SUBROUTINE callradite(icount,ngrid,nlayer,nq,zday,ls,pq,albedo, $ emis,mu0,pplev,pplay,pt,tsurf,fract,dist_sol,igout, $ dtlw,dtsw,fluxsurf_lw,fluxsurf_sw,fluxtop_lw,fluxtop_sw, & tauref,tau,aerosol,ccn,rdust,rice,nuice) IMPLICIT NONE c======================================================================= c subject: c -------- c Subroutine designed to call the main canonic c radiative transfer subroutine "lwmain" et "swmain" c to compute radiative heating and cooling rate and c radiative fluxes to the surface. c c These calculations are only valid on the part of the atmosphere c where Local Thermal Equilibrium (NLTE) is verified. In practice c The calculations are only performed for the first "nlaylte" c parameters (nlaylte is calculated by subroutine "nlthermeq" c and stored in common "yomlw.h"). c c The purpose of this subroutine is to: c 1) Make some initial calculation at first call c 2) Split the calculation in several sub-grid c ("sub-domain") to save memory and c be able run on a workstation at high resolution c The sub-grid size is defined in dimradmars.h c 3) Compute the 3D scattering parameters depending on the c size distribution of the different tracers (added by JBM) c 4) call "lwmain" and "swmain" c c c authors: c ------ c Francois Forget / Christophe Hourdin / J.-B. Madeleine (2009) c c c 3D scattering scheme user's guide (J.-B. Madeleine) c --------------------------------- c c This routine has been modified to take into account 3D, time c dependent scattering properties of the aerosols. c---- The look-up tables that contain the scattering parameters c of a given tracer, for different sizes, are read by SUAER.F90. c The names of the corresponding ASCII files have to be set in c this subroutine (file_id variable), and files must be in the c directory specified in datafile.h. Please make sure that the c ASCII files are correctly written, and that the range c of particle sizes is consistent with what you would expect. c---- SUAER.F90 is in charge of reading the ASCII files and averaging c the scattering parameters in each GCM channel, using the three last c equations of Forget et al. 1998 (GRL 25, No.7, p.1105-1108). c---- These look-up tables, loaded during the firstcall, are then c constantly used by the subroutine "aeroptproperties.F" to compute, c online, the 3D scattering parameters, based on the size distribution c (reffrad and nueffrad) of the different tracers, in each grid box. c These 3D size distributions are loaded by the "updatereffrad.F" c subroutine. A log-normal distribution is then assumed in c "aeroptproperties.F", along with a Gauss-Legendre integration. c---- The optical depth at the visible reference wavelength (set in c SUAER.F90, after the file_id variable) is then computed by c the subroutine "aeropacity.F", by using the size and spatial c distribution of the corresponding tracer. This connection has to c be implemented in "aeropacity.F" when adding a new tracer. To do so, c one can use equation 2 of Forget et al. 1998 (Icarus 131, p.302-316). c---- The resulting variables "aerosol", "QVISsQREF3d", "omegaVIS3d" and c "gVIS3d" (same in the infrared) are finally used by lwmain.F and c swmain.F to solve the radiative transfer equation. c c changes: c ------- c c > SRL 7/2000 c c This version has been modified to only calculate radiative tendencies c over layers 1..NFLEV (set in dimradmars.h). Returns zero for higher c layers, if any. c In other routines, nlayermx -> nflev. c Routines affected: lwflux, lwi, lwmain, lwxb, lwxd, lwxn. c c > J.-B. Madeleine 10W12 c This version uses the variable's splitting, which can be usefull c when performing very high resolution simulation like LES. c c ---------- c Here, solar band#1 is spectral interval between "long1vis" and "long2vis" c set in dimradmars.h c Here, solar band#2 is spectral interval between "long2vis" and "long3vis" c set in dimradmars.h c c input: c ----- c icount counter of call to subroutine physic by gcm c ngrid number of gridpoint of horizontal grid c nlayer Number of layer c nq Number of tracer c ls Solar longitude (Ls) , radian c zday Date (time since Ls=0, in martian days) c pq(ngrid,nlayer,nq) Advected fields c c albedo (ngrid,2) hemispheric surface albedo c albedo (i,1) : mean albedo for solar band#1 c (see below) c albedo (i,2) : mean albedo for solar band#2 c (see below) c emis Thermal IR surface emissivity (no unit) c mu0(ngridmx) cos of solar zenith angle c (=1 when sun at zenith) c pplay(ngrid,nlayer) pressure (Pa) in the middle of each layer c pplev(ngrid,nlayer+1) pressure (Pa) at boundaries of each layer c pt(ngrid,nlayer) atmospheric temperature in each layer (K) c tsurf(ngrid) surface temperature (K) c fract(ngridmx) day fraction of the time interval c =1 during the full day ; =0 during the night c declin latitude of subsolar point c dist_sol sun-Mars distance (AU) c igout coordinate of analysed point for debugging c reffrad(ngrid,nlayer,naerkind) Aerosol effective radius c nueffrad(ngrid,nlayer,naerkind) Aerosol effective variance c c output: c ------- c dtlw (ngrid,nlayer) longwave (IR) heating rate (K/s) c dtsw(ngrid,nlayer) shortwave (Solar) heating rate (K/s) c fluxsurf_lw(ngrid) surface downward flux tota LW (thermal IR) (W.m-2) c fluxsurf_sw(ngrid,1) surface downward flux SW for solar band#1 (W.m-2) c fluxsurf_sw(ngrid,2) surface downward flux SW for solar band#2 (W.m-2) c c fluxtop_lw(ngrid) outgoing upward flux tota LW (thermal IR) (W.m-2) c fluxtop_sw(ngrid,1) outgoing upward flux SW for solar band#1 (W.m-2) c fluxtop_sw(ngrid,2) outgoing upward flux SW for solar band#2 (W.m-2) c tauref Prescribed mean column optical depth at 700 Pa c tau Column total visible dust optical depth at each point c aerosol(ngrid,nlayer,naerkind) aerosol extinction optical depth c at reference wavelength "longrefvis" set c in dimradmars.h , in each layer, for one of c the "naerkind" kind of aerosol optical c properties. c======================================================================= c c Declarations : c ------------- c #include "dimensions.h" #include "dimphys.h" #include "dimradmars.h" #include "comcstfi.h" #include "callkeys.h" #include "yomlw.h" #include "aerkind.h" c----------------------------------------------------------------------- c Input/Output c ------------ INTEGER icount INTEGER ngrid,nlayer,nq INTEGER igout REAL pq(ngrid,nlayer,nq) REAL ccn(ngridmx,nlayermx) ! Cloud condensation nuclei ! (particules kg-1) REAL albedo(ngrid,2),emis(ngrid) REAL ls,zday REAL pplev(ngrid,nlayer+1),pplay(ngrid,nlayer) REAL pt(ngrid,nlayer) REAL tsurf(ngrid) REAL dist_sol,mu0(ngrid),fract(ngrid) REAL dtlw(ngridmx,nlayermx),dtsw(ngridmx,nlayermx) REAL fluxsurf_lw(ngridmx), fluxtop_lw(ngridmx) REAL fluxsurf_sw(ngridmx,2), fluxtop_sw(ngridmx,2) REAL tauref(ngrid), tau(ngrid,naerkind) REAL aerosol(ngrid,nlayer,naerkind) REAL rdust(ngridmx,nlayermx) ! Dust geometric mean radius (m) REAL rice(ngridmx,nlayermx) ! Ice geometric mean radius (m) REAL nuice(ngridmx,nlayermx) ! Estimated effective variance c c Local variables : c ----------------- INTEGER j,l,ig,n,ich INTEGER aer_count,iaer INTEGER jd,ig0,nd real cste_mars ! solar constant on Mars (Wm-2) REAL ptlev(ngridmx,nlayermx+1) INTEGER ndomain parameter (ndomain = (ngridmx-1) / ndomainsz + 1) c Thermal IR net radiative budget (W m-2) real znetrad(ndomainsz,nflev) real zfluxd_sw(ndomainsz,nflev+1,2) real zfluxu_sw(ndomainsz,nflev+1,2) REAL zplev(ndomainsz,nflev+1) REAL zztlev(ndomainsz,nflev+1) REAL zplay(ndomainsz,nflev) REAL zt(ndomainsz,nflev) REAL zaerosol(ndomainsz,nflev,naerkind) REAL zalbedo(ndomainsz,2) REAL zdp(ndomainsz,nflev) REAL zdt0(ndomainsz) REAL zzdtlw(ndomainsz,nflev) REAL zzdtsw(ndomainsz,nflev) REAL zzflux(ndomainsz,6) real zrmuz REAL :: zQVISsQREF3d(ndomainsz,nflev,nsun,naerkind) REAL :: zomegaVIS3d(ndomainsz,nflev,nsun,naerkind) REAL :: zgVIS3d(ndomainsz,nflev,nsun,naerkind) REAL :: zQIRsQREF3d(ndomainsz,nflev,nir,naerkind) REAL :: zomegaIR3d(ndomainsz,nflev,nir,naerkind) REAL :: zgIR3d(ndomainsz,nflev,nir,naerkind) c Aerosol size distribution REAL :: reffrad(ngrid,nlayer,naerkind) REAL :: nueffrad(ngrid,nlayer,naerkind) c Aerosol optical properties REAL :: QVISsQREF3d(ngridmx,nlayermx,nsun,naerkind) REAL :: omegaVIS3d(ngridmx,nlayermx,nsun,naerkind) REAL :: gVIS3d(ngridmx,nlayermx,nsun,naerkind) REAL :: QIRsQREF3d(ngridmx,nlayermx,nir,naerkind) REAL :: omegaIR3d(ngridmx,nlayermx,nir,naerkind) REAL :: gIR3d(ngridmx,nlayermx,nir,naerkind) REAL :: QREFvis3d(ngridmx,nlayermx,naerkind) REAL :: QREFir3d(ngridmx,nlayermx,naerkind) REAL :: omegaREFvis3d(ngridmx,nlayermx,naerkind) REAL :: omegaREFir3d(ngridmx,nlayermx,naerkind) c local saved variables c --------------------- real pview(ngridmx) save pview real zco2 ! volume fraction of CO2 in Mars atmosphere DATA zco2/0.95/ SAVE zco2 LOGICAL firstcall DATA firstcall/.true./ SAVE firstcall c---------------------------------------------------------------------- c Initialisation c -------------- IF (firstcall) THEN c Please name the different scatterers here ---------------- c PLEASE MAKE SURE that you set up the right number of c scatterers in dimradmars.h (naerkind); name_iaer(1) = "dust_conrath" !! default choice is good old Conrath profile IF (doubleq.AND.active) name_iaer(1) = "dust_doubleq" !! two-moment scheme IF (water.AND.activice) name_iaer(2) = "h2o_ice" !! radiatively-active clouds IF (submicron.AND.active) name_iaer(2) = "dust_submicron" !! JBM experimental stuff c ---------------------------------------------------------- c Assign a number to the different scatterers c ------------------------------------------- iaer_dust_conrath=0 iaer_dust_doubleq=0 iaer_dust_submicron=0 iaer_h2o_ice=0 aer_count=0 if (.NOT.active) then do iaer=1,naerkind if (name_iaer(iaer).eq."dust_conrath") then iaer_dust_conrath = iaer aer_count = aer_count + 1 endif enddo endif if (doubleq.AND.active) then do iaer=1,naerkind if (name_iaer(iaer).eq."dust_doubleq") then iaer_dust_doubleq = iaer aer_count = aer_count + 1 endif enddo endif if (submicron.AND.active) then do iaer=1,naerkind if (name_iaer(iaer).eq."dust_submicron") then iaer_dust_submicron = iaer aer_count = aer_count + 1 endif enddo endif if (water.AND.activice) then do iaer=1,naerkind if (name_iaer(iaer).eq."h2o_ice") then iaer_h2o_ice = iaer aer_count = aer_count + 1 endif enddo endif c Check that we identified all tracers: if (aer_count.ne.naerkind) then write(*,*) "callradite: found only ",aer_count," scatterers" write(*,*) " expected ",naerkind write(*,*) "please make sure that the number of" write(*,*) "scatterers in dimradmars.h, the names" write(*,*) "in callradite.F, and the flags in" write(*,*) "callphys.def are all consistent!" do iaer=1,naerkind write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) enddo stop else write(*,*) "callradite: found all scatterers, namely:" do iaer=1,naerkind write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) enddo endif c ------------------------------------------- DO ig=1,ngrid pview(ig)=1.66 ! cosecant of viewing angle ENDDO gcp = g/cpp c Logical tests for radiatively active water-ice clouds: IF ( (activice.AND.(.NOT.water)).OR. & (activice.AND.(naerkind.LT.2)) ) THEN WRITE(*,*) 'If activice is TRUE, water has to be set' WRITE(*,*) 'to TRUE, and "naerkind" must be at least' WRITE(*,*) 'equal to 2 in dimradmars.h.' CALL ABORT ELSE IF ( (.NOT.activice).AND.(naerkind.GT.1) ) THEN WRITE(*,*) 'naerkind is greater than unity, but' WRITE(*,*) 'activice has not been set to .true.' WRITE(*,*) 'in callphys.def; this is not logical!' CALL ABORT ENDIF c Loading the optical properties in external look-up tables: CALL SUAER CALL SULW write(*,*) 'Splitting radiative calculations: ', $ ' ngridmx,ngrid,ndomainsz,ndomain', $ ngridmx,ngrid,ndomainsz,ndomain if (ngridmx .EQ. 1) then if (ndomainsz .NE. 1) then print* print*,'ATTENTION !!!' print*,'pour tourner en 1D, ' print*,'fixer ndomainsz=1 dans phymars/dimradmars.h' print* call exit(1) endif endif firstcall=.false. END IF c Computing aerosol optical properties and opacity c ------------------------------------------------ c Updating aerosol size distributions: CALL updatereffrad(ngrid,nlayer, & rdust,rice,nuice, & reffrad,nueffrad, & pq) c Computing 3D scattering parameters: CALL aeroptproperties(ngrid,nlayer,reffrad,nueffrad, & QVISsQREF3d,omegaVIS3d,gVIS3d, & QIRsQREF3d,omegaIR3d,gIR3d, & QREFvis3d,QREFir3d, & omegaREFvis3d,omegaREFir3d) c Computing aerosol optical depth in each layer: CALL aeropacity(ngrid,nlayer,nq,zday,pplay,pplev,ls, & pq,ccn,tauref,tau,aerosol,reffrad,nueffrad, & QREFvis3d,QREFir3d,omegaREFvis3d,omegaREFir3d) c Starting loop on sub-domain c ---------------------------- DO jd=1,ndomain ig0=(jd-1)*ndomainsz if (jd.eq.ndomain) then nd=ngridmx-ig0 else nd=ndomainsz endif c Spliting input variable in sub-domain input variables c --------------------------------------------------- do l=1,nlaylte do ig = 1,nd do iaer = 1, naerkind do ich = 1, nsun zQVISsQREF3d(ig,l,ich,iaer) = & QVISsQREF3d(ig0+ig,l,ich,iaer) zomegaVIS3d(ig,l,ich,iaer) = & omegaVIS3d(ig0+ig,l,ich,iaer) zgVIS3d(ig,l,ich,iaer) = & gVIS3d(ig0+ig,l,ich,iaer) enddo do ich = 1, nir zQIRsQREF3d(ig,l,ich,iaer) = & QIRsQREF3d(ig0+ig,l,ich,iaer) zomegaIR3d(ig,l,ich,iaer) = & omegaIR3d(ig0+ig,l,ich,iaer) zgIR3d(ig,l,ich,iaer) = & gIR3d(ig0+ig,l,ich,iaer) enddo enddo enddo enddo do l=1,nlaylte+1 do ig = 1,nd zplev(ig,l) = pplev(ig0+ig,l) enddo enddo do l=1,nlaylte do ig = 1,nd zplay(ig,l) = pplay(ig0+ig,l) zt(ig,l) = pt(ig0+ig,l) c Thickness of each layer (Pa) : zdp(ig,l)= pplev(ig0+ig,l) - pplev(ig0+ig,l+1) enddo enddo do n=1,naerkind do l=1,nlaylte do ig=1,nd zaerosol(ig,l,n) = aerosol(ig0+ig,l,n) enddo enddo enddo do j=1,2 do ig = 1,nd zalbedo(ig,j) = albedo(ig0+ig,j) enddo enddo c Intermediate levels: (computing tlev) c --------------------------------------- c Extrapolation for the air temperature above the surface DO ig=1,nd zztlev(ig,1)=zt(ig,1)+ s (zplev(ig,1)-zplay(ig,1))* s (zt(ig,1)-zt(ig,2))/(zplay(ig,1)-zplay(ig,2)) zdt0(ig) = tsurf(ig0+ig) - zztlev(ig,1) ENDDO DO l=2,nlaylte DO ig=1, nd zztlev(ig,l)=0.5*(zt(ig,l-1)+zt(ig,l)) ENDDO ENDDO DO ig=1, nd zztlev(ig,nlaylte+1)=zt(ig,nlaylte) ENDDO c Longwave ("lw") radiative transfer (= thermal infrared) c ------------------------------------------------------- call lwmain (ig0,icount,nd,nflev . ,zdp,zdt0,emis(ig0+1),zplev,zztlev,zt . ,zaerosol,zzdtlw . ,fluxsurf_lw(ig0+1),fluxtop_lw(ig0+1) . ,znetrad & ,zQIRsQREF3d,zomegaIR3d,zgIR3d) c Shortwave ("sw") radiative transfer (= solar radiation) c ------------------------------------------------------- c Mars solar constant (W m-2) c 1370 W.m-2 is the solar constant at 1 AU. cste_mars=1370./(dist_sol*dist_sol) call swmain ( nd, nflev, S cste_mars, zalbedo, S mu0(ig0+1), zdp, zplev, zaerosol, fract(ig0+1), S zzdtsw, zfluxd_sw, zfluxu_sw, & zQVISsQREF3d,zomegaVIS3d,zgVIS3d) c ------------------------------------------------------------ c Un-spliting output variable from sub-domain input variables c ------------------------------------------------------------ do l=1,nlaylte do ig = 1,nd dtlw(ig0+ig,l) = zzdtlw(ig,l) dtsw(ig0+ig,l) = zzdtsw(ig,l) enddo enddo do l=1,nlaylte+1 do ig = 1,nd ptlev(ig0+ig,l) = zztlev(ig,l) enddo enddo do ig = 1,nd fluxsurf_sw(ig0+ig,1) = zfluxd_sw(ig,1,1) fluxsurf_sw(ig0+ig,2) = zfluxd_sw(ig,1,2) fluxtop_sw(ig0+ig,1) = zfluxu_sw(ig,nlaylte+1,1) fluxtop_sw(ig0+ig,2) = zfluxu_sw(ig,nlaylte+1,2) enddo ENDDO ! (boucle jd=1, ndomain) c Zero tendencies for any remaining layers between nlaylte and nlayer if (nlayer.gt.nlaylte) then do l = nlaylte+1, nlayer do ig = 1, ngrid dtlw(ig, l) = 0. dtsw(ig, l) = 0. enddo enddo endif c Output for debugging if lwrite=T c -------------------------------- c Write all nlayer layers, even though only nlaylte layers may have c non-zero tendencies. IF(lwrite) THEN PRINT*,'Diagnotique for the radiation' PRINT*,'albedo, emissiv, mu0,fract,fluxsurf_lw,fluxsurf_sw' PRINT*,albedo(igout,1),emis(igout),mu0(igout), s fract(igout), fluxsurf_lw(igout), $ fluxsurf_sw(igout,1)+fluxsurf_sw(igout,2) PRINT*,'Tlay Tlev Play Plev dT/dt SW dT/dt LW (K/s)' PRINT*,'daysec',daysec DO l=1,nlayer PRINT*,pt(igout,l),ptlev(igout,l), s pplay(igout,l),pplev(igout,l), s dtsw(igout,l),dtlw(igout,l) ENDDO ENDIF return end