!------------------------------------------------------------------------------- ! Code_Saturne version 4.0.2 ! -------------------------- ! 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. !------------------------------------------------------------------------------- ! Purpose: ! ------- ! User subroutines for input of calculation parameters (Fortran modules). ! These subroutines are called in all cases. ! If the Code_Saturne GUI is used, this file is not required (but may be ! used to override parameters entered through the GUI, and to set ! parameters not accessible through the GUI). ! Several routines are present in the file, each destined to defined ! specific parameters. ! To modify the default value of parameters which do not appear in the ! examples provided, code should be placed as follows: ! - usipsu for numerical and physical options ! - usipes for input-output related options ! As a convention, "specific physics" defers to the following modules only: ! pulverized coal, gas combustion, electric arcs. ! In addition, specific routines are provided for the definition of some ! "specific physics" options. ! These routines are described at the end of this file and will be activated ! when the corresponding option is selected in the usppmo routine. !------------------------------------------------------------------------------- !=============================================================================== subroutine usppmo & !================ ( ixmlpu ) !=============================================================================== ! Purpose: ! ------- ! User subroutine. ! Define the use of a specific physics amongst the following: ! - combustion with gas / coal / heavy fuel oil ! - compressible flows ! - electric arcs ! - atmospheric modelling ! - radiative transfer ! - cooling towers modelling ! Only one specific physics module can be activated at once. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! name !type!mode ! role ! !__________________!____!_____!________________________________________________! ! ixmlpu ! i ! <-- ! indicates if the XML file from the GUI is ! ! ! ! ! used (1: yes, 0: no) ! !__________________!____!_____!________________________________________________! ! 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 cstphy use ppppar use ppthch use ppincl use ppcpfu use coincl use radiat use cs_c_bindings !=============================================================================== implicit none ! Arguments integer ixmlpu !=============================================================================== ! 1. Choice for a specific physics !=============================================================================== ! --- cod3p: Diffusion flame with complete fast chemistry (3 points) ! ========== ! if = -1 module not activated ! if = 0 adiabatic model ! if = 1 extended model with enthalpy source term if (ixmlpu.eq.0) then ippmod(icod3p) = -1 endif ! --- coebu: Eddy-Break Up pre-mixed flame ! ========== ! if = -1 module not activated ! if = 0 reference Spalding model ! (adiabatic, homogeneous mixture fraction) ! if = 1 extended model with enthalpy source term ! (homogeneous mixture fraction : perfect premix) ! if = 2 extended model with mixture fraction transport ! (adiabatic, no variance of mixture fraction) ! if = 3 extended model with enthalpy and mixture fraction transport ! (dilution, thermal losses, etc.) if (ixmlpu.eq.0) then ippmod(icoebu) = -1 endif ! --- colwc: Libby-Williams pre-mixed flame ! ========== ! if = -1 module not activated ! if = 0 reference two-peak model with adiabatic condition ! if = 1 extended two-peak model with enthapy source terms ! if = 2 extended three-peak model, adiabatic ! if = 3 extended three-peak model with enthalpy source terms ! if = 4 extended four-peak model, adiabatic ! if = 5 extended four-peak model with enthalpy source terms if (ixmlpu.eq.0) then ippmod(icolwc) = -1 endif ! --- Soot model ! ================= ! if = -1 module not activated ! if = 0 constant fraction of fuel Xsoot ! if = 1 2 equations model of Moss et al. if (.false.) then isoot = 0 xsoot = 0.1d0 ! ( if isoot = 0 ) rosoot = 2000.d0 ! kg/m3 endif ! --- cfuel: Heavy fuel oil combustion ! ========== ! Progressive evaporation (temperature gap) ! Char residue ! Sulphur tracking ! if = -1 module not activated ! if = 0 module activated if (ixmlpu.eq.0) then ippmod(icfuel) = -1 endif ! --- coal : ! ========== ! ! Pulverized coal combustion ! Description of granulometry ! Assumption of diffusion flame around particles ! (extension of 3-point fast chemistry "D3P") ! Between a mixture of gaseous fuels (volatiles matters, CO from char ! oxydation) ! and a mixture of oxidisers (air and water vapor) ! Enthalpy for both mix and solid phase are solved ! ! if = -1 module not activated ! if = 0 module activated ! if = 1 with drying if (ixmlpu.eq.0) then ippmod(iccoal) = -1 endif ! Activate the drift: 0 (no activation), ! 1 (transported particle velocity) ! 2 (limit drop particle velocity) if (.false.) then i_coal_drift = 1 endif ! --- cpl3c: Pulverized coal with Lagrangian reciprocal approach ! ========== ! Not recently tested... at least outdated, may be obsolete ! if = -1 module not activated ! if = 0 module activated ! if = 1 with drying (NOT functional) if (ixmlpu.eq.0) then ippmod(icpl3c) = -1 endif ! --- compf: Compressible flows ! ========== ! if = -1 module not activated ! if = 0 module activated if (ixmlpu.eq.0) then ippmod(icompf) = -1 endif ! --- eljou: Joule effect ! ========== ! if = -1 module not activated ! if = 1 Potentiel reel ! if = 2 Potentiel complexe ! if = 3 Potentiel reel + CDL Transfo ! if = 4 Potentiel complexe + CDL Transfo if (ixmlpu.eq.0) then ippmod(ieljou) = -1 endif ! --- elarc: Electric arcs ! ========== ! if = -1 module not activated ! if = 1 electric potential ! if = 2 electric potential and vector potential (hence 3D modelling) if (ixmlpu.eq.0) then ippmod(ielarc) = -1 endif ! --- atmos: Atmospheric flows ! ========== ! if = -1 module not activated ! if = 0 standard modelling ! if = 1 dry atmosphere ! if = 2 humid atmosphere (experimental) if (ixmlpu.eq.0) then ippmod(iatmos) = -1 endif ! --- aeros: Cooling towers ! ========== ! if = -1 module not activated ! if = 0 no model (NOT functional) ! if = 1 Poppe's model ! if = 2 Merkel's model if (ixmlpu.eq.0) then ippmod(iaeros) = -1 endif ! --- igmix: Gas mixtures modelling ! ========== ! if =-1 module not activated ! if = 0 Air/Helium gas mixtures ! if = 1 Air/Hydrogen gas mixtures ! if = 2 Air/Steam gas mixtures ! if = 3 Air/Helium/Steam gas mixtures ! if = 4 Air/Hydrogen/Steam gas mixtures if (.false.) then ippmod(igmix) = 0 endif ! Radiative transfer module (iirayo) !-------------------------- ! if = 0: not activated (Default) ! if = 1: DOM ! if = 2: approximation P1 method if (.false.) then iirayo = 1 endif ! --- richards model ! ========== ! if = -1 module not activated ! if = 1 module activated if (.false.) then ippmod(idarcy) = -1 endif !=============================================================================== ! 2. Specific options related to herebefore modules !=============================================================================== ! These options are defined here at the moment, this might change in the future ! --- Enthalpy-Temperature conversion law (for gas combustion modelling) ! if = 0 user-specified ! if = 1 tabulated by JANAF (default) if (ixmlpu.eq.0) then indjon = 1 endif ! --- Kinetic model for CO <=> CO2 ! Compatible with coal and heavy fuel oil combustion ! if = 0 unused (maximal conversion in turbulent model) ! if = 1 transport of CO2 mass fraction ! if = 2 transport of CO mass fraction if (ixmlpu.eq.0) then ieqco2 = 0 endif !=============================================================================== ! 2. Data file related to modules above !=============================================================================== if (ixmlpu.eq.0) then ! Combustion if ( ippmod(icod3p).ge.0 & .or. ippmod(icoebu).ge.0 .or. ippmod(icolwc).ge.0) then if (indjon.eq.1) then ficfpp = 'dp_C3P' else ficfpp = 'dp_C3PSJ' endif endif ! Fuel combustion if (ippmod(icfuel).ge.0) then ficfpp = 'dp_FUE' endif ! Electric arcs if (ippmod(ielarc).ge.1) then ficfpp = 'dp_ELE' endif ! Joule effect if (ippmod(ieljou).eq.1 .or. ippmod(ieljou).eq.2) then ficfpp = 'dp_ELE' else if (ippmod(ieljou).eq.3 .or. ippmod(ieljou).eq.4) then ficfpp = 'dp_transfo' endif ! Atmospheric flows if (ippmod(iatmos).ge.0) then ficmet = 'meteo' endif if ( ippmod(igmix).ge.0 ) then !> Specific condensation modelling !> if = -1 module not activated !> if = 0 condensation source terms activated !> if = 1 condensation source terms with metal !> structures activate icond = -1 endif endif !---- ! End !---- return end subroutine usppmo !=============================================================================== subroutine usipph & !================ ( ixmlpu, iturb , itherm, iale , icavit ) !=============================================================================== ! Purpose: ! -------- ! User subroutine for input of parameters. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! name !type!mode ! role ! !__________________!____!_____!________________________________________________! ! ixmlpu ! i ! <-- ! indicates if the XML file from the GUI is ! ! ! ! ! used (1: yes, 0: no) ! ! iturb ! i ! <-> ! turbulence model ! ! itherm ! i ! <-> ! thermal model ! ! iale ! i ! <-> ! ale module ! ! icavit ! i ! <-> ! cavitation model ! !__________________!____!_____!________________________________________________! ! 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 entsor, only: nfecra ! No other module should appear here !=============================================================================== implicit none ! Arguments integer ixmlpu integer iturb, itherm, iale, icavit ! Local variables !=============================================================================== !=============================================================================== ! In this subroutine, only the parameters which already appear may ! be set, to the exclusion of any other. ! ================ ! If we are not using the Code_Saturne GUI: ! All the parameters which appear in this subroutine must be set. ! === ! If we are using the Code_Saturne GUI: ! parameters protected by a test of the form: ! if (ixmlpu.eq.0) then ! ... ! endif ! should already have been defined using the GUI, so only ! experts should consider removing the test and adapting them here. !=============================================================================== ! --- Turbulence ! 0: Laminar ! 10: Mixing length ! 20: k-epsilon ! 21: k-epsilon (linear production) ! 30: Rij-epsilon, (standard LRR) ! 31: Rij-epsilon (SSG) ! 32: Rij-epsilon (EBRSM) ! 40: LES (Smagorinsky) ! 41: LES (Dynamic) ! 42: LES (WALE) ! 50: v2f (phi-model) ! 51: v2f (BL-v2/k) ! 60: k-omega SST ! 70: Spalart Allmaras ! For 10, contact the development team before use if (ixmlpu.eq.0) then iturb = 42 endif ! --- Thermal model ! 0: none ! 1: temperature ! 2: enthalpy ! 3: total energy (only for compressible module) ! ! For temperature, the temperature scale may be set later using itpscl ! (1 for Kelvin, 2 for Celsius). ! ! Warning: When using specific physics, this value is ! set automatically by the physics model. if (.true.) then itherm = 2 endif ! --- Cavitation module ! - -1: module not activated ! - 0: no vaporization/condensation model ! - 1: Merkle's model ! ! Specific cavitation module input parameters should be set usipsu ! (see example in cs_user_parameters-cavitation.f90) ! if (.false.) then icavit = -1 endif ! --- Activation of ALE (Arbitrary Lagrangian Eulerian) method if (.false.) then iale = 1 endif !---- ! Formats !---- return end subroutine usipph !=============================================================================== subroutine usipsu & !================ ( nmodpp ) !=============================================================================== ! Purpose: ! ------- ! User subroutine for the input of additional user parameters. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! name !type!mode ! role ! !__________________!____!_____!________________________________________________! ! nmodpp ! i ! <-- ! number of active specific physics models ! !__________________!____!_____!________________________________________________! ! 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 cstnum use dimens use numvar use optcal use cstphy use entsor use parall use period use ihmpre use albase use ppppar use ppthch use ppincl use coincl use cpincl use elincl use field use cavitation use rotation !=============================================================================== implicit none ! Arguments integer nmodpp ! Local variables logical ilved, inoprv integer ii, jj, kscmin, kscmax, keydri integer f_id, idim1, itycat, ityloc, iscdri, iscal, ifcvsl !=============================================================================== ! This subroutine allows setting parameters ! which do not already appear in the other subroutines of this file. ! It is possible to add or remove parameters. ! The number of physical properties and variables is known here. !=============================================================================== ! Calculation options (optcal) ! ============================ ! In case of restart, read auxiliary restart file ileaux (= 1) or not (0). ! By default, this file is read, but it may be useful to deactivate ! its use when restarting after a preprocessing stage possibly leading ! to a different number of faces (such as simply joining meshes on ! a different architecture or optimization level or with different options). ! Writing of auxiliary restart files may also be deactivated using: iecaux = 0 if (.false.) then ileaux = 0 endif ! --- Time stepping (0 : uniform and constant ! 1 : variable in time, uniform in space ! 2 : variable in time and space ! -1 : steady algorithm) if (.true.) then idtvar = 0 endif ! --- Duration ! ntmabs = absolute number of the last time step required ! if we have already run 10 time steps and want to ! run 10 more, ntmabs must be set to 10 + 10 = 20 if (.true.) then ntmabs = 16000 endif ! --- Reference time step ! The example given below is probably not adapted to your case. if (.true.) then dtref = 0.0001d0 endif ! --- Maximum time step: dtmax ! Set a value base on characteristic values of your case. ! otherwise, the code will use a multiple of dtref by default. ! Example with ! Ld: "dynamic" length (for example, the domain length) ! Ud: characteristic flow velocity ! Lt: thermal length (for example, the domain height gravity-wise) ! Delta_rho/rho: relative density difference ! g: gravity acceleration ! dtmax = min(Ld/Ud, sqrt(Lt/(g.Delta_rho/rho))) ! --- Handling of hydrostatic pressure ! iphydr = 0 : ignore hydrostatic pressure (by default) ! 1 : with hydrotatic pressure computation to handle the balance ! between the pressure gradient and source terms (gravity and ! head losses) ! 2 : with hydrostatic pressure computation to handle the imbalance ! between the pressure gradient and gravity source term if (.false.) then iphydr = 1 endif ! --- Algorithm to take into account the density variation in time ! ! idilat = 0 : Boussinesq algorithm with constant density (not available) ! 1 : dilatable steady algorithm (default) ! 2 : dilatable unsteady algorithm ! 3 : low-Mach algorithm if (.false.) then idilat = 1 endif ! --- Temperature or enthalpy ! When used without specific physics, if we have chosen to solve in temperature ! (that is if itherm = 1), the fluid temperature is considered to be in ! degrees Kelvin by default (be careful for boundary conditions an expression ! of physical properties depending on temperature)t. ! If we wish for the fluid solver to work with a temperature in degrees Celsius, ! we must set itpscl = 2. ! This is recommended for Syrthes Coupling, but not recommended for the ! radiative model, as it is a source of user errors in this case: ! Indeed, the boundary conditions for the fluid temperature will then be ! in degrees Celsius, while the boundary conditions for radiation in ! cs_user_radiative_transfer_bcs.f90 must still be in Kelvin. if (.false.) then if (nmodpp.eq.0) then itpscl = 2 endif endif ! If a USER scalar behaves like a temperature (relative to Cp): ! we set iscacp(isca) = 1. ! ! Otherwise, we do not modify iscacp(isca) if (.false.) then if (nscaus.gt.0) then do ii = 1, nscaus iscacp(isca(ii)) = 1 enddo endif endif ! --- Solver taking a scalar porosity into account: ! 0 No porosity taken into account (Standard) ! 1 Porosity taken into account ! if (.false.) then iporos = 1 endif ! --- Calculation (restart) with frozen velocity field (1 yes, 0 no) if (.false.) then iccvfg = 1 endif ! --- Vortex method for inlet conditions in L.E.S. ! (0: not activated, 1: activated) ! The vortex method only regards the L.E.S. models ! To use the vortex method, edit the 'usvort.f90' user file. if (.true.) then if (itytur.eq.4) then ivrtex = 0 endif endif ! --- Velocity/pressure coupling (0 : classical algorithm, ! 1 : transient coupling) if (.true.) then ipucou = 0 endif ! --- Convective scheme ! blencv = 0 for upwind (order 1 in space, "stable but diffusive") ! = 1 for centered/second order (order 2 in space) ! we may use intermediate real values. ! Here we choose: ! for the velocity and user scalars: ! an upwind-centered scheme with 100% centering (blencv=1) ! for other variables ! the default code value (upwind standard, centered in LES) ! Specifically, for user scalars ! if we suspect an excessive level of numerical diffusion on ! a variable ivar representing a user scalar ! iscal (with ivar=isca(iscal)), it may be useful to set ! blencv(ivar) = 1.0d0 to use a second-order scheme in space for ! convection. For temperature or enthalpy in particular, we ! may thus choose in this case: ! blencv(isca(iscalt)) = 1.0d0 ! For non-user scalars relative to specific physics (coal, combustion, ! electric arcs: see usppmo) implicitly defined by the model, ! the corresponding information is set automatically elsewhere: ! we do not modify blencv here. if (.true.) then blencv(iu) = 1.0d0 blencv(iv) = 1.0d0 blencv(iw) = 1.0d0 if (nscaus.ge.1) then do ii = 1, nscaus blencv(isca(ii)) = 1.0d0 enddo endif endif ! --- Linear solver parameters (for each unknown) ! epsilo: relative precision for the solution of the linear system. if (.false.) then if (nscaus.ge.1) then do ii = 1, nscaus epsilo(isca(ii)) = 1.d-6 enddo endif endif ! --- Dynamic reconstruction sweeps to handle non-orthogonlaities ! This parameter computes automatically a dynamic relax factor, ! and can be activated for any variable. ! - iswdyn(ipr) = 1: means that the last increment is relaxed ! - iswdyn(ipr) = 2: means that the last two increments are used to ! relax ! NB: when iswdyn is greater than 1, then the number of ! non-orthogonality sweeps is increased to 20. if (.false.) then iswdyn(ipr) = 1 endif ! --- Rotation/curvature correction for eddy-viscosity turbulence models ! 0: deactivated ! 1: activated if (.false.) then irccor = 1 endif ! --- Stabilization in turbulent regime ! For difficult cases, a stabilization may be obtained by not ! reconstructing the convective and diffusive flux for variables ! of the turbulence model, that is ! in k-epsilon: if (itytur.eq.2) then ! ircflu(ik) = 0 and ircflu(iep) = 0 ! in Rij-epsilon: if (itytur.eq.3) then ! ircflu(ir11) = 0, ircflu(ir22) = 0, ! ircflu(ir33) = 0, ! ircflu(ir12) = 0, ircflu(ir23) = 0, ! ircflu(ir23) = 0, ! and ircflu(iep) = 0 ! (note that variable itytur is equal to iturb/10) if (.false.) then if (itytur.eq.2) then ircflu(ik) = 0 ircflu(iep) = 0 endif endif ! --- Turbulent diffusion model for second moment closure (iturb = 3x) ! 0: scalar diffusivity (Shir model) ! 1: tensorial diffusivity (Daly and Harlow model, default model) if (.false.) then if (itytur.eq.3) then idirsm = 1 endif endif ! Physical constants (cstphy) ! =========================== ! --- gravity (g in m/s2, with the sign in the calculation coordinate axes). if (.true.) then gx = 0.d0 gy = 0.d0 gz = 0.d0 endif ! --- rotation of the reference frame (omega in s-1) ! If the rotation is not nul, then ! icorio = 0: rotation is taken into account by rotating the mesh ! (simulation in the absolute frame) ! = 1: rotation is taken into account by Coriolis source terms ! (simulation in the relative frame) if (.false.) then icorio = 0 call rotation_define(0.d0, 0.d0, 0.d0, & ! rotation vector 0.d0, 0.d0, 0.d0) ! invariant point endif ! --- Reference fluid properties ! ro0 : density in kg/m3 ! viscl0 : dynamic viscosity in kg/(m s) ! cp0 : specific heat in J/(Kelvin kg) ! t0 : reference temperature in Kelvin ! p0 : total reference pressure in Pascal ! the calculation is based on a ! reduced pressure P*=Ptot-ro0*g.(x-xref) ! (except in compressible case) ! xyzp0(3) : coordinates of the reference point for ! the total pressure (where it is equal to p0) ! In general, it is not necessary to furnish a reference point xyz0. ! If there are outlets, the code will take the center of the ! reference outlet face. ! On the other hand, if we plan to explicitly fix Dirichlet conditions ! for pressure, it is better to indicate to which reference the ! values relate (for a better resolution of reduced pressure). ! Other properties are given by default in all cases. ! Nonetheless, we may note that: ! In the standard case (no gas combustion, coal, electric arcs, ! compressibility): ! --------------------- ! ro0, viscl0 and cp0 ! are useful and represent either the fluid properties if they ! are constant, either simple mean values for the initialization ! if properties are variable and defined in usphyv. ! t0 is not useful ! p0 is useful but is not used in an equation of state. p0 ! is a reference value for the incompressible solver ! which will serve to set the (possible) domain outlet pressure. ! We may also take it as 0 or as a physical value in Pascals. ! With the electric module: ! ------------------------ ! ro0, viscl0 and cp0 ! are useful but simply represent mean initial values; ! the density, molecular dynamic viscosity, and specific ! heat are necessarily given in propce (whether they are ! physically variable or not): see uselph for the Joule effect ! module and the electric arcs dp_ELE data file. ! t0 is useful an must be in Kelvin (> 0) but represents a simple ! initialization value. ! p0 is useful bu is not used in the equation of state. p0 ! is a reference value for the incompressible solver which ! will be used to calibrate the (possible) outlet pressure ! of the domain. We may take it as zero or as a physical ! value in Pascals. ! With gas combustion: ! -------------------- ! ro0 is not useful (it is automatically recalculated by the ! law of ideal gases from t0 and p0). ! viscl0 is indispensable: it is the molecular dynamic viscosity, ! assumed constant for the fluid. ! cp0 is indispensable: it is the heat capacity, assumed constant, ! (modelization of source terms involving a local Nusselt in ! the Lagrangian module, reference value allowing the ! calculation of a radiative ! (temperature, exchange coefficient) couple). ! t0 is indispensible and must be in Kelvin (> 0). ! p0 is indispensable and must be in Pascal (> 0). ! With pulverized coal: ! --------------------- ! ro0 is not useful (it is automatically recalculated by the ! law of ideal gases from t0 and p0). ! viscl0 is indispensable: it is the molecular dynamic viscosity, ! assumed constant for the fluid (its effect is expected to ! be small compared to turbulent effects). ! cp0 is indispensable: it is the heat capacity, assumed constant, ! (modelization of source terms involving a local Nusselt in ! the coal or Lagrangian module, reference value allowing the ! calculation of a radiative ! (temperature, exchange coefficient) couple). ! t0 is indispensable and must be in Kelvin (> 0). ! p0 is indispensable and must be in Pascal (> 0). ! With compressibility: ! --------------------- ! ro0 is not useful, stricto sensu; nonetheless, as experience ! shows that users often use this variable, it is required ! to assign to it a strictly positive value (for example, ! an initial value). ! viscl0 is useful and represents the molecular dynamic viscosity, ! when it is constant, or a value which will be used during ! initializations (or in inlet turbulence conditions, ! depending on the user choice. ! cp0 is indispensable: it is the heat capacity, assumed constant ! in the thermodynamics available by default ! t0 is indispensable and must be in Kelvin (> 0). ! p0 is indispensable and must be in Pascal (> 0). ! With the thermodynamic law available by default, ! t0 and p0 are used for the initialization of the density. ! xyzp0 is not useful because the pressure variable directly ! represents the total pressure. if (.true.) then ro0 = 589.13d0 viscl0 = 6.8078d-5 cp0 = 8079.6d0 endif if (.true.) then t0 = 633.0d0 p0 = 25.0d6 endif ! --- irovar, ivivar, icp: constant or variable density, ! viscosity/diffusivity, and specific heat ! When a specific physics module is active ! (coal, combustion, electric arcs, compressible: see usppmo) ! we MUST NOT set variables 'irovar', 'ivivar', and 'icp' here, as ! they are defined automatically. ! Nonetheless, for the compressible case, ivivar may be modified ! in the uscfx2 user subroutine. ! When no specific physics module is active, we may specify if the ! density, specific heat, and the molecular viscosity ! are constant (irovar=0, ivivar=0, icp=0), which is the default ! or variable (irovar=1, ivivar=1, icp=1) ! For those properties we choose as variable, the corresponding law ! must be defined in usphyv ! (incs_user_physical_properties.f90); ! if they are constant, they take values ro0, viscl0, and cp0. if (.true.) then irovar = 1 ivivar = 1 icp = 1 endif ! We only specify XYZ0 if we explicitely fix Dirichlet conditions ! for the pressure. if (.false.) then xyzp0(1) = 0.d0 xyzp0(2) = 0.d0 xyzp0(3) = 0.d0 endif ! --- Minimum and maximum admissible values for each USER scalar: ! Results are clipped at the end of each time step. ! If min > max, we do not clip. ! For a scalar jj representing the variance of another, we may ! abstain from defining these values ! (a default clipping is set in place). ! This is the purpose of the test on iscavr(jj) in the example below. ! For non-user scalars relative to specific physics (coal, combustion, ! electric arcs: see usppmo) implicitly defined according to the ! model, the information is automatically set elsewhere: we ! do not set min or max values here. if (.false.) then call field_get_key_id("min_scalar_clipping", kscmin) call field_get_key_id("max_scalar_clipping", kscmax) ! Thermal scalar: if (iscalt.gt.0) then ! We define the min and max bounds call field_set_key_double(ivarfl(isca(iscalt)), kscmin, -grand) call field_set_key_double(ivarfl(isca(iscalt)), kscmax, +grand) endif ! Loop on user scalars: do jj = 1, nscaus ! For scalars which are not variances if (iscavr(jj).le.0) then ! We define the min and max bounds call field_set_key_double(ivarfl(isca(jj)), kscmin, -grand) call field_set_key_double(ivarfl(isca(jj)), kscmax, +grand) endif enddo endif ! --- Reference diffusivity visls0 in kg/(m s) for each ! USER scalar except those which represent the variance of another. ! For non-user scalars relative to specific physics (coal, combustion, ! electric arcs: see usppmo) implicitly defined in the model, ! the information is given automatically elsewhere: ! we do not modify visls0 here. ! For user scalars JJ which represent the variance of another user ! scalar, we do not define visls0(jj) here. ! This is the purpose of the test on iscavr(jj) in the example below. ! Indeed the diffusivity of the variance of a scalar is assumed ! identical to that scalar's diffusivity. ! For user scalars jj behaving as a temperature (iscacp(jj) = 1), ! Cp is outside of the diffusion term in the temperature equation, so: ! visls0(jj) = Lambda ! For user scalars jj NOT behaving as a temperature (iscacp(jj) = 0), ! visls0(jj) = Lambda/Cp ! Here, as an example, we assign to viscl0 the viscosity of the fluid ! phase, which is fitting for passive tracers which follow the fluid ! (this is also the default used if not modified here or using the GUI). if (.true.) then ! Thermal model: ! In case of specific physic, this value could be automatically set and should ! not be modified. !~ if (iscalt.gt.0) visls0(iscalt) = viscl0 ! We loop on user scalars: do jj = 1, nscaus ! For scalars which are not variances if (iscavr(jj).le.0) then ! We define the scalar diffusivity ! visls0(jj) = viscl0 visls0(jj) = 5.763d-5 endif enddo endif ! --- Variable diffusivity field id (ifcvsl>=0) or constant ! diffusivity (ifcvsl=-1) for the thermal scalar and USER scalars. ! With ifcvsl = 0, the field will be added automatically, and later calls to ! field_get_key_int(ivarfl(isca(iscal)), kivisl, ifcvsl) ! will return its id. ! With ifcvsl > 0, the id of an existing, predifined field is given. This ! may allow sharing a diffusivity between multiple scalars. ! For user scalars iscal which represent the variance of another user ! scalar, the diffusivity of the variance of a scalar is assumed to ! have the same behavior as the diffusivity of this scalar, ! so values set here will be ignored. ! For non-user scalars relative to specific physics (coal, combustion, ! electric arcs: see usppmo) implicitly defined in the model, ! the diffusivity should not be modified here. ! Caution: complete usphyv with the law defining the diffusivity ! ======== if and only if ifcvsl = 0 has been set here. if (.true.) then ! For thermal scalar if (iscalt.gt.0) call field_set_key_int(ivarfl(isca(iscalt)), kivisl, ifcvsl) do iscal = 1, nscaus if (iscavr(iscal).le.0) then ifcvsl = 0 call field_set_key_int(ivarfl(isca(iscal)), kivisl, ifcvsl) endif enddo endif ! --- Turbulent flux model u'T' for the scalar T ! Algebraic Model ! 0 SGDH ! 10 GGDH ! 20 AFM ! Model with transport equations ! 30 DFM if (.false.) then ! GGDH for thermal scalar: if (iscalt.gt.0) iturt(iscalt) = 10 ! GGDH for all the scalars: do jj = 1, nscaus iturt(jj) = 10 enddo endif ! --- Reference velocity for turbulence initialization (m2/s) ! (useful only with turbulence) if (.true.) then uref = 0.0030447d0 endif ! --- Reference length scale in meters for initialization ! of epsilon (and specific clipping of turbulence, but ! this is not the default option) ! Assign a value of the order of the largest dimension of the ! physical domain in which the flow may develop. ! If a negative value is set here, or no value set and the GUI not ! used, the cubic root of the domain will be used. ! (useful only for turbulence). if (.false.) then almax = 0.5 endif ! --- Scalar with a drift (key work "drift_scalar_model">0) or without drift ! ((key work "drift_scalar_model"=0, default option) for each USER scalar. ! - to specify that a scalar have a drift and need the drift computation: ! iscdri = ibset(iscdri, DRIFT_SCALAR_ADD_DRIFT_FLUX) ! ! --- Then, for each scalar with a drift, add a flag to specify if ! specific terms have to be taken into account: ! - thermophoresis terms: ! iscdri = ibset(iscdri, DRIFT_SCALAR_THERMOPHORESIS) ! - turbophoresis terms: ! iscdri = ibset(iscdri, DRIFT_SCALAR_TURBOPHORESIS) ! - centrifugal force terms: ! iscdri = ibset(iscdri, DRIFT_SCALAR_CENTRIFUGALFORCE) if (.false.) then ! Key id for drift scalar call field_get_key_id("drift_scalar_model", keydri) if (nscaus.ge.1) then iscdri = 1 iscdri = ibset(iscdri, DRIFT_SCALAR_ADD_DRIFT_FLUX) if (.false.) then iscdri = ibset(iscdri, DRIFT_SCALAR_THERMOPHORESIS) endif if (.false.) then iscdri = ibset(iscdri, DRIFT_SCALAR_TURBOPHORESIS) endif if (.false.) then iscdri = ibset(iscdri, DRIFT_SCALAR_CENTRIFUGALFORCE) endif iscal = 1 f_id = ivarfl(isca(iscal)) ! Set the key word "drift_scalar_model" into the field structure call field_set_key_int(f_id, keydri, iscdri) endif endif ! Postprocessing-related fields ! ============================= ! Example: enforce existence of 'yplus', 'tplus' and 'tstar' fields, so that ! yplus, a boundary temperature or Nusselt number may be computed using ! the post_boundary_temperature or post_boundary_nusselt subroutines. ! When postprocessing of these quantities is activated, those fields ! are present, but if we need to compute them in the ! cs_user_extra_operations user subroutine without postprocessing them, ! forcing the definition of these fields to save the values computed ! for the boundary layer is necessary. if (.false.) then itycat = FIELD_INTENSIVE + FIELD_PROPERTY ityloc = 3 ! boundary faces idim1 = 1 ! dimension ilved = .true. ! interleaved inoprv = .false. ! no previous time step values needed call field_get_id_try('yplus', f_id) if (f_id.lt.0) then call field_create('yplus', itycat, ityloc, idim1, ilved, inoprv, f_id) ! yplus postreated and in the log call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) endif call field_get_id_try('tplus', f_id) if (f_id.lt.0) then call field_create('tplus', itycat, ityloc, idim1, ilved, inoprv, f_id) ! tplus postreated and in the log call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) endif call field_get_id_try('tstar', f_id) if (f_id.lt.0) then call field_create('tstar', itycat, ityloc, idim1, ilved, inoprv, f_id) ! tplus postreated and in the log call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) endif endif ! Error estimators for Navier-Stokes (non-frozen velocity field) ! We recommend running a calculation restart on a few time steps ! with the activation of the most interesting of those. ! (=2 to activate, =0 to deactivate). if (.false.) then iescal(iescor) = 2 ! div(rho u) -Gamma iescal(iestot) = 2 ! resolution precision for the momentum endif ! ALE (Arbitrary Lagrangian Eulerian) related options !==================================================== ! Number of iterations for fluid initialization. Contrary to ntmabs, ! nalinf is not an absolute iteration number, meaning that in case of ! restart calculation nalinf corresponds to the number of iterations ! for fuid initialization beginning from the first current iteration of ! the calculation restart. In general nalinf = 0 in that case. if (.false.) then nalinf = 75 endif ! Maximum number of iterations in case of implicit Fluid Structure Coupling ! with structural calculations (internal and/or external ! (i.e. using Code_Aster)). ! nalimx = 1, in case of explicit FSI algorithm. if (.false.) then nalimx = 15 endif ! Relative precision of sub-cycling Fluid Structure Coupling algorithm. if (.false.) then epalim = 1.d-5 endif ! Mesh viscosity modeling (cf. usvima) ! 0: isotropic ! 1: orthotropic if (.false.) then iortvm = 0 endif !---- ! Formats !---- return end subroutine usipsu !=============================================================================== subroutine usipes & !================ ( nmodpp ) !=============================================================================== ! Purpose: ! -------- ! User subroutine for the input of additional user parameters for ! input/output. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! name !type!mode ! role ! !__________________!____!_____!________________________________________________! ! nmodpp ! i ! <-- ! number of active specific physics models ! !__________________!____!_____!________________________________________________! ! 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 cstnum use dimens use numvar use optcal use cstphy use entsor use field use parall use period use ihmpre use ppppar use ppthch use ppincl use cs_c_bindings !=============================================================================== implicit none ! Arguments integer nmodpp ! Local variables integer ii, ipp, f_id, n_moments, imom !=============================================================================== ! This subroutine allows setting parameters ! which do not already appear in the other subroutines of this file. ! It is possible to add or remove parameters. ! The number of physical properties and variables is known here. !=============================================================================== !=============================================================================== ! 1. Logging !=============================================================================== ! Frequency of log output if (.true.) then ntlist = 1 endif ! Log (listing) verbosity if (.true.) then do ii = 1, nvar iwarni(ii) = 1 enddo iwarni(ipr) = 2 iwarni(iu) = 2 iwarni(iv) = 2 iwarni(iw) = 2 iwarni(isca(1)) = 2 endif !=============================================================================== ! 2. Definition of probes !=============================================================================== ! --- probes output step if (.true.) then nthist = 1 frhist = -1.d0 endif ! --- Number of monitoring points (probes) and their positions ! (limited to ncaptm=100) tplflw=100 if (.true.) then ncapt = 100 tplfmt = 1 ! time plot format (1: .dat, 2: .csv, 3: both) !levl=-0.471 xyzcap(1,1) =0d0 xyzcap(2,1) =0.002012d0 xyzcap(3,1) =-0.471d0 xyzcap(1,2) =0.015991972d0 xyzcap(2,2) =0.0040091782d0 xyzcap(3,2) =-0.471d0 xyzcap(1,3) =0.0252772519d0 xyzcap(2,3) =0.0061759222d0 xyzcap(3,3) =-0.471d0 xyzcap(1,4) =0.0428647438d0 xyzcap(2,4) =0.0093725678d0 xyzcap(3,4) =-0.471d0 xyzcap(1,5) =0d0 xyzcap(2,5) =0.060412d0 xyzcap(3,5) =-0.471d0 xyzcap(1,6) =0.025d0 xyzcap(2,6) =0.016d0 xyzcap(3,6) =-0.471d0 xyzcap(1,7) =0.03d0 xyzcap(2,7) =0.03d0 xyzcap(3,7) =-0.471d0 xyzcap(1,8) =0.025d0 xyzcap(2,8) =0.042848d0 xyzcap(3,8) =-0.471d0 xyzcap(1,9) =-0.015991972d0 xyzcap(2,9) =0.0040091782d0 xyzcap(3,9) =-0.471d0 xyzcap(1,10) =-0.0252772519d0 xyzcap(2,10) =0.0061759222d0 xyzcap(3,10) =-0.471d0 xyzcap(1,11) =-0.0428647438d0 xyzcap(2,11) =0.0093725678d0 xyzcap(3,11) =-0.471d0 xyzcap(1,12) =-0.025d0 xyzcap(2,12) =0.016d0 xyzcap(3,12) =-0.471d0 xyzcap(1,13) =-0.03d0 xyzcap(2,13) =0.03d0 xyzcap(3,13) =-0.471d0 xyzcap(1,14) =-0.025d0 xyzcap(2,14) =0.042848d0 xyzcap(3,14) =-0.471d0 !levl=-0.628 xyzcap(1,15) =0d0 xyzcap(2,15) =0.002012d0 xyzcap(3,15) =-0.628d0 xyzcap(1,16) =0.015991972d0 xyzcap(2,16) =0.0040091782d0 xyzcap(3,16) =-0.628d0 xyzcap(1,17) =0.0252772519d0 xyzcap(2,17) =0.0061759222d0 xyzcap(3,17) =-0.628d0 xyzcap(1,18) =0.0428647438d0 xyzcap(2,18) =0.0093725678d0 xyzcap(3,18) =-0.628d0 xyzcap(1,19) =0d0 xyzcap(2,19) =0.060412d0 xyzcap(3,19) =-0.628d0 xyzcap(1,20) =0.025d0 xyzcap(2,20) =0.016d0 xyzcap(3,20) =-0.628d0 xyzcap(1,21) =0.03d0 xyzcap(2,21) =0.03d0 xyzcap(3,21) =-0.628d0 xyzcap(1,22) =0.025d0 xyzcap(2,22) =0.042848d0 xyzcap(3,22) =-0.628d0 xyzcap(1,23) =-0.015991972d0 xyzcap(2,23) =0.0040091782d0 xyzcap(3,23) =-0.628d0 xyzcap(1,24) =-0.0252772519d0 xyzcap(2,24) =0.0061759222d0 xyzcap(3,24) =-0.628d0 xyzcap(1,25) =-0.0428647438d0 xyzcap(2,25) =0.0093725678d0 xyzcap(3,25) =-0.628d0 xyzcap(1,26) =-0.025d0 xyzcap(2,26) =0.016d0 xyzcap(3,26) =-0.628d0 xyzcap(1,27) =-0.03d0 xyzcap(2,27) =0.03d0 xyzcap(3,27) =-0.628d0 xyzcap(1,28) =-0.025d0 xyzcap(2,28) =0.042848d0 xyzcap(3,28) =-0.628d0 !levl=-0.785 xyzcap(1,29) =0d0 xyzcap(2,29) =0.002012d0 xyzcap(3,29) =-0.785d0 xyzcap(1,30) =0.015991972d0 xyzcap(2,30) =0.0040091782d0 xyzcap(3,30) =-0.785d0 xyzcap(1,31) =0.0252772519d0 xyzcap(2,31) =0.0061759222d0 xyzcap(3,31) =-0.785d0 xyzcap(1,32) =0.0428647438d0 xyzcap(2,32) =0.0093725678d0 xyzcap(3,32) =-0.785d0 xyzcap(1,33) =0d0 xyzcap(2,33) =0.060412d0 xyzcap(3,33) =-0.785d0 xyzcap(1,34) =0.025d0 xyzcap(2,34) =0.016d0 xyzcap(3,34) =-0.785d0 xyzcap(1,35) =0.03d0 xyzcap(2,35) =0.03d0 xyzcap(3,35) =-0.785d0 xyzcap(1,36) =0.025d0 xyzcap(2,36) =0.042848d0 xyzcap(3,36) =-0.785d0 xyzcap(1,37) =-0.015991972d0 xyzcap(2,37) =0.0040091782d0 xyzcap(3,37) =-0.785d0 xyzcap(1,38) =-0.0252772519d0 xyzcap(2,38) =0.0061759222d0 xyzcap(3,38) =-0.785d0 xyzcap(1,39) =-0.0428647438d0 xyzcap(2,39) =0.0093725678d0 xyzcap(3,39) =-0.785d0 xyzcap(1,40) =-0.025d0 xyzcap(2,40) =0.016d0 xyzcap(3,40) =-0.785d0 xyzcap(1,41) =-0.03d0 xyzcap(2,41) =0.03d0 xyzcap(3,41) =-0.785d0 xyzcap(1,42) =-0.025d0 xyzcap(2,42) =0.042848d0 xyzcap(3,42) =-0.785d0 !levl=-0.942 xyzcap(1,43) =0d0 xyzcap(2,43) =0.002012d0 xyzcap(3,43) =-0.942d0 xyzcap(1,44) =0.015991972d0 xyzcap(2,44) =0.0040091782d0 xyzcap(3,44) =-0.942d0 xyzcap(1,45) =0.0252772519d0 xyzcap(2,45) =0.0061759222d0 xyzcap(3,45) =-0.942d0 xyzcap(1,46) =0.0428647438d0 xyzcap(2,46) =0.0093725678d0 xyzcap(3,46) =-0.942d0 xyzcap(1,47) =0d0 xyzcap(2,47) =0.060412d0 xyzcap(3,47) =-0.942d0 xyzcap(1,48) =0.025d0 xyzcap(2,48) =0.016d0 xyzcap(3,48) =-0.942d0 xyzcap(1,49) =0.03d0 xyzcap(2,49) =0.03d0 xyzcap(3,49) =-0.942d0 xyzcap(1,50) =0.025d0 xyzcap(2,50) =0.042848d0 xyzcap(3,50) =-0.942d0 xyzcap(1,51) =-0.015991972d0 xyzcap(2,51) =0.0040091782d0 xyzcap(3,51) =-0.942d0 xyzcap(1,52) =-0.0252772519d0 xyzcap(2,52) =0.0061759222d0 xyzcap(3,52) =-0.942d0 xyzcap(1,53) =-0.0428647438d0 xyzcap(2,53) =0.0093725678d0 xyzcap(3,53) =-0.942d0 xyzcap(1,54) =-0.025d0 xyzcap(2,54) =0.016d0 xyzcap(3,54) =-0.942d0 xyzcap(1,55) =-0.03d0 xyzcap(2,55) =0.03d0 xyzcap(3,55) =-0.942d0 xyzcap(1,56) =-0.025d0 xyzcap(2,56) =0.042848d0 xyzcap(3,56) =-0.942d0 !levl=-1.099 xyzcap(1,57) =0d0 xyzcap(2,57) =0.002012d0 xyzcap(3,57) =-1.099d0 xyzcap(1,58) =0.015991972d0 xyzcap(2,58) =0.0040091782d0 xyzcap(3,58) =-1.099d0 xyzcap(1,59) =0.0252772519d0 xyzcap(2,59) =0.0061759222d0 xyzcap(3,59) =-1.099d0 xyzcap(1,60) =0.0428647438d0 xyzcap(2,60) =0.0093725678d0 xyzcap(3,60) =-1.099d0 xyzcap(1,61) =0d0 xyzcap(2,61) =0.060412d0 xyzcap(3,61) =-1.099d0 xyzcap(1,62) =0.025d0 xyzcap(2,62) =0.016d0 xyzcap(3,62) =-1.099d0 xyzcap(1,63) =0.03d0 xyzcap(2,63) =0.03d0 xyzcap(3,63) =-1.099d0 xyzcap(1,64) =0.025d0 xyzcap(2,64) =0.042848d0 xyzcap(3,64) =-1.099d0 xyzcap(1,65) =-0.015991972d0 xyzcap(2,65) =0.0040091782d0 xyzcap(3,65) =-1.099d0 xyzcap(1,66) =-0.0252772519d0 xyzcap(2,66) =0.0061759222d0 xyzcap(3,66) =-1.099d0 xyzcap(1,67) =-0.0428647438d0 xyzcap(2,67) =0.0093725678d0 xyzcap(3,67) =-1.099d0 xyzcap(1,68) =-0.025d0 xyzcap(2,68) =0.016d0 xyzcap(3,68) =-1.099d0 xyzcap(1,69) =-0.03d0 xyzcap(2,69) =0.03d0 xyzcap(3,69) =-1.099d0 xyzcap(1,70) =-0.025d0 xyzcap(2,70) =0.042848d0 xyzcap(3,70) =-1.099d0 xyzcap(1,71) =0d0 xyzcap(2,71) =0.002012d0 xyzcap(3,71) =-0.35325d0 xyzcap(1,72) =0d0 xyzcap(2,72) =0.002012d0 xyzcap(3,72) =-0.3925d0 xyzcap(1,73) =0d0 xyzcap(2,73) =0.002012d0 xyzcap(3,73) =-0.43175d0 xyzcap(1,74) =0d0 xyzcap(2,74) =0.002012d0 xyzcap(3,74) =-0.51025d0 xyzcap(1,75) =0d0 xyzcap(2,75) =0.002012d0 xyzcap(3,75) =-0.5495d0 xyzcap(1,76) =0d0 xyzcap(2,76) =0.002012d0 xyzcap(3,76) =-0.58875d0 xyzcap(1,77) =0d0 xyzcap(2,77) =0.002012d0 xyzcap(3,77) =-0.66725d0 xyzcap(1,78) =0d0 xyzcap(2,78) =0.002012d0 xyzcap(3,78) =-0.7065d0 xyzcap(1,79) =0d0 xyzcap(2,79) =0.002012d0 xyzcap(3,79) =-0.74575d0 xyzcap(1,80) =0d0 xyzcap(2,80) =0.002012d0 xyzcap(3,80) =-0.82425d0 xyzcap(1,81) =0d0 xyzcap(2,81) =0.002012d0 xyzcap(3,81) =-0.8635d0 xyzcap(1,82) =0d0 xyzcap(2,82) =0.002012d0 xyzcap(3,82) =-0.90275d0 xyzcap(1,83) =0d0 xyzcap(2,83) =0.002012d0 xyzcap(3,83) =-0.98125d0 xyzcap(1,84) =0d0 xyzcap(2,84) =0.002012d0 xyzcap(3,84) =-1.0205d0 xyzcap(1,85) =0d0 xyzcap(2,85) =0.002012d0 xyzcap(3,85) =-1.05975d0 xyzcap(1,86) =0d0 xyzcap(2,86) =0.060412d0 xyzcap(3,86) =-0.35325d0 xyzcap(1,87) =0d0 xyzcap(2,87) =0.060412d0 xyzcap(3,87) =-0.3925d0 xyzcap(1,88) =0d0 xyzcap(2,88) =0.060412d0 xyzcap(3,88) =-0.43175d0 xyzcap(1,89) =0d0 xyzcap(2,89) =0.060412d0 xyzcap(3,89) =-0.51025d0 xyzcap(1,90) =0d0 xyzcap(2,90) =0.060412d0 xyzcap(3,90) =-0.5495d0 xyzcap(1,91) =0d0 xyzcap(2,91) =0.060412d0 xyzcap(3,91) =-0.58875d0 xyzcap(1,92) =0d0 xyzcap(2,92) =0.060412d0 xyzcap(3,92) =-0.66725d0 xyzcap(1,93) =0d0 xyzcap(2,93) =0.060412d0 xyzcap(3,93) =-0.7065d0 xyzcap(1,94) =0d0 xyzcap(2,94) =0.060412d0 xyzcap(3,94) =-0.74575d0 xyzcap(1,95) =0d0 xyzcap(2,95) =0.060412d0 xyzcap(3,95) =-0.82425d0 xyzcap(1,96) =0d0 xyzcap(2,96) =0.060412d0 xyzcap(3,96) =-0.8635d0 xyzcap(1,97) =0d0 xyzcap(2,97) =0.060412d0 xyzcap(3,97) =-0.90275d0 xyzcap(1,98) =0d0 xyzcap(2,98) =0.060412d0 xyzcap(3,98) =-0.98125d0 xyzcap(1,99) =0d0 xyzcap(2,99) =0.060412d0 xyzcap(3,99) =-1.0205d0 xyzcap(1,100) =0d0 xyzcap(2,100) =0.060412d0 xyzcap(3,100) =-1.05975d0 endif !=============================================================================== ! 3. Fine control of variables output !=============================================================================== ! Per variable output control. ! More examples are provided in cs_user_parameters-output.f90 if (.true.) then ! Current dynamic variables ! pressure variable f_id = ivarfl(ipr) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 ! velocity vector f_id = ivarfl(iu) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 ihisvr(ipp+1,1) = -1 ihisvr(ipp+2,1) = -1 endif ! User scalar variables. if (.true.) then if (isca(1).gt.0.and.nscaus.ge.1) then f_id = ivarfl(isca(1)) call field_set_key_str(f_id, keylbl, 'Enthalpy') call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ipp = field_post_id(f_id) ihisvr(ipp,1)= -1 endif if (isca(2).gt.0.and.nscaus.ge.2) then f_id = ivarfl(isca(2)) call field_set_key_str(f_id, keylbl, 'Scalar 2') call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ipp = field_post_id(f_id) ihisvr(ipp,1)= -1 endif endif ! Other variables if (.true.) then ! Density variable (output for post-processing only if variable or ! in the case of specific physics) f_id = iprpfl(irom) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, max(irovar,nmodpp)) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 ! specific heat if (icp .gt. 0) then f_id = iprpfl(icp) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 0) ihisvr(ipp,1) = 0 endif ! laminar viscosity f_id = iprpfl(iviscl) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 0) call field_set_key_int(f_id, keylog, 0) ihisvr(ipp,1) = 0 ! turbulent viscosity f_id = iprpfl(ivisct) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 ! Courant number f_id = iprpfl(icour) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 0) ihisvr(ipp,1) = 0 ! Fourier number f_id = iprpfl(ifour) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 0) ihisvr(ipp,1) = 0 ! 'csmago' variable for dynamic L.E.S. models ! (square of the Samgorinsky "constant") if (ismago.gt.0) then f_id = iprpfl(ismago) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 0) ihisvr(ipp,1) = -1 endif ! total pressure (not defined in compressible case) if (ippmod(icompf).lt.0) then f_id = iprpfl(iprtot) ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 endif ! local time step f_id = ippdt ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 ! characteristic time of transient velocity/pressure coupling f_id = ipptx ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 f_id = ippty ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 f_id = ipptz ipp = field_post_id(f_id) call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 n_moments = cs_time_moment_n_moments() if (n_moments.gt.0) then do imom=1,n_moments f_id=time_moment_field_id(imom) ipp = field_post_id(f_id) if (ntcabs.le.6000)then call field_set_key_int(f_id, keyvis, 0) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = 0 else call field_set_key_int(f_id, keyvis, 1) call field_set_key_int(f_id, keylog, 1) ihisvr(ipp,1) = -1 endif enddo endif endif return end subroutine usipes !=============================================================================== subroutine usati1 !================ !=============================================================================== ! Purpose: ! -------- ! Initialize non-standard calculation options for the atmospheric version. !------------------------------------------------------------------------------- ! 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 dimens use numvar use optcal use cstphy use entsor use cstnum use ppppar use atincl use atsoil use atchem use atimbr use siream !=============================================================================== implicit none !=============================================================================== !=============================================================================== ! 1. Example of calculation options to modify !=============================================================================== !!! Reading the meteo file imeteo = 1 !!! For radiative model or chemistry ! Time of the simulation ! syear --> starting year ! squant --> starting quantile ! shour --> starting hour (UTC) ! smin --> starting minute ! ssec --> starting second syear = 1994 squant = 1 shour = 1 smin = 0 ssec = 0.d0 ! Geographic position ! xlon --> longitude of the domain origin ! xlat --> latitude of the domain origin xlon = 0.d0 xlat = 45.d0 ! ----------------------------------------------------------------------------- ! Atmospheric imbrication on large scale meteo (atimbr module) ! ----------------------------------------------------------------------------- ! ! -------------------------------------------------------------- ! activation flag ! -------------------------------------------------------------- imbrication_flag = .false. imbrication_verbose = .false. ! ------------------------------------------------------------------------------ ! flags for activating the cressman interpolation for the boundary conditions ! ------------------------------------------------------------------------------ cressman_u = .true. cressman_v = .true. cressman_tke = .true. cressman_eps = .true. cressman_theta = .true. cressman_qw = .true. cressman_nc = .true. ! -------------------------------------------------------------- ! numerical parameters for the cressman interpolation formulas ! -------------------------------------------------------------- horizontal_influence_radius = 8500.d0 vertical_influence_radius = 100.d0 ! -------------------------------------------------------------- !!! Gaseous chemistry ! ichemistry: choice of chemistry resolution scheme !0 --> no atmospheric chemistry !1 --> quasi steady equilibrium NOx scheme with 4 species and 5 reactions !2 --> scheme with 20 species and 34 reactions !3 --> scheme CB05 with 52 species and 155 reactions !4 --> user defined schema ichemistry = 0 ! ificchemistry: choice to read (=1,2,3,4, according to the scheme) ! or not (0) a concentration profile file ! if ichemistry>0 ifilechemistry is automaticaly set to ichemistry ifilechemistry = 0 ! isepchemistry: splitted (=1) or semi-coupled (=2, pu-sun) ! resolution of chemistry isepchemistry = 1 ! iphotolysis: inclusion (=1) or not (=2) of photolysis reactions iphotolysis = 1 ! dtchemmax: maximal time step (s) for chemistry resolution dtchemmax = 10.0d0 !!! Aerosol chemistry ! iaerosol: flag to activate aerosol chemistry ! if iaerosol = 1, ichemistry is automatically set to 3 (scheme 3) iaerosol = 1 ! inogaseouschemistry: flag to prevent automatic resolution (=1) ! of gaseous chemistry (scheme 3) inogaseouschemistry = 0 ! ncycle_aer: number of iterations for time splitting ncycle_aer = 1 ! icoag_siream: flag to activate (=1) or not (=0) coagulation icoag_siream = 1 ! icond_siream: flag to activate (=1) or not (=0) condensation/evaporation icond_siream = 1 ! inucl_siream: flag to activate (=1) or not (=0) nucleation inucl_siream = 1 ! icut_siream: cutting bin between equilibrium (1 to icut_siream) ! and dynamic bins (icut_siream to nbin_aer) icut_siream = nbin_aer !---- ! End !---- return end subroutine usati1 !=============================================================================== ! Purpose: ! ------- ! !> 1. Additional Calculation Options !> a. Density Relaxation !> !> 2. Physical Constants !> a.Dynamic Diffusion Coefficient !> b.Constants of the chosen model (EBU, Libby-Williams, ...) ! !> This routine is called: !> ---------------------- !> !> - Eddy Break Up pre-mixed flame !> - Diffusion flame in the framework of ``3 points'' rapid complete chemistry !> - Libby-Williams pre-mixed flame !> - Lagrangian module coupled with pulverized coal: !> Eulerian combustion of pulverized coal and !> Lagrangian transport of coal particles !> - Pulverised coal combustion !> - Fuel (oil) combustion ! !=============================================================================== subroutine cs_user_combustion !=============================================================================== ! Module files !=============================================================================== use paramx use dimens use numvar use optcal use cstphy use entsor use cstnum use parall use ihmpre use period use ppppar use ppthch use coincl use cpincl use ppincl use ppcpfu use cs_coal_incl use cs_fuel_incl use radiat !=============================================================================== implicit none !=============================================================================== !=============================================================================== ! 1. Additional Calculation Options !=============================================================================== ! --> Density Relaxation ! RHO(n+1) = SRROM * RHO(n) + (1-SRROM) * RHO(n+1) srrom = 0.8d0 !=============================================================================== ! 2. Physical Constants !=============================================================================== ! diftl0: Dynamic Diffusion Coefficient (kg/(m s)) diftl0 = 4.25d-5 ! ----------------------------------------------------------------------------- ! 2.1 For 3 points combusution model ONLY ! ----------------------------------------------------------------------------- ! Reference temperature for fuel and oxydant (K) tinfue = 436.d0 tinoxy = 353.d0 ! ----------------------------------------------------------------------------- ! 2.2 For EBU-model ONLY ! ----------------------------------------------------------------------------- ! cebu: EBU-model constant cebu = 2.5d0 ! ----------------------------------------------------------------------------- ! 2.3 For Libby-Williams model ONLY ! ----------------------------------------------------------------------------- ! Reference velocity vref = 60.d0 ! Reference length scale lref = 0.1d0 ! Activation Temperature ta = 0.2d5 ! Cross-over Temperature (combustion of propane) tstar= 0.12d4 !---- ! End !---- return end subroutine cs_user_combustion !=============================================================================== !=============================================================================== ! Purpose : ! ------- ! User subroutines for input of calculation parameters, ! and to initialize variables used for radiative transfer module ! !------------------------------------------------------------------------------- subroutine cs_user_radiative_transfer_param !=============================================================================== ! Module files !=============================================================================== use paramx use dimens use numvar use entsor use optcal use cstphy use parall use period use ppppar use radiat !=============================================================================== implicit none !=============================================================================== ! 1. Parameters for the radiative transfer module !=============================================================================== ! Indicator: indicates whether the radiation variables should be ! initialized (=0) or read from a restart file (=1) ! Useful if and only if the radiation module is activated (in this case, a ! restart file rayamo must be available) if (.false.) then isuird = isuite endif ! Period of the radiation module. if (.false.) then nfreqr = 1 endif !--> Quadrature Sn (n(n+2) directions) ! ! 1: S4 (24 directions) ! 2: S6 (48 directions) ! 3: S8 (80 directions) ! !--> Quadrature Tn (8n^2 directions) ! ! 4: T2 (32 directions) ! 5: T4 (128 directions) ! 6: Tn (8*ndirec^2 directions) if (.false.) then i_quadrature = 4 ndirec = 3 endif ! Indicates the method used to calculate the radiative source term: ! - 0: semi-analytic calculation (compulsory with transparent media) ! - 1: conservative calculation ! - 2: semi-analytic calculation corrected in order to be globally conservative ! Useful if and only if the radiation module is activated ! Note: If the medium is transparent, the choice has no effect on the calculation if (.false.) then idiver = 2 endif ! Verbosity level in the listing concerning the calculation of ! the wall temperatures (0, 1 or 2) if (.false.) then iimpar = 1 endif ! Verbosity mode for the Luminance (0, 1 or 2) if (.false.) then iimlum = 0 endif ! Compute the absorption coefficient through Modak (if 1), or do not use ! Modak (if 0) ! Useful ONLY when gas or coal combustion is activated if (.false.) then imodak = 0 endif !=============================================================================== return end subroutine cs_user_radiative_transfer_param !=============================================================================== subroutine uscfx1 !================ !=============================================================================== ! Purpose: ! ------- ! User subroutine. ! Initialize non standard options for the compressible flow scheme such ! what kind of equation of state must be used. ! In addition to options set in the user subroutine 'uscfx2' (or in ! the GUI): this subroutine allows to set switches to indicate if the ! volumetric viscosity and the conductivity are constants, their ! values being given in the subroutine 'uscfx2'. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! nom !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 ihmpre use dimens use numvar use optcal use cstphy use entsor use cstnum use parall use period use ppppar use ppthch use ppincl use field !=============================================================================== implicit none ! Arguments ! Local variables integer :: ifcvsl !=============================================================================== !=============================================================================== !=============================================================================== ! 1. Scheme options !=============================================================================== if (iihmpr.eq.0) then ! Remove test to set values here when also using GUI. ! Equation of state choice ! --> ieos = 1: Perfect gas with constant Gamma ! --> ieos = 2: Perfect gas with variable Gamma (please fill-in the source file ! cfther.f90 in this case, otherwise it won't work!) ieos = 1 ! --> Molecular thermal conductivity ! constant : ifcvsl = -1 ! variable : ifcvsl = 0 ifcvsl = 0 call field_set_key_int(ivarfl(isca(itempk)), kivisl, ifcvsl) ! --> Volumetric molecular viscosity ! iviscv = 0 : uniform in space and constant in time ! = 1 : variable in space and time iviscv = 0 endif !---- ! End !---- return end subroutine uscfx1 !=============================================================================== subroutine uscfx2 !================ ! Purpose: ! ------- ! User subroutine. ! Set values for the reference volumic viscosity, the reference ! conductivity and the molar mass for compressible flow. ! Initialize non standard options for the compressible flow scheme such ! as the hydrostatic equilibrium. ! In addition to options set in the user subroutine 'uscfx1' (or in ! the GUI): this subroutine allows to set a switch to indicate if the ! molecular viscosity is constant, its values being given in the user ! subroutine 'usipsu'. !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! nom !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 ihmpre use dimens use numvar use optcal use cstphy use entsor use cstnum use ppppar use ppthch use ppincl !=============================================================================== implicit none ! Arguments ! Local variables !=============================================================================== !=============================================================================== ! 1. Physical properties !=============================================================================== if (iihmpr.eq.0) then ! Remove test to set values here when also using GUI. ! --> Molecular viscosity ! constant : ivivar = 0 ! variable : ivivar = 1 ivivar = 0 ! --> Reference molecular thermal conductivity ! visls0 = lambda0 (molecular thermal conductivity, W/(m K)) ! WARNING: visls0 must be strictly positive ! (set a realistic value here even if conductivity is variable) visls0(itempk) = 3.d-2 ! If the molecular thermal conductivity is variable, its values ! must be provided in the user subroutine 'usphyv' ! --> Volumetric molecular viscosity ! Reference volumetric molecular viscosity ! viscv0 = kappa0 (volumetric molecular viscosity, kg/(m s)) viscv0 = 0.d0 ! If the volumetric molecular viscosity is variable, its values ! must be provided in the user subroutine 'usphyv' ! --> Molar mass of the gas (kg/mol) ! For example with dry air, xmasml is around 28.8d-3 kg/mol if (ieos.eq.1) then xmasmr = 0.028966 endif ! --> Hydrostatic equilibrium ! Specify if the hydrostatic equilibrium must be accounted for ! (yes = 1 , no = 0) icfgrp = 1 endif !---- ! End !---- return end subroutine uscfx2 !=============================================================================== subroutine useli1 & !================ ( iihmpu ) !=============================================================================== ! Purpose : ! ------- ! User subroutines for input of calculation parameters, ! and to initialize variables used for specific electric models, ! !------------------------------------------------------------------------------- ! Arguments !__________________.____._____.________________________________________________. ! name !type!mode ! role ! !__________________!____!_____!________________________________________________! ! iihmpu ! i ! <-- ! indicates if the XML file from the GUI is ! ! ! ! ! used (1: yes, 0: no) ! !__________________!____!_____!________________________________________________! ! 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 dimens use numvar use optcal use cstphy use entsor use cstnum use ppppar use ppthch use ppincl use elincl use mesh !=============================================================================== implicit none ! Arguments integer iihmpu ! Local variables !=============================================================================== !=============================================================================== ! 1. Calculation options !=============================================================================== ! --> Relaxation coefficient for mass density ! RHO(n+1) = SRROM * RHO(n) + (1-SRROM) * RHO(n+1) if (.false.) then srrom = 0.d0 endif ! --> "Electric variables" scaling (Joule effect or electric arc version) ! IELCOR = 0 : NO Correction ! IELCOR = 1 : CORRECTION if (.false.) then ielcor = 0 endif ! Imposed current intensity (electric arc) in Amp ! and Imposed Power (Joule effect for glass melting applications) in Watt ! These values have to be positive ! if (.false.) then couimp = 0.d0 puisim = 0.d0 endif ! Initial Potential Difference (positive value) if (.false.) then dpot = 0.d0 endif ! ---> Model for scaling intensity (electric arcs) ! MODREC = 0 : user defined ! MODREC = 1 : standard model ! MODREC = 2 : resetting plane model for electromagnetic quantities if (.false.) then modrec = 1 endif ! ---> Define current density component used to calculate current when MODREC = 2 ! IDRECA (1, 2 or 3) for component (x, y or z) if (.false.) then idreca = 3 ! Example : plane z = 3 with epsilon 0.0002 crit_reca(1) = 0. crit_reca(2) = 0. crit_reca(3) = 1. crit_reca(4) = -3. crit_reca(5) = 0.0002 endif !---- ! End !---- return end subroutine useli1 !=============================================================================== subroutine uscti1 !================ !=============================================================================== ! Purpose: ! ------- ! Definition of cooling tower model and exchange zones !------------------------------------------------------------------------------- ! 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 dimens use numvar use optcal use cstphy use entsor use cstnum use parall use period use ppppar use ppthch use ppincl use ctincl !=============================================================================== implicit none !=============================================================================== !=============================================================================== !=============================================================================== ! 1. Parameters for prescibed temperature difference !=============================================================================== ! Activation iaeeri = 0 ! Temperature difference (cooling) to prescribe vaeeri = 13.d0 ! Temperature modification frequency iaeerp = 5 ! Temperature step to compute difference slope tref(teau) paseri = 0.015d0 ! Maximum average hot water temperature aetemx = 80.d0 ! Minimum average cooled water temperature aetemn = 10.d0 ! Number of excange zones with a water inlet boundary nbzsup = 2 ! List of the nbzsup exchange zones at water inlet boundary lizsup(1) = 1 lizsup(2) = 2 ! Number of excange zones with a water outlet boundary nbzinf = 2 ! List of the nbzinf exchange zones at water outlet boundary lizinf(1) = 1 lizinf(2) = 2 ! Prescribed difference activation start time inbaei = 1000.d0 !=============================================================================== ! 2. Post-processing of exchange zones !=============================================================================== ichrze = 1 !=============================================================================== ! 3. Cooling tower restart !=============================================================================== isuict = isuite !---- ! End !---- return end subroutine uscti1 !=============================================================================== subroutine user_darcy_ini1 !======================== !=============================================================================== ! Purpose: ! -------- ! User routine for definition of computation parameters dealing with darcy module !------------------------------------------------------------------------------- ! 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 ihmpre, only: iihmpr use entsor use darcy_module !=============================================================================== implicit none !=============================================================================== if (.false.) then darcy_anisotropic_permeability = 0 ! permeability : 0 isotrop, 1 anisotrop endif if (.false.) then darcy_anisotropic_diffusion = 0 ! diffusion : 0 isotrop, 1 anisotrop endif if (.false.) then darcy_unsteady = 0 ! 0 steady flow, 1 unsteady flow endif if (.false.) then darcy_convergence_criterion = 0 ! convergence criterion of Newton scheme : 0, over pressure, 1, over velocity endif if (.false.) then darcy_gravity = 0 ! gravity is taken into account : 0 no, 1 yes endif ! if gravity is taken into account define gravity vector if (.false.) then darcy_gravity_x = 0. darcy_gravity_y = 0. darcy_gravity_z = 1. endif !---- ! End !---- return end subroutine user_darcy_ini1 !===============================================================================