon EBRSM and Spalart-Allmaras turbulence models.

User and pre/post processing changes
------------------------------------

- Separate usproj.f90 into multiple examples.

- Add a user example for LES inflow.

- SYRTHES coupling: in case of unlocated Code_Saturne elements in SYRTHES mesh,
  these elements are now post-processed.

- In case of a single SYRTHES coupling, adjust name to automatic match.

- Split usray5 ("User" subroutine for radiative transfert) into 2 parts:
  - raycll, which is not a User subroutines, which sets BCs on luminance
  - usray5 (iappel=2) where a net flux is computed.
  This should allow to remove luminance from rtp (ilum).

- Add variable/port name to SALOME Kernel Calcium API messages.

- Postprocess deformation in ALE mode.

- Add user function to disable or force mesh_output.

- Replace usphyv by cs_user_physical_properties.

- Force use atphyv for density property for meteo physics.

- Update of the max number of particles to visualize from 500 to 100000

- EnSight Gold variable description limit is now 49 characters, not 19.

- Autovnv: add new option --update in order to upgrade a repository
  of test cases by reload files of parameters (i.e. run the
  backwardCompatibility method) and changes pathes for SaturneGUI and
  runcase. Add capability to mix Code_Saturne and NEPTUNE_CFD test
  cases in the same Study.

- New Autovnv. functionality: 2D view of scalar (needs pyvtk).

- Remove Fortran utility subroutines used to obtain global mesh element numbers.

Architectural changes
---------------------

- Use 16 characters instead of 8 for variable and property names.
  Improve formatting, and make default variable names witout GUI more
  consistent.

- Add C parallel operation wrappers.

- Add new structures for measures set -> global mesh interpolation
  (cs_measures_set_t) and global mesh -> point cloud interpolation
  (cs_interpol_grid_t).
  These features will be used soon in atmospheric module.

- Dependencies on libraries are now handled in the standard
  Automake manner, to avoid issues with the gold linker
  (this means building a dynamic libsaturne on top of static dependency
  may no longer be possible).

- Detection of dynamic versions of SCOTCH, METIS, and HDF5 is
  now made possible.

- On Mac OS X, build is static by default, and compiling of user
  subroutines for a static build requires unarchiving the library and
  overwriting selected object files, to avoid issues with multiple
  definitions not being handled by the Mac OS X linker.

- Move partitioning to main solver executable.
  This simplifies the toolchain, as a separate partitioner is no
  longer required. Additional options for finer-grained control
  are provided, and parallel partitioning is encouraged.

- libPLE: use same FLAGS as parent Code_Saturne build.
  This helps ensure subconfigure is consistent. Bootstrapping also
  inherits prior cleaning stage from that of parent.
  Also, dependencies on MPI are handled in the standard Automake
  manner when building libPLE (this means building a dynamic
  libPLE on top of a static MPI may no longer be possible).
  This implies changing at least the patch release number for PLE.

- Port to Blue Gene/Q.

- Moved block distribution functions from fvm to base.

- Allow user configuration of compilation flags for performance-critical files.

- Merge fvm_parall.* and cs_parall.*.

- Remove support for coupling with (obsolete) version 3.4 of SYRTHES.

- Reduce use of external BLAS functions based on recent comparisons
  with internal functions.
  Reduce usage of external BLAS to benchmarking (to allow for occasional
  comparisons).

- Replace external BLAS dot product with superblock variant for
  better expected precision.

- Move definition of parallel rank and thread status from cs_base.*
  to cs_defs.*.

Bug fixes
---------

- Many bug fixes (see ChangeLog for details).


Release 2.2.0 (30 Mar 2012)
===========================

Changes
-------

- Add a porosity formulation.
  The transport equations (espacially in turbulence) have to be checked.
  We also have to check if the formulation is all right in presence of
  Coriolis forces.

- Add Least square method for gradients of a vector.
  Add a clipping for gradients of a vector. Only available for
  coupled velocity components algo (ivelco=1).

- Multigrid: iagmax variable in autmgr.f90/_automatic_aggregation should
  be reset to for each coarsening, and should thus be an internal variable,
  not an argument.
  This leads to more regular aggregation patterns, though often 1 or 2
  more grid levels.

- Make the Cocg matrix for the vectorial iterative gradient DIMENSIONLESS.

- Update handling of periodicity of rotation for more consistent usage
  of halo synchronization. The parcom and percom routines are now
  fully replaced by the halo syn*** series of routines.
  At this stage, the effective operations are unchanged, although
  the API should be clearer.

- Lagrangian module: Implementation of a simpler way to calculate the
  determinant in the trajectography sub-module (default choice from now on)

- Make the Coriolis source term partially implicit with the coupled solver.

- Make free-surface flow independant of the axis direction but dependant of the
  gravity direction.  A checking is added in vericl.

- Add initial version of renumbering for hypbrid parallelism using OpenMP.
  The renumbering algorithm for interior faces is based upon one of the simpler
  algorithms provided by IBM, and is mainly destined for tests, as better
  performing algorithms will be added as a second step.
  The renumbering for boundary faces is simpler and is not based on the
  IBM library.

- New option added: dynamic relaxp in resopv (swpdyn = 1).
  Only available with ivelco = 1.

- Add the Rij EBRSM model (iturb = 32)

- CS-CS coupling avalaible in ivelco=1.

- Remove the multigrid algorithm by the default for eletric variables.

- Use reserved name for temperature or enthalpy field.

- Interleaved ALE displacement array for ivelco=1.

- Log SYRTHES 4 overheads timing information.

- Improve the temperature calculation  in the Libby-Williams model when
  the model is not adiabatic by using the transported enthalpy.

- Improve SALOME CFDSTUDY module

- Ensure Laplacian used to compute wall distance is positive.
  A second pass without reconstruction is run if this is not the case.

- Add matrix dump to file function.

- Add a free surface boundary conditions for the mesh velocity (only
  available with the coupled framework ivelco = 1). Also add a utilitarian
  function to find the closest node of a given point.

- Add a coupled framework for the ALE module.

- Make implicit the handling of the transpose gradient of the velocity
  as well as the secondary viscosity within the diffusive flux
  computation routine (bilsc4).

- Add mesh smoother with initial unwarping algorithm.

- Many minor changes (see ChangeLog for details).

User and pre/post processing changes
------------------------------------

- Allow choice of ADF or HDF5 format for CGNS.

- Add postprocessing options for Syrthes in runcase_coupling.

- Move all user files in a single dedicated directory named src/user.

- Empty reference boundary conditions and initialization user subroutines.
  Examples are now given separately in a SRC/EXAMPLES case subdirectory.
  - Replace all the specific boundary conditions routines by a single
    cs_user_boundary_conditions one.
  - Replace all the specific initialization routines by a single
    cs_user_initialization one.

- Merge all the option initializations for the specific physics
  into the existing usini1.f90, including usppmo.f90

- Merge mesh-related user files in a single cs_user_mesh.c

- Merge nearly all source terms definition in a single cs_user_source_terms.f90

- The mechanism for advanced selection or modification of postprocessing
  meshes is now based on user-defined selection functions.

- Remove never-used user function for multigrid coarsening.

Architectural changes
---------------------

- Remove support for CGNS versions < 3.1

- Remove support of PROSTAR/ngeom input format.

- Remove MED 2.3 support.

- Added function attributes to bft_printf() and bft_error() with GNU or Intel
  compilers so as to check format arguments, and fixed all errors and
  warnings subsequently reported.

- Rewrite multigrid autmgr.f90 and crstgr.f90 in C (respectively
  _automatic_aggregation and _build_coarse_lvl in cs_grid.c).

- Rewrite gradient reconstruction in C, with interleaving and OpenMP loops.

- Add typedefs for multidimensional arrays. This allows for much
  clearer syntax for interleaved multidimensional arrays with
  fixed "local" dimensions. Examples of their use may be found
  in gradient computation functions.

- Force link with C++ when using MEDCoupling or PARAMEDMEM.

- Remove obsolete/unused parallel call counters in Fortran wrappers.

- Move additional quantities such as COCG, II', and JJ' from Fortran to
  cs_mesh_quantities structure.

- Added field (and mesh location) API for both C and Fortran
  Field maintain their own metadata, including keywords and boundary condition
  coefficients information.

- Add initial MEDCoupling output plugin writer.

- Add plugin mechanism when dlopen/dlsym/dlclose are available.

- Add a variable related to the Fortran modules directory so as to enable
  NEPTUNE_CFD to compile Code_Saturne Fortran files.

- ChangeLog is now now automatically generated either by running
  'make changelog' on a Subversion checkout, or when
  distributing an archive by running 'make dist'.

- Separation of postprocessing into a common part (usable by other codes)
  and specific Code_Saturne additional default outputs.

- Separate extended neighborhood management from LES filter.

- Maintain vertices interface set in mesh structure for use by mesh
  modification or ALE.

- Replace fvm_interface_t with cs_interface_t structure.
  The API is slightly modified, as cs_interface_t uses 0-based ids for
  local elements, uses a send order to fix bugs with the previous
  API when periodic local and matching elements could not both be sorted by
  increasing global number, and includes some utility functions,
  for copies and sums.

- Use cs_lnum_t instead of cs_int_t for mesh structure.

- Merge system info from bft_sys_info.* and cs_base.* to cs_sytem_info.*.

- Rename cs_perio_* to cs_halo_perio_* (prepares move of fvm_perio_*
  to cs_perio_*).

- Migrate some fvm_ functions and types to the cs_ name prefix.
  fvm_order_* is also moved to cs_order_*.

- New LaTeX classes are added.
  A new plan is added in the theory guide.
  A note on basic rules to write the theory guide is added in the
  developer guide.

- Improve documentation tools detection and add a doc rule at the top level
  directory, and rename the doc directory to docs to avoid Makefile
  incoherency). Also add an update-po rule at the top level directory.

- Add a --with-salome configure option that takes care of SALOME modules
  detection avoiding the use of the different --with-salome-xxx.

- Remove tests using diagonal matrix BLAS 2 from benchmark mode,
  as initial tests show they are slower than specific code, while
  they would require more costly storage than a blocked diagonal.

- Improve handling of external BLAS.
  Either wrappers with the "cs_" rather than "cblas_d" prefix are used
  (for daxpy and ddot with strides of 1), or those functions are
  provided if no external BLAS is available.
  Support for Fortran BLAS is dropped, except for IBM ESSL and AMD ACML
  (which is added), as most other modern BLAS provide C API's.

- Add logging API, which is used for improved multigrid performance information.

Bug fixes
---------

- Many bug fixes (see ChangeLog for details).


Release 2.1.0 (20 Oct 2011)
===========================

Changes
-------

- Add thermochemistry reference files for the unified combustion modeling.

- Add coupling with SYRTHES 4.0
  This includes boundary and volume coupling features.
  A conservativity flag ay also be used to force energy conservation.

- Set the relaxation coefficient to the classical value of 0.7 instead of
  0.9 for the steady algorithm.

- Make the thermochemistry file name coherent with the scripts.

- New turbulence model in the framework of the v2-f models.
  This is a "blended" v2f (iturb = 51).

- Add a prototype of solving the velocity components in a coupled way.
  It can be tested by setting the ivelco variable to 1 but is not yet
  compatible with every feature (use with caution...).

- Add an experimental combustion model for coal and heavy fuel oil
  with a unified gas-combustion modelling.
  This new modelling replaces the previous fuel modelling (which is
  still available as a backup).

- Add thin wall insertion.

- Implement the correct behavior to handle thermal wall-function in
  the framework of the scalable wall-functions.

- First implementation of a V&V automatization tool.

- Non-symmetric matrix coefficients are now interleaved.
  (the Fortran API still allows non-interleaved matrixes as an option).

- Remove synchronization of postprocessing with Code_Aster.

- Add a particle deposition model to the Lagrangian module.

- Prefer initializing the random-number generator with a seed equal
  to 1 instead of 0 (as advised in the zufall.f90 comments).

- Delay discarding of isolated faces to just prior calculation phase.
  This allows post-processing of those faces, as well as their usage
  in mesh joining (not updated for this yet) or user modification.

- Add possibility of defining a default destination rank for
  block to part distributor based on strided adjacency, so as to
  also distribute elements with no adjacency.

- Added choice of Hilbert SFC for domain partitioning.

- Added GMRES to linear solvers.

- Enable build of Doxygen documentation (currently minimal).

- Finalize Code_Saturne/Code_Aster coupling s now known to work
  with SALOME 5.1.5 and Code_Aster NEW10 recent enough on Calibre 5.

- Add a one-equation turbulence  model: the Spalart-Allmaras model.

- Added single-reduction variant of preconditioned conjugate gradient solver.

- Optional merge of coarse grids across processors so as to allow coarsening
  beyond domain boundaries.

- Remove the MATISSE module.
  The MATISSE module can be found in its last version by the Subversion
  tag pre_removing_matisse.

- Fix a mesh-numbering dependancy (and number-of-processors dependancy) in the
  choice of the face at which one takes the reference presure, when the user
  defined a free outlet boundary condition.
  Results may differ from previous calculations but should be not much wrong
  than before and will be less dependant on other parameters.

- Log number of cycles instead of equivalent iterations for multigrid.

- Handle multiple batch systems through the GUI depending on the configuration file.

- Add SALOME module generation, for future Code_Saturne/Code_Aster coupling.

- Move the mass-flux update in case of a rotating mesh, only relevant when
  disabling the pressure reconstruction (no impact on current simulations).

- Remove rarely used interior faces selection for mesh checking.

- Many minor changes (see ChangeLog for details).

User and pre/post processing changes
------------------------------------

- Many updates and additions to GUI.

- Switch to new case directory hierarchy, allowing a new coupling
  directory structure using one subdirectory per domain.
  A domain's name matches its subdirectory, and a new
  runcase_coupling may be generated by cs_create when multiple domains
  are present.
  File and directories are not renamed by the script anymore, so
  copying of results from the execution directory is better automated
  and the latter may be purged when no error has occured. Better,
  the case may be run directly in the results directory.
  The user does not need to specify files to retrieve, but may specify
  scratch files not to retrieve (which should be much rarer).

- Add a master script Python module to call the different modules.

- Scripts and GUI overhauled, with user Python functions and script XML reader.
  Restart behavior is now based on the presence of a restart sub-directory in
  the execution directory. A "--preprocess" option has also been added to the
  Kernel so as to handle purely preprocessing runs.

- Remove inconsistant 'check_mesh' command from the main script (superseded
  by both the graphical interface and the 'run' command). Also remove
  the 'check_consistency' command which was a pale copy of the verification
  stage (--quality option of the solver).

- Allow selection of an alternate build for compute tasks.
  This is useful mainly for supercomputers with separate front-ends, such
  as IBM Blue Gene machines.
  Also allow disabling build of front-end tools.

- Try to use the same shell as the user's current shell in generated
  scripts used by the "code_saturne run" command.

- Add a SALOME command to the main Code_Saturne script so as to launch the
  SALOME platform with the CFDSTUDY module enabled.

- Remove the now useless "code_saturne plot_probes" command since the probes
  now have only one first column for either the time-step number of the time
  value (it was only a wrapper aroun xmgrace -nxy $file).

- Replace the drag'n drop feature in the graphical interface by a more
  intuitive add/remove mechanism for the profile and time average pages.

- Allow reading of CGNS files with BC's referring non-existant edges, as a
  workaround for a bug in ICEM CFD 13 CGNS export.

- Use SCOTCH instead of METIS by default when partitioning.

- Update ParMETIS support to version 4.0.

- Add the possibility for the user to define advanced post-processing,
  writers and meshes, from the GUI.

- ficstp.MOD renamed to ficstp_updated to avoid confusion with Fortran modules.

- Use the "executable" mode of YACS instead of the "loader" one
  for both Code_Saturne and Code_Aster.

- Separate mesh joining verbosity and visualization level. Above verbosity
  level 2, output is directed to a processor-local log file.

- Move activation of Cooling Towers postprocessing to that module.

- Make activation of SYRTHES postprocessing coupling-instance specific.

- MED output: a field must have different names on different MED
  meshes within a single file, so postpend mesh name if necessary.

- Add the possibility of setting up a frequency output in seconds in the GUI.

- Remove all the occurences of the user and developer arrays. User should now
  use the user_modules.f90 suggested in the user files, and developers should
  use allocatable arrays in one of the modules (see src/Makefile.am).

- Transform user files for joining, periodicity, mesh modification,
  SYRTHES and Code_Saturne coupling from Fortran to C.

- Preprocessor: merging of coincident vertices or multiply-referenced
  vertices in face definitions moved inside generation of descending
  connectivity so as to handle cases where quadrangle faces transformed
  into triangles by vertex merging may be identical with faces already
  defined as triangles.

- Preprocessor: extracted meshes should only contain connected vertices.

- Preprocessor: removed postprocessing format options
  and additional minor source code cleanup.

- Preprocessor only creates visualization files if necessary.

- Removed preprocessor meta-file and command-line input file support.

- Preprocessor now converts all colors to groups on mesh import.

- Add output of default volume and boundary mesh groups to EnSight format.
  This requires the usage of additional cases, so as to avoid time dependency
  issues and group name clashes between surface and volume parts.
  Removed group output by Preprocessor for EnSight format now it is in Kernel.

- Improve the cs_solver options management so that the error message is clearer
  in case the code is not compiled with X feature support.

- For code coupling, remove all occurences of the application number and
  replace it by the, application name, which is based on the matching
  computation domain case's direcory name.

- The monitoring files are now created in a specific directory.

- The checkpoint files are now created in a specific directory. Likewise, the
  restart files are read from a specific directory.
  Moreover, the filenames cannot be changed by the user anymore (it was
  already breaking the scripts anyway).

- Add bash completions for Code_Saturne executables.

- GUI: handle batch system based on batch template and code_saturne.cfg.

- Add optional code_saturne.cfg configuration file:
    - select batch type and default batch card.
    - handle the temporary directory from the config file.
    - handle the notion of mesh database directory.

- Change the default behavior for copying the result files (without suffix).

- Make the particles output compliant with EnSight 6 format and improve the
  robustness of the output for visualizing with ParaView.

- Add diff capabilities to the I/O dump utility.

- Move the warped-face-cutting setup from the command line option to a Fortran
  user routine and XML file.

- Switch the joining and periodicity support from the runcase script to the
  XML reader when using the graphical interface.

- Switch to the Python runcase script; the GUI now handles this script,
  and the old (shell) script is removed.

- Add timing information for mesh input I/O.

Architectural changes
---------------------

- Add a developers guide with coding standards.

- Add an installation documentation.

- Enable build with MED 3.0 (based on 2.9) as well as with MED 2.3.

- Enable build with CGNS 3.1 as well as CGNS 2.5.

- Print additional MPI environment info for Blue Gene/P.

- Use specific intracommunicator instead of MPI_COMM_WORLD for coupling with
  SYRTHES 3, to avoid bug due to non-contiguous MPMD rank-numbering on
  BLue Gene/P or similar machines.

- Many changes to matrix API:
  - Move matrix type definitions to cs_matrix_priv.h,
    so as to allow implementing matrix operations over several files
    (adding cs_matrix_util.* here).
  - Assign coefficients to matrices outside linear solvers.
    This and allows for simpler and more consitent calls to linear solvers.
    An added benefit is the fact that the overhead of assigning coefficients
    is applied once per time step instead of once per multigrid cycle.
  - Remove alpha.A.x + beta.y operation type for matrixes.

- Added Matrix tuning infrastructure and updated benchmark mode.
  Benchmark mode now uses a fixed minimum time rather than number of
  passes, so as to be less dependant on mesh size.
  Matrixes now include an MSR structure, (modified CSR, with separate diagonal),
  and new operators are added.

- Add OpenMP directives for linear solvers.

- Express Jacobi solvers using y <- A.x rather than y <- alpha.A.x - beta.y
  formulations, and take advantage of the new (A-D).x operator to
  remove extra matrix for polynomial preconditioning.

- Remove sockets support for SYRTHES3 coupling.

- Remove support for IRIX and Tru64 Unix, as these systems are now obsolete.

- Merge bft_file.* and fvm_file.* into cs_file.*, replacing bft_file_printf()
  by simple fprintf(), and making endian-swapping code local where needed.

- Replace cs_bool_t with bool.

- Merge bft_config_defs.h, fvm_config_defs.h, and some definitions from
  cs_base.h into a single cs_defs.h header. This also includes preparations
  for replacing fvm_*num_t by cs_*num_t.

- Un-version TODO file.

- Add --with-modules configure option to allow override of automatic detection.

- Update METIS support for METIS 5.0.

- Upgrade post-processing management API for better mapping with the
  GUI, and for better clarity of user options. All related settings
  are now local to cs_post.c, and are removed from entsor.f90.

- Add a relocatable option to the configure script to handle relocatable
  installation (of executables). It is based on the $ORIGIN variable for
  RPATHs that should be understood by at least GNU and SOLARIS linkers.

- Split the base directory into 4 directories with 3 new ones dedicated
  to the mesh handling, the turbulence modelling, and the Finite Volume
  schemes and resolution.

- Major memory management update: a dynamic allocation when
  necessary, remove useless work arrays and move work arrays where
  there are really used.
  Remove the allocation of main arrays in the C part and the
  corresponding user interface (both graphical and Fortran).
  The only remaining bits of the macro arrays are the ones related to
  the post-processing management (aka ipp2ra): rtp, rtpa, propce, dt and
  tpucou.

- Split the gradient API into subroutines to highlight the pressure
  gradient computation and facilitate future simplifications and tests.
  Only the new 'grdpot' subroutine is now able to account for body forces.

- Remove explicit support of n phases (support was never used, and is still
  possible using adequate variables and defining relations between them).
  Phase index is removed from all arrays, improving code readability and
  avoid bugs in which iphas was not re-set to 1 after a previous loop on
  phases.

- Add a developers guide with coding standards.

- Remove the vectorization directives (when forced) so as to simplify
  the code maintainance and since we do not have  access to a vector
  computer at the moment. Thus, the ivecti/b indicators are now useless.

- Remove matrix structure symmetry flag, replacing if by using a specific
  symmetric matrix type where applicable (added symmetric CSR type).

- Move the calculation of geometric quantities (useful for handling the
  non-orthogonalities) from the Fortran part to the C part.
  The arrays are now accessed directly instead of through a pointer to ra.

- Make use of the "package" concept in the graphical interface to have an
  easier management of both Code_Saturne and NEPTUNE_CFD codes.

- Added detection and handling of environment modules. The configuration
  detected at configure/build time are saved and applied when compiling
  user subroutines or when running a calculation script. A --with-modules
  configure option allows overriding of automatic detection.

- Add the CFD Proxy library to Code_Saturne repository.
  This library is used when Code_Saturne must be wrapped by YACS (SALOME
  component) as a shared library, providing specific Calcium wrappers, for
  example in the Code_Aster / Code_Saturne coupling case. This library
  should be removed when we switch to the executable mode of YACS.

- Use C++ wrapper to link with MED library if necessary.
  This avoids requiring the definition of MED dependency
  libraries, which could interfere with libtool in cases
  mixing static and dynamic libraries and cross-compilation.

- Added C API to handle probes.
  This allows not writing to a temporary file anymore and enabling both
  the legacy .dat (text block data/XmGrace) format and CSV files.

- Add members to the cs_vars_t structure to account for the number of phases,
  in order for NEPTUNE_CFD to be able to link against Code_Saturne source code.

- Introduce a package-specific Python module to avoid too many overloading of
  Python classes by NEPTUNE_CFD. It replaces the cs_config.dirs class and adds
  some useful specific information like the package name, version, ...
  Some work remains to be done in the graphical user interface code, because
  the cs_package module is directly used instead of being passed on.

- C++ compiler detection for a possible link with this compiler when linking
  with MED support and to ease NEPTUNE_CFD configury.

- Move the bison/yacc compilation from the bootstrap stage to the
  compilation stage. Also generate the corresponding C files at dist stage.

- Generate the documenation at dist stage.
  Install the documentation with install target if present.

- Added selection functions for faces at cell criteria boundaries
  and for pre-selection of families.

- Attributes are removed from group classes.:
  Attributes read in the input mesh are converted to group names so as
  to be renamable by the user and listed in the meshe's groups, but
  additional mesh family items may be built when group names are convertible
  to integers so that user subroutines looping on families and family
  properties still work as before.

  Also, selectors still contain internal attributes so as to ensure a
  range[] of integers works as expected, but these are now built directly
  from group names which are convertible to integers.

- EnSight writer now enables parallel IO in binary mode.

- Output information on groups and periodic faces in solver log file,
  and add selection functions to list periodic faces.

- Enable saving of meshes in preprocessor data output whenever
  the input mesh has been modified or meshes have been concatenated.

- Add preprocessor_output files concatenation to the kernel (works in parallel).
  Appending multiple meshes is now done through a user function:
  coordinate transformations and group renames are now possible.
  Mesh concatenation support is removed from Preprocessor.

- Transform all Fortran common blocks to modules.
  Fold dimfbr into dimens and vector into parall.

- Move all Fortran include files from include/* to src/* and rename
  their extension to .f90 in preparation for switch to modules.
  Rename vortex.h to vorinc.f90 to avoid conflict with existing vortex.f90.

- Instrumentation of the gradient computation. Also add a first
  implementation of a pure C interface fo the gradients.

- Add a new API for halo synchronization. Four new functions are available for
  scalars, vectors, diagonal tensor and 9x9 tensor. The old API
  "parcom/percom" remains available.

- Make the CCM files reader able to read both 2.6.1 and later versions.

- Move the preprocessor into the Code_Saturne tree.
  Major code refactoring to ease the maintenance.

- Rename the package from ncs to code-saturne instead.

- Change the behavior of the configure option for finding a Python interpreter.

- Migrate the BFT (Basic Functions and Tools) library to the Code_Saturne tree.

- Migrate the MEI (Mathematical Expression Interpreter) library to the
  Code_Saturne tree.

- Migrate the FVM (Finite Volume Mesh) library to the Code_Saturne tree.

- Replace the FVM coupling library by the new PLE one, which may be installed
  either as part of Code_Saturne, or separately (Code_Saturne may use either
  its internal PLE library or an external build).

- Replace the SWIG dependency for the syntax checking in the graphical
  interface by a small executable called at each check.

- Add the periodicity joining handling to the solver's parallel joining
  algorithm.

- Move the partitioning and I/O dump tools from the preprocessor to the kernel
  package. Add ParMETIS and PT-SCOTCH/SCOTCH support. By default, serial
  partitionning is done, but parallel partitioning may be selected with
  the user script.

Bug fixes
---------

- Many bug fixes (see ChangeLog for details).


Release 2.0.0 (20 Aug 2010)
===========================

Code_Saturne 2.0 is a major (fully validated) production release, replacing
version 1.3 (which is to be maintained until the release of version 3.0).

- Correct value for the diffusion coefficient in k-omega SST.

- Move the mass-flux update in case of a rotating mesh, only relevant when
  disabling the pressure reconstruction (no impact on current simulations).

- Translate variable and property names in the example Xml files.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 2.0.0-rc1 (22 Jun 2010)
===============================

- By-pass a possible bug with the flush Fortran 2003 statement on BG systems.

- Make the particles output compliant with EnSight 6 format and improve the
  robustness of the output for visualizing with ParaView.

- Revert a changeset regarding the turbulence relaxation (k/epsilon/omega) to
  avoid stability issues in some calculations. This still needs to be
  investigated in order to have a correct unsteadyness when needed.

- Under HP-UX, handle both hppa and Itanium systems.

- Miscellaneous improvements for the parallel joining algorithm,
  added the periodicity "joining" handling in parallel by the solver.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 2.0.0-rc1 (19 Feb 2010)
===============================

- English translation of more Fortran subroutines headers.

- Move upwards the definition of additional scalars in the GUI because the
  physical properties can depend on them.

- Change the behavior of the xml file relatively to the time step min/max
  factor so that it corrresponds to what is given by the user in the gui.

- Add rotor/stator interaction (specific interpolation) for relative frame
  calculation.

- Add new interpolation schemes to code/code coupling for
  rotor/stator interaction modelling.

- Improve robustness for wall boundary conditions for atmospheric modelling.

- Use new discovery mechanism for coupling applications.

- Remove hyphens and dots from variable names defined by the GUI.

- Rename the main script in code_saturne to avoid a conflict
  with the cs executable of csound package.

- Set the relaxation factor between P0/P1 interpolations to 0.95 in multigrid
  algorithm in order to stabilize the algorithm in some calculations.

- Set the aggregation limit to 3 instead of 8 in the multigrid solver
  for better robustness (but slightly lower performance).

- Upgrade to FVM 0.15

- The space-filling-curve algorithm for backup domain splitting is activated
  by default.

- Add a mpi_io option to the command line so that one can use FVM compiled
  with MPI/IO support and decide at runtime which type of I/O to use.

- Merge the preprocessor user guide into Code_Saturne user guide.

- Add a new Python runcase script with more code coupling capabilities
  and better handling of MPI and batch environments. This scipt is enabled by
  the --new-runcase option to the "code_saturne create" command.
  The GUI still only handles the legacy (shell) script.

- Disable by default the multigrid algorithm for the potential vector
  in MHD as it does not seem to work correctly.

- Many GUI improvements and fixes.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 2.0.0-beta1 (29 Jul 2009)
=================================

- Move loop on velocity/pressure system so that it includes
  the boundary conditions calculation.

- Use selection mechanism for exchange zone definition.

- Improve cooling tower module.

- Information on SYRTHES installation and compilers can now be
  given after Code_Saturne installation.

- Fix a wrong assumed behavior on x86_64 and IA64 computers
  in the particles tracking algorithm. One assumed that the internal
  FP precision was always 80 bits (true for FPU x87 coprocessor on
  x86 processors but wrong with SSE optimizations)...
  This is a short term fix (assembler + compiler-dependent option).

- Add Coriolis source terms in standard calculations.

- Do not relax turbulent variables (k/epsilon/omega) in unsteady
  simulations.

- Adapt 1d-profiles file to SALOME format for title and labels.

- Add radiative transfer support for fuel combustion.

- Add a space-filling-curve algorithm for parallel partitioning.
  This algorithm is based on a Morton curve.

- On Linux systems, use fenv library to trap floating point exceptions.

- Add parall mesh joining feature in the Kernel (by default, the legacy
  joining feature from the Preprocessor is still used.

- Add non-neutral atmosphere modelling (both dry and humid, though
  humid atmosphere modelling is not yet fully functional).

- When detecting a divergence in the linear system solver stage, abort
  and write graphical data of the given matrix (rhs, diagonal, ...).

- Simplify running a SYRTHES 3 / Code_Saturne coupling through sockets.

- Add a mesh category for an easier management of user-defined
  post-processing.

- Add a new turbulence model for LES: the WALE model.

- Fix when testing for radiative transfer.

- Enable the multigrid algorithm for the diffusion equation in the
  electric arcs, Lagrangian, radiative transfer (P1 model) and ALE modules.

- Replace all the different user scripts by a single one.

- The GUI is now based on QT4 rather than Tk, and is now part of the
  kernel source tree to simplify version control and installation.

- The Syrthes coupling library is now included in the kernel source
  tree for easier versioning and installation.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 2.0.0-beta1 (26 May 2009)
=================================

- Add a quick reference card documentation.

- Add man pages for the main scripts to the documentation.

- Do not compile the code if there is no user file.

- Create a graphical post-processing view of the boundary

- New build system, based on the GNU Autotools.

- Conversion of all the Fortran files (headers included)
  form fixed F77 format to free f90 format. A small-case
  extension is used so that one can, in the future, skip the
  preprocessing stage.

- Change the mesh quality verification behavior. The different
  gradient calculation modes are now done in one pass. Thus, only
  one option remains for the command line (-q, with no sub-option).

- The kernel is now able to post-process edges for a given
  mesh via the PSTEDG subroutine. This functionnality is
  thus removed from the preprocessor.

- English translation of many C source files.

- Add cell renumbering capability and re-organize face renumbering.

- SYRTHES coupling upgraded to syr_cs 2.3.0.

- Upgrade checkpoint/restart to allow MPI-IO.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 1.4.0 (28 Nov. 2008)
============================

Code_Saturne 1.4 is an intermediate development release, very similar to
version 1.3.3 except for the items below:

- Add atmospheric flow modelling for neutral atmosphere flows.

- Always set the head loss tensor to be a full symmetric tensor
  in order to ease the setup within the Graphical User Interface
  (NCKPDC has been removed and replaced by the constant 6).

- Make the test on the convergence of the gradient reconstruction
  method dimensionless if the maximum control volume is greater
  than 1 (useful for some atmospheric simulations).

- Remove the forcing to ASCII mode for post-processing when
  the calculation is in verification mode.

- Remove the pipe communication mode for SYRTHES coupling.

- Add oxycombustion and fuel classes management.

- Separate preprocessing from partitioning. There is now a single
  preprocessor_output file, so that mesh joining does not need to be run again
  for a different number of processors.

- Preprocessor output, partitioning, and restart files a now use a common
  binary format (independent of the number of processors), which may be
  written or read using MPI-IO (not enabled for restart files yet).

- Scripts translation and improvements.

- The reconstruction of the right-hand side has now its own precision
  parameter (EPSRSM) instead of using EPSILO.

- Re-write of the algebric multigrid algorithm for the resolution of
  the of pressure equation. The algorithm works in serial and parallel,
  and is now the default, leading to run-times reduced by a factor or
  2 to 3 on average.

- Add wet cooling tower heat exchange specific physics model.

- The size of the work arrays IA and RA is now defined with a Fortran
  user file and no more via the scripts, making them independent of
  the number of sub-domains in case of a parallel run.

- Simplified the command line option for a parallel runs.

- Several bug fixes and minor improvements (see ChangeLog for details).


Release 1.3.3 (27 Nov 2008)
===========================

- Upgrade dependencies to FVM 0.12.0 and BFT 1.0.8.

- Upgrade SYRTHES to 3.4.2 version (syr_cs 2.1.0).  Restarting
  from SYRTHES 3.3 is not possible due to incompatible format.

- Add a QUALITY_ASSURANCE file which precises if the current
  version of Code_Saturne is validated under EDF quality
  assurance.

- Portability updates.

- Add a patch directory in which the user can find
  some untested patches fixing tricky issues.

- Updating the halos at the beginning of an outer iteration is now
  done on extended halos (reducing error with rotational periodicity).

- Improved mesh and coherency tests.

- Added localization (French or English) to the Code_Saturne Kernel
  and translated all scripts to English.

- Several bug fixes (see ChangeLog for details).


Release 1.3.2 (16 Apr 2008)
===========================

- Port to BlueGene/P and Cray XT

- Update FVM API to take into account some particular cases
  where two periodicities are not commutative.

- Add a warning when changing the mesh vertices coordinates along
  with periodicity, which can break the periodicity parameters.

- Correct distance use at the first time-step when using the k-w SST
  model and the old algorithm to compute the wall distance.

- Change the behavior when trying to get a list of cells or faces
  with the selector. Revert to the old behavior when the selection
  was done through the mesh properties. A warning is issued instead
  of an error when the criteria returns an empty selection.

- Move unmaintained macros files to aux/macros_old.

- Make Code_Saturne stop when a Lagrangian calculation is run with the
  steady-state algorithm.

- Change the name Syrthes to SYRTHES following the trademark registration.

- Add documentation on faces/cells selection with GETxxx via fvm_selector

- Add comments on steady-state algorithm IDTVAR=-1.

- Add a temporary "tmp_Saturne/$ETUDE.$CAS.$DATE" directory when running
  a case in $TMPDIR (when defined by the system) to avoid an issue
  with the linux distribution CAELinux

- Complete reorganisation of the theory documentation to follow the template
  of the user and tutorial documents

- Variant for Intel compiler on Itanium only, optimizations by BULL.

- Rename the Preprocessor listing from listenv to listpre.

- Portability improvements in scripts.

- Several bug fixes (see ChangeLog for details).


Release 1.3.1 (28 Nov 2007)
===========================

- Storage on preprocessor files in a subdirectory of
  the temporary execution directory.

- Added code_Saturne tutorial.

- synchronization with Syrthes only if ITRALE>0 in caltri.F

- creation of erreur_n*** files only for processor 0 and the
  processors receiving a segmentation fault or floating point
  exception message.

- change of kernel options "couleur" and "groupe" to "color"
  and "group" for Syrthes options.

- modification of residue test to detect when conjugate
  gradient diverges.

- Several bug fixes (see ChangeLog for details).


Release 1.3.0 (2 Aug 2007)
==========================

Code_Saturne 1.3 is a major (fully validated) production release.
Release 1.3.0 is the feature-freeze release, and versions 1.3.1
and 1.3.2 are validation bug-fix versions. 1.3.3 is the first production
version of Code_Saturne 1.3.

This version of the code is also the first version of Code_Saturne distributed
under a free software (GPL + LGPL) licence.

