code-saturne-data 4.2.0+repack-1build1 / usr / share / code_saturne / user / uslag1.f90

!-------------------------------------------------------------------------------

!                      Code_Saturne version 4.2.0
!                      --------------------------
! This file is part of Code_Saturne, a general-purpose CFD tool.
!
! Copyright (C) 1998-2015 EDF S.A.
!
! This program is free software; you can redistribute it and/or modify it under
! the terms of the GNU General Public License as published by the Free Software
! Foundation; either version 2 of the License, or (at your option) any later
! version.
!
! This program is distributed in the hope that it will be useful, but WITHOUT
! ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
! FOR A PARTICULAR PURPOSE.  See the GNU General Public License for more
! details.
!
! You should have received a copy of the GNU General Public License along with
! this program; if not, write to the Free Software Foundation, Inc., 51 Franklin
! Street, Fifth Floor, Boston, MA 02110-1301, USA.

!-------------------------------------------------------------------------------

subroutine uslag1
!================

!===============================================================================
! Purpose:
! -------

!    User subroutine of the Lagrangian particle-tracking module:

!    User subroutine for input of calculation parameters (Fortran commons).
!    This parameters concern physical, numerical and post-processing options.

!-------------------------------------------------------------------------------
! Arguments
!__________________.____._____.________________________________________________.
! name             !type!mode ! role                                           !
!__________________!____!_____!________________________________________________!
!__________________!____!_____!________________________________________________!

!     Type: i (integer), r (real), s (string), a (array), l (logical),
!           and composite types (ex: ra real array)
!     mode: <-- input, --> output, <-> modifies data, --- work array
!===============================================================================

!===============================================================================
! Module files
!===============================================================================

use paramx
use entsor
use lagdim
use lagpar
use lagran
use ihmpre

!===============================================================================

implicit none

! Local variables

integer          ii , ipv , icha
double precision sio2 , al2o3 , fe2o3 , cao

!===============================================================================


!===============================================================================
! 1. Particle-tracking mode
!===============================================================================

! iilagr = 0 : no particle tracking (default)
!        = 1 : particle-tracking one-way coupling
!        = 2 : particle-tracking two-way coupling
!        = 3 : particle tracking on frozen field
!              (this option requires a calculation restart isuite=1,
!              all Eulerian fields are frozen (pressure, velocities,
!              scalars). This option is stronger than iccvfg)

iilagr = 1

!===============================================================================
! 2. Particle-tracking calculation restart
!===============================================================================

! isuila = 0 : no restart (default)
!        = 1 : restart (this value requires a restart on the continuous
!              phase too, i.e. isuite = 1)

isuila = 0

! Restart on volume and boundary statistics, and two-way coupling terms;
! useful if isuila = 1 (defaul off: 0 ; on: 1)

if (isuila.eq.1) isuist = 0

!===============================================================================
! 3. Particle tracking: specific models
!===============================================================================

! iphyla = 0 : only transport modeling (default)
!        = 1 : equation on temperature (in Celsius degrees), diameter or mass
!        = 2 : pulverized coal combustion (only available if the continuous
!              phase is a flame of pulverized coal)

iphyla = 0

! 3.1  equation on temperature, diameter or mass

if (iphyla.eq.1) then

  ! equation on diameter
  ! (default off: 0 ; on: 1)

  idpvar = 0

  ! equation on temperature (in Celsius degrees)
  ! (default off: 0 ; on: 1)
  ! This option requires a thermal scalar for the continuous phase.

  itpvar = 0

  ! equation on mass
  ! (default off: 0 ; on: 1)

  impvar = 0

endif

! 3.2 coal fouling

! Reference internal reports EDF/R&D: HI-81/00/030/A and HI-81/01/033/A

! Evaluation of the probability for a particle to stick to a wall.
! This probability is the ratio of a critical viscosity on the
! viscosity of coal ashes

!          visref
! P(Tp) = --------   for viscen >= visref
!          viscen

!       = 1 otherwise

! The expression of J.D. Watt and T.Fereday (J.Inst.Fuel-Vol42-p99)
! is used to evaluate the viscosity of the ashes

!                     Enc1 * 1.0d+7
! Log  (10*viscen) = --------------- + Enc2
!    10                            2
!                    (Tp(C) - 150)

! In literature, the range of the critical viscosity visref is between
! 8 Pa.s and 1.D7 Pa.s  For general purpose 1.0D+4 Pa.s is chosen

if (iphyla.eq.2) then

  ! iencra = 0 no fouling (default)
  !        = 1 fouling

  ! * In uslag2.f90, the boundary on which the fouling can occur must be given
  ! * Post-processing:  iensi3 = 1 and
  ! *                   iencnbbd = 1 / iencmabd = 1 / iencdibd = 1 /iencckbd = 1 (10.2)

  iencra = 0

  ! Example of definition of fouling criteria for each coal

  ! first (and single) coal icha = 1

  icha = 1

  ! tprenc : threshold temperature below which no fouling occurs
  !          (in degrees Celcius)

  tprenc(icha) = 600.d0

  ! visref : critical viscosity (Pa.s)

  visref(icha) = 10000.d0

  ! > coal composition in mineral matters:
  !   (with  SiO2 + Al2O3 + Fe2O3 + CaO + MgO = 100% in mass)

  sio2   =  36.0d0
  al2o3  =  20.8d0
  fe2o3  =   4.9d0
  cao    =  13.3d0

  ! Enc1 and Enc2 : coefficients in Watt and Fereday expression

  enc1(icha) = 0.00835d0 * sio2 + 0.00601d0 * al2o3 - 0.109d0

  enc2(icha) =   0.0415d0 * sio2  + 0.0192d0 * al2o3                &
               + 0.0276d0 * fe2o3 + 0.016 * cao - 3.92d0

endif

!===============================================================================
! 4. Calculation features for the dispersed phases
!===============================================================================

! 4.1 Additional variables
! ------------------------

! * these additional variables are stored in eptp and eptpa arrays
! * nvls is the number of additional variables
! * the upper limit is nusvar = 10 (fixed in block common lagpar.f90)
! * one access to additional variables in eptp eptpa using the pointer jvls:

! current step  -> eptp(jvls(nvus),nbpt)
! previous step -> eptpa(jvls(nvus),npbt)

! nbpt is the number of the considered particle
!      (integer between 1 and nbpart),
! nvus is the number of the additional variable
!      (integer between 1 and nvls),
! * the integration of the associated differential stochastic equation
!   requires a user intervention in uslaed.f90 subroutine

nvls = 0

! 4.2 Steady or unsteady continuous phase

! * if steady: isttio = 1
! * if unsteady: isttio = 0
! * if iilagr = 3 then isttio = 1

! Remark: if isttio = 0, then the statistical averages are reset
!         at each lagrangian iteration

if (iilagr.ne.3) isttio = 0

! 4.3 Two-way coupling: (iilagr = 2)

if (iilagr.eq.2) then

  ! * number of absolute lagrangian iteration (i.e. with restart)
  !   from which a time average for two-way coupling source terms is
  !   computed (steady source terms)
  ! * if the Lagrangian iteration is lower than NSTITS, source terms are
  !   unsteady: they are reset at each lagrangian iteration
  ! * useful only if ISTTIO = 1.
  ! * the min value for NSTITS is 1

  nstits = 1

  ! two-way coupling for dynamic (velocities and turbulent scalars)
  ! (default off: 0 ; on: 1)
  ! (useful if ICCVFG = 0)

  ltsdyn = 0

  ! two-way coupling for mass (if IPHYLA = 1 and IMPVAR = 1)
  ! (default off: 0 ; on: 1)

  if(iphyla.eq.1 .and. (impvar.eq.1 .or. idpvar.eq.1)) ltsmas = 0

  ! two-way coupling for thermal scalar
  ! (if iphyla = 1 and impvar = 1, or iphyla = 2)
  ! or for coal variables (if IPHYLA = 2)
  ! (default off: 0 ; on: 1)

  if((iphyla.eq.1 .and. itpvar.eq.1) .or. iphyla.eq.2) ltsthe = 0

endif

! 4.4 Volume statistics
! ---------------------

! 4.4.1 Generic parameters
! ~~~~~~~~~~~~~~~~~~~~~~~~~

! Calculation of the volume statistics
! (default off: 0 ; on: 1)

istala = 0

if (istala.eq.1) then

  ! Threshold for the management of volume statistics
  ! -------------------------------------------------
  ! * the value of the seuil variable is a statistical weight.
  ! * each cell of the mesh contains a statistical weight
  !   (sum of the statistical weights of all the particles
  !   located in the cell); seuil is the minimal value from
  !   which the contribution in statistical weight of a particle
  !   is not taken into account anymore in the full model
  !   of turbulent dispersion, in the resolution of the
  !   Poisson equation of correction of the mean velocities, and
  !   in the writing of the listing and post-processing.
  !

  seuil = 0.d0

  ! Calculation of the volume statistics from the absolute number
  ! of Lagrangian iterations
  ! * idstnt is a  absolute number of Lagrangian iterations
  !   (i.e. including calculation restarts)

  idstnt = 1

  ! Steady calculation from the absolute Lagrangian iteration nstist
  ! *  nstist is a  absolute number of Lagrangian iterations
  !   (i.e. including calculation restarts) from which the statistics
  !    are averaged in time.
  ! *  useful if the calculation is steady (isttio=1)
  ! *  if the number of Lagrangian iterations is lower than nstits,
  !    the transmitted source terms are unsteady (i.e. they are reset to
  !    zero ar each Lagrangian iteration)
  ! *  the minimal value acceptable for nstist is 1.

  nstist = idstnt

  ! 4.4.2 Volume statistical variables
  ! ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

  ! Activation of the calculation of the particle volume fraction
  ! Name of the mean : Part_vol_frac

  iactfv = 1

  ! Activation of the calculation of the particle velocity x-component
  ! (mean and variance)
  ! Name of the mean: Part_velocity_X
  ! Name of the variance: var_Part_velocity_X

  iactvx = 1

  ! Activation of the calculation of the particle velocity y-component
  ! (average and variance)
  ! Name of the mean: Part_velocity_Y
  ! Name of the variance: var_Part_velocity_Y

  iactvy = 1

  ! Activation of the calculation of the particle velocity z-component
  ! (average and variance)
  ! Name of the mean: Part_velocity_Z
  ! Name of the variance: var_Part_velocity_Z

  iactvz = 1

  ! Activation of the calculation of the particle residence time
  ! (mean and variance)
  ! Name of the mean: Part_resid_time
  ! Name of the variance: var_Part_resid_time

  iactts = 1

  ! 2) Specific models (iphyla = 1) following the chosen options:
  !      Mean and variance of the temperature
  !      Mean and variance of the diameter
  !      Mean and variance of the mass

  if (iphyla.eq.1) then

    if (itpvar.eq.1) then
      ipv  = ipv  + 1
      nomlag(ipv) = 'MoTempPt'
      nomlav(ipv) = 'VaTempPt'
      ihslag(ipv)  = 2
    endif
    if (idpvar.eq.1) then
      ipv  = ipv  + 1
      nomlag(ipv) = 'MoDiamPt'
      nomlav(ipv) = 'VaDiamPt'
      ihslag(ipv)  = 2
    endif
    if (impvar.eq.1) then
      ipv  = ipv  + 1
      nomlag(ipv) = 'MoMassPt'
      nomlav(ipv) = 'VaMassPt'
      ihslag(ipv)  = 2
    endif

  else if (iphyla.eq.2) then

    ! 3) Pulverized coal (iphyla = 2) :
    !      Mean and variance of the mass
    !      Mean and variance of the temperature
    !      Mean and variance of the water mass
    !      Mean and variance of the mass of reactive coal
    !      Mean and variance of the mass of coke
    !      Mean and variance of the diameter of the shrinking core

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_mass'
    nomlav(ipv) = 'var_Part_mass'
    ihslag(ipv)  = 2

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_temperature'
    nomlav(ipv) = 'var_Part_temperature'
    ihslag(ipv)  = 2

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_wat_mass'
    nomlav(ipv) = 'var_Part_wat_mass'
    ihslag(ipv)  = 2

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_ch_mass'
    nomlav(ipv) = 'var_Part_ch_mass'
    ihslag(ipv)  = 2

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_ck_mass'
    nomlav(ipv) = 'var_Part_ck_mass'
    ihslag(ipv)  = 2

    ipv  = ipv  + 1
    nomlag(ipv) = 'Part_shrink_core_diam'
    nomlav(ipv) = 'var_Part_shrink_core_diam'
    ihslag(ipv)  = 2

  endif

  ! 4) Additional volume statistical variables
  !    ---------------------------------------
  ! * If the user wishes other statistic calculations
  !   than the standard ones, he must 1) prescribe
  !   their number nvlsts, 2) prescribe their names,
  !   3) prescribe ihslag and 4) intervene in the
  !   user subroutines uslast and uslaen to implement
  !   his new statistics (see the given examples)
  ! * Default maximal number of additional statistics: 20.
  !   (Otherwise, modify the nussta parameter is the
  !   include file lagpar.f90)

  nvlsts = 0

  if (nvlsts.gt.0) then
    do ii = 1,nvlsts
      ilvu(ii) = ipv + ii
      WRITE(NOMLAG(ILVU(II)),'(A6,I4.4)') 'MoyLag',II
      WRITE(NOMLAV(ILVU(II)),'(A6,I4.4)') 'VarLag',II
      ihslag(ilvu(ii))  = 1
    enddo
    ipv = ipv + nvlsts
  endif

  ! 6) Statistics per group:
  !    ----------------------
  ! * if the user wishes to calculate statistics per group of particles
  !   (by default there is no statistics of this kind), he must:
  !   1) prescribe nbclst the number of groups (limited to 100)
  !   2) assign in uslag2 the group to which belongs each particle
  !      through the iuslag array.
  !
  ! * Be careful, nbclst cannot be modified during a calculation restart
  !   (isuila=1); even if the calculation of the statistics is not triggered yet
  !   (istala=0).

  nbclst = 0

endif

!===============================================================================
! 6. Option concerning particle inlet
!===============================================================================

! Continous particle injection during the time step
! (and not only at the beginning the time step; this option
! makes it possible to avoid bunches of particles in the vicinity
! of the inlet zones)
! (default off: 0 ; on: 1)

injcon = 0

!===============================================================================
! 7. Techniue of variance reduction: cloning/merge of the particles
!===============================================================================

! Use of the Russian roulette
!                default off : 0
!                        on  : 1 without Y+ calculation
!                              2 with Y+ calculation

iroule = 0

!===============================================================================
! 8. Options concerning the numerical treatment of the dispersed phase
!===============================================================================

! Integration order of the stochastic differential equations
! (default 2; acceptable values 1 or 2)
!

nordre = 2

! Resolution of the Poisson equation for the particle mean velocity
! and correction of the particle instantaneous velocity
!      = 0: not correction of the velocities (default values)
!      = 1: correction of the instantaneous velocities

! Caution: OPTION STRICTLY FOR DEVELOPERS; PLEASE LEAVE THE DEFAULT VALUE FOR A
! ======== STANDARD USE OF THE CODE.           !

ilapoi = 0

!===============================================================================
! 9. Options concerning the treatment of the dispersed phase
!===============================================================================

! Caution: In this version, the turbulent dispersion works only if
! -------  the continuous phase is calculated with a k-eps or a Rij-eps model

! Activation of the turbulent dispersion
! (default on: 1 ; off: 0)

idistu = 1

! Turbulent dispersion imposed to the fluid one.

! If activated, then particle turbulent dispersion is
! equal to the fluid-particle one. The crossing-trajectory effects
! are suppressed ; it is then a case of turbulent diffusion. If the
! simulated particle density is equal to the fluid density, then
! we are simulating the displacement of fluid particles.
! (default off: 0 ; on: 1)

idiffl = 0

! modcpl :
!   = 0 for the incomplete model (default value)
!   > 0 for the full model, is equal the absolute number
!       of Lagrangian iterations from which the full model is activated
!       modcpl must not be lower than idstnt

modcpl = 0

! idirla (=1 or 2 or 3) : 1st, 2nd or 3rd direction
!   of the full model. Corresponds to the main direction
!   of the flow. Allow to calculate a non-isotropic Lagrangian timescale
!   (default idirla=1)

if (modcpl.gt.0) idirla = 1

!===============================================================================
! 10. Options concerning the treatment of specific forces
!===============================================================================
! idlvo = 0
!       = 1   dlvo deposition conditions are activated for the
!             wall with appropriate conditions idepfa (see uslag2.f90)

idlvo = 0

if (idlvo.eq.1) then

  ! Constants for the van der Waals forces
  ! --------------------------------------
  ! Hamaker constant for the particle/fluid/substrate system:

  cstham = 6.d-20

  ! Constants for the elecstrostatic forces
  !----------------------------------------

  ! Dielectric constant of the fluid (example: water at 293 K)

  epseau = 80.10d0

  ! Electrokinetic potential of the first solid - particle (Volt)

  phi_p = 50.d-3

  ! Electrokinetic potential of the second solid - surface (Volt)

  phi_s = -50.d-3

  ! Valency of ions in the solution (used for EDL forces)

  valen = 1.0d0

  ! Ionic force (mol/l)

  fion = 1.d-2

endif

!===============================================================================
! 11. Activation of Brownian motion
!===============================================================================

! Activation of Brownian motion:
! (default off: 0 ; on: 1)

! Caution: OPTION FOR DEVELOPERS ONLY
! ========

lamvbr = 0

!===============================================================================
! 12. Activation of deposition model
!===============================================================================

! Activation of the deposition model
! (default off: 0 ; on: 1)

idepst = 0

!===============================================================================
! 13. Activation of roughness and resuspension model
!===============================================================================

! Activation of the resuspension model
! (default off: 0 ; on: 1)

ireent = 0

! Caution: OPTION FOR DEVELOPERS ONLY
! ========

irough = 0  ! dlvo deposition conditions for roughness surface

! Parameters of the particle resuspension model for the roughness

!average distance between two large-scale asperities
espasg = 20.d-6

!density of the small-scale asperities
denasp = 6.36d13

!radius of small asperities
rayasp = 5.d-9

!radius of large asperities
rayasg = 2.d-6

!Young's modulus (GPa)
modyeq = 266.d9

!===============================================================================
! 14. Activation of the clogging model
!===============================================================================

! Activation of the clogging model
! (default off: 0 ; on: 1)

! Caution: OPTION FOR DEVELOPERS ONLY
! ========

iclogst = 0

! Parameters for the particle clogging model

jamlim = 0.74d0       ! Jamming limit

mporos = 0.366d0      ! Minimal porosity

csthpp = 5.0d-20      ! Hamaker constant for the particle/fluid/particle system

!===============================================================================
! 14bis. Influence of the deposit on the flow
!===============================================================================
! Activation of the influence of the deposit on the flow
! by the head losses calculation (with clogging model only)
! (default off: 0 ; on: 1)

iflow = 0

if (iflow .eq.1 ) then
iilagr = 1 !one-way coupling
isttio = 1 !the statistical averages are not reset
           !at each lagrangian iteration
endif

!===============================================================================
! 15. Activation of the precipitation/disolution model
!===============================================================================

! Activation of the precipitation/dissolution model
! (default off: 0 ; on: 1)

! Caution: OPTION FOR DEVELOPERS ONLY
ipreci = 0

!diameter of particles formed by precipitation
dprec =  2.d-6

!diameter of particles formed by precipitation
rho_preci =  5200.d0

!number of particle classes
nbrclas = 2

!===============================================================================
! 16. Variables to visualize on the trajectories or the particles
!
!     See also cs_user_postprocess_mesh in cs_user_postprocess.c to define
!     the associated visualization particle or trajectory segment meshes.
!===============================================================================

! For all the following variables, a value of 0 means "off", and 1 means "on"

! velocity of the flow seen
ivisv1  = 0

! particle velocity
ivisv2  = 0

! residence time
ivistp  = 0

! diameter
ivisdm  = 0

! temperature
if (iphyla.eq.1 .and. itpvar.eq.1) iviste  = 0

! mass
ivismp  = 0

if (iphyla.eq.2) then

  ! coal: diameter of the shrinking core
  ivisdk  = 0

  ! coal: mass of water
  iviswat  = 0

  ! coal: mass of reactive coal
  ivisch  = 0

  ! coal: mass of coke
  ivisck  = 0

endif

! 16.1 Boundary statistics: visualization of the particle/boundaries interactions
! ------------------------------------------------

! 16.1.1 Generic parameters
! ~~~~~~~~~~~~~~~~~~~~~~~~~~

! Particle/boundary interaction mode
! (default off: 0 ; on: 1)

iensi3 = 0

! Steady calculation of the boundary statistics from
! the absolute Lagrangian iteration nstbor.
! * nstbor is the absolute number of Lagrangian iterations
!   (i.e. including restarts) from which the statistics are averaged
!   (in time or by number of interactions)
! * useful if the calculation is steady (isttio=1)
! * if the absolute number of Lagrangian iterations is inferior to
!   nstbor, the statistics are unsteady (i.e. they are reset to zero at each
!   Lagrangian iteration)

nstbor = 1

! Seuilf for the management of the boundary statistics
! * the value of seuilf is a statistical weight
! * Each boundary face has undergone a number of particle interactions
!   in term of statistical weight (sum of the statistical weights of all
!   the particles that interacted with the boundary face); seuilf is the
!   minimal value from which the contribution of a face (in statistical terms)
!   is not taken into account anymore in the writing of the listing and
!   post-processing.

seuilf = 0.d0

! 16.1.2 Information to be recorded
! ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
!
! * To activate them, the user has to set below
!   the corresponding keyword to 1.
! * The default selection must be validated or modified by the user.
! * By default the asked information for all the particle/wall interactions
!   are written in the same recording.
! * The boundary statistic 'number of particle/boundary interactions' must be
!   selected to activate the particle average imoybr(...) = 2

! Number of particle/boundary interactions
! (default off: 0 ; on: 1)
inbrbd = 1

! Particle mass flux associated to particle/boundary interactions
! (default off: 0 ; on: 1)
iflmbd = 1

! Angle between particle velocity and the plan of the boundary face
! (default off: 0 ; on: 1)
iangbd = 0

! Norm of particle velocity during the interation with the boundary face
! (default off: 0 ; on: 1)
ivitbd = 0

! (default off: 0 ; on: 1)
 if (iphyla.eq.2 .and. iencra.eq.1) then
   ! Number of particle/boundary interactions with fouling
   iencnbbd = 0
   ! Mass of fouled coal particles
   iencmabd = 0
   ! Diameter of fouled coal particles
   iencdibd = 0
   ! Coke fraction of fouled coal particles
   iencckbd = 0
 endif
! Additional user information to be recorded
! ------------------------------------------
! (for instance, erosion rate, temperature..)
! * these additional recordings are stored in the parbor array
! * here we prescribe the nusbor number of additional recordings
! * the max value of this number is nusbrd=10 (in lagpar.f90)

nusbor = 0

! 16.1.3 Name of the recordings for display,
!        Average in time of particle average
!        of the boundary statistics
! ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

! * A priori the user intervenes only in the additional user information
!   to be recorded: he must prescribe the name of the recording as well as
!   the type of average that he wishes to apply to it for the writing
!   of the listing and the post-processing.

! * The applied average is prescribed through the imoybr array:
!   - if imoybr(iusb(ii)) = 0 -> no average applied
!   - if imoybr(iusb(ii)) = 1 -> a time average is applied, i.e. the
!     statistic is divided by the last time step in the case of an unsteady
!     calculation with a number of iterations lower than nstbor; or that
!     the statistic is divided by the recording time in the case of a
!     steady calculation.
!    -if imoybr(iusb(ii)) = 2 -> a particle average is applied, i.e. the
!     statistic is divided by the number of recorded particle/boundary
!     interactions (in terms of statistical weight) in parbor(nfabor,inbr)
!     To use this average, inbrbd must be set to 1.
!   - if imoybr(iusb(ii)) = 3 -> (coal fouling only) a particle average
!     is applied, i.e. the statistic is divided by the number of recorded
!     particle/boundary interactions with fouling (in terms of statistical
!     weight) in parbor(nfabor,inbr), To use this average, iencnbbd must be
!     set to 1.
! * The back-ups in the restart file are performed without applying
!   this average.
! * The average is applied if the number of interactions (in statistical
!   weight) of the boundary face considered is greater than seuilf;
!   otherwise this average is set to zero.

!===============================================================================
! 17. Lagrangian listing
!===============================================================================

! Lagrangian period for the writing of the Lagrangian listing

ntlal = 1

!===============================================================================

return

end subroutine uslag1