C $Header: /u/gcmpack/MITgcm/pkg/thsice/thsice_solve4temp.F,v 1.37 2013/08/22 02:10:48 jmc Exp $ C $Name: $ #include "THSICE_OPTIONS.h" #ifdef ALLOW_AUTODIFF_TAMC # ifdef ALLOW_EXF # include "EXF_OPTIONS.h" # endif #endif CBOP C !ROUTINE: THSICE_SOLVE4TEMP C !INTERFACE: SUBROUTINE THSICE_SOLVE4TEMP( I bi, bj, I iMin,iMax, jMin,jMax, dBugFlag, I useBulkForce, useEXF, I icMask, hIce, hSnow1, tFrz, flxExSW, U flxSW, tSrf1, qIc1, qIc2, O tIc1, tIc2, dTsrf1, O sHeat, flxCnB, flxAtm, evpAtm, I myTime, myIter, myThid ) C !DESCRIPTION: \bv C *==========================================================* C | S/R THSICE_SOLVE4TEMP C *==========================================================* C | Solve (implicitly) for sea-ice and surface temperature C *==========================================================* C \ev C ADAPTED FROM: C LANL CICE.v2.0.2 C----------------------------------------------------------------------- C.. thermodynamics (vertical physics) based on M. Winton 3-layer model C.. See Bitz, C. M. and W. H. Lipscomb, 1999: An energy-conserving C.. thermodynamic sea ice model for climate study. C.. J. Geophys. Res., 104, 15669 - 15677. C.. Winton, M., 1999: "A reformulated three-layer sea ice model." C.. Submitted to J. Atmos. Ocean. Technol. C.. authors Elizabeth C. Hunke and William Lipscomb C.. Fluid Dynamics Group, Los Alamos National Laboratory C----------------------------------------------------------------------- Cc****subroutine thermo_winton(n,fice,fsnow,dqice,dTsfc) C.. Compute temperature change using Winton model with 2 ice layers, of C.. which only the top layer has a variable heat capacity. C !USES: IMPLICIT NONE C == Global variables === #include "EEPARAMS.h" #include "SIZE.h" #include "THSICE_PARAMS.h" #ifdef ALLOW_AUTODIFF_TAMC # include "tamc.h" # include "tamc_keys.h" #include "THSICE_SIZE.h" c#include "THSICE_VARS.h" # ifdef ALLOW_EXF # include "EXF_FIELDS.h" # include "EXF_PARAM.h" # include "EXF_CONSTANTS.h" # endif #endif C !INPUT/OUTPUT PARAMETERS: C == Routine Arguments == C bi,bj :: tile indices C iMin,iMax :: computation domain: 1rst index range C jMin,jMax :: computation domain: 2nd index range C dBugFlag :: allow to print debugging stuff (e.g. on 1 grid point). C useBulkForce:: use surf. fluxes from bulk-forcing external S/R C useEXF :: use surf. fluxes from exf external S/R C--- Input: C icMask :: sea-ice fractional mask [0-1] C hIce :: ice height [m] C hSnow1 :: snow height [m] C tFrz :: sea-water freezing temperature [oC] (function of S) C flxExSW :: surf. heat flux (+=down) except SW, function of surf. temp Ts: C 0: Flx(Ts=0) ; 1: Flx(Ts=Ts^n) ; 2: d.Flx/dTs(Ts=Ts^n) C--- Modified (input&output): C flxSW :: net Short-Wave flux (+=down) [W/m2]: input= at surface C :: output= below sea-ice, into the ocean C tSrf1 :: surface (ice or snow) temperature C qIc1 :: ice enthalpy (J/kg), 1rst level C qIc2 :: ice enthalpy (J/kg), 2nd level C--- Output C tIc1 :: temperature of ice layer 1 [oC] C tIc2 :: temperature of ice layer 2 [oC] C dTsrf1 :: surf. temp adjusment: Ts^n+1 - Ts^n C sHeat :: surf heating flux left to melt snow or ice (= Atmos-conduction) C flxCnB :: heat flux conducted through the ice to bottom surface C flxAtm :: net flux of energy from the atmosphere [W/m2] (+=down) C without snow precip. (energy=0 for liquid water at 0.oC) C evpAtm :: evaporation to the atmosphere [kg/m2/s] (>0 if evaporate) C--- Input: C myTime :: current Time of simulation [s] C myIter :: current Iteration number in simulation C myThid :: my Thread Id number INTEGER bi,bj INTEGER iMin, iMax INTEGER jMin, jMax LOGICAL dBugFlag LOGICAL useBulkForce LOGICAL useEXF _RL icMask(1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL hIce (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL hSnow1 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL tFrz (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxSW (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL tSrf1 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL qIc1 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL qIc2 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL tIc1 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL tIc2 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL sHeat (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxCnB (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxAtm (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL evpAtm (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxExSW(iMin:iMax,jMin:jMax,0:2) _RL dTsrf1 (iMin:iMax,jMin:jMax) _RL myTime INTEGER myIter INTEGER myThid CEOP #ifdef ALLOW_THSICE C !LOCAL VARIABLES: C == Local Variables == C useBlkFlx :: use some bulk-formulae to compute fluxes over sea-ice C :: (otherwise, fluxes are passed as argument from AIM) C iterate4Tsf :: to stop to iterate when all icy grid pts Tsf did converged C iceFlag :: True= do iterate for Surf.Temp ; False= do nothing C frsnow :: fractional snow cover C fswpen :: SW penetrating beneath surface (W m-2) C fswdn :: SW absorbed at surface (W m-2) C fswint :: SW absorbed in ice (W m-2) C fswocn :: SW passed through ice to ocean (W m-2) C Tsf :: surface (ice or snow) temperature (local copy of tSrf1) C flx0exSW :: net surface heat flux over melting snow/ice, except short-wave. C flxTexSW :: net surface heat flux, except short-wave (W/m2) C dFlxdT :: deriv of flxNet wrt Tsf (W m-2 deg-1) C evap00 :: evaporation over melting snow/ice [kg/m2/s] (>0 if evaporate) C renamed to evap00 because TAF confuses symbol with EXF evap0 C evapT :: evaporation over snow/ice [kg/m2/s] (>0 if evaporate) C dEvdT :: derivative of evap. with respect to Tsf [kg/m2/s/K] C flxNet :: net surf heat flux (+=down), from Atmos. to sea-ice (W m-2) C netSW :: net Short-Wave flux at surface (+=down) [W/m2] C fct :: heat conducted to top surface C k12, k32 :: thermal conductivity terms C a10,b10,c10 :: coefficients in quadratic eqn for T1 C a1, b1, c1 :: coefficients in quadratic eqn for T1 C dt :: timestep LOGICAL useBlkFlx LOGICAL iterate4Tsf INTEGER i, j, k, iterMax INTEGER ii, jj, icount, stdUnit CHARACTER*(MAX_LEN_MBUF) msgBuf _RL frsnow _RL fswpen _RL fswdn _RL fswint _RL fswocn _RL iceFlag (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL Tsf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flx0exSW(1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxTexSW(1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL dFlxdT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL evap00 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL evapT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL dEvdT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL flxNet _RL fct _RL k12 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL k32 _RL a10 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL b10 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL c10 (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL a1, b1, c1 _RL dt _RL recip_dhSnowLin #ifdef ALLOW_DBUG_THSICE _RL netSW #endif C- Define grid-point location where to print debugging values #include "THSICE_DEBUG.h" 1010 FORMAT(A,I3,3F11.6) 1020 FORMAT(A,1P4E14.6) C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-| #ifdef ALLOW_AUTODIFF_TAMC act1 = bi - myBxLo(myThid) max1 = myBxHi(myThid) - myBxLo(myThid) + 1 act2 = bj - myByLo(myThid) max2 = myByHi(myThid) - myByLo(myThid) + 1 act3 = myThid - 1 max3 = nTx*nTy act4 = ikey_dynamics - 1 ticekey = (act1 + 1) + act2*max1 & + act3*max1*max2 & + act4*max1*max2*max3 #endif /* ALLOW_AUTODIFF_TAMC */ #ifdef ALLOW_AUTODIFF_TAMC CADJ STORE flxsw(:,:) = comlev1_bibj,key=ticekey,byte=isbyte DO j = 1-OLy, sNy+OLy DO i = 1-OLx, sNx+OLx tIc1(i,j) = 0. _d 0 tIc2(i,j) = 0. _d 0 C- set these arrays everywhere: overlap are not set and not used, C but some arrays are stored and storage includes overlap. flx0exSW(i,j) = 0. _d 0 flxTexSW(i,j) = 0. _d 0 dFlxdT (i,j) = 0. _d 0 evap00 (i,j) = 0. _d 0 evapT (i,j) = 0. _d 0 dEvdT (i,j) = 0. _d 0 iceFlag (i,j) = 0. _d 0 Tsf (i,j) = 0. _d 0 ENDDO ENDDO #endif stdUnit = standardMessageUnit useBlkFlx = useEXF .OR. useBulkForce dt = thSIce_dtTemp IF ( dhSnowLin.GT.0. _d 0 ) THEN recip_dhSnowLin = 1. _d 0 / dhSnowLin ELSE recip_dhSnowLin = 0. _d 0 ENDIF iterate4Tsf = .FALSE. icount = 0 DO j = jMin, jMax DO i = iMin, iMax #ifdef ALLOW_AUTODIFF_TAMC ikey_1 = i & + sNx*(j-1) & + sNx*sNy*act1 & + sNx*sNy*max1*act2 & + sNx*sNy*max1*max2*act3 & + sNx*sNy*max1*max2*max3*act4 C-- CADJ STORE hSnow1(i,j) = comlev1_thsice_1, key=ikey_1 cCADJ STORE flxsw(i,j) = comlev1_thsice_1, key=ikey_1 cCADJ STORE qic1(i,j) = comlev1_thsice_1, key=ikey_1 cCADJ STORE qic2(i,j) = comlev1_thsice_1, key=ikey_1 #endif IF ( icMask(i,j).GT.0. _d 0) THEN iterate4Tsf = .TRUE. iceFlag(i,j) = 1. _d 0 #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,'(A,2I4,2I2)') & 'ThSI_SOLVE4T: i,j=',i,j,bi,bj #endif IF ( hIce(i,j).LT.hIceMin ) THEN C if hi < hIceMin, melt the ice. C keep the position of this problem but do the stop later ii = i jj = j icount = icount + 1 ENDIF C-- Fractional snow cover: C assume a linear distribution of snow thickness, with dhSnowLin slope, C from hs-dhSnowLin to hs+dhSnowLin if full ice & snow cover. C frsnow = fraction of snow over the ice-covered part of the grid cell IF ( hSnow1(i,j) .GT. icMask(i,j)*dhSnowLin ) THEN frsnow = 1. _d 0 ELSE frsnow = hSnow1(i,j)*recip_dhSnowLin/icMask(i,j) IF ( frsnow.GT.0. _d 0 ) frsnow = SQRT(frsnow) ENDIF C-- Compute SW flux absorbed at surface and penetrating to layer 1. fswpen = flxSW(i,j) * (1. _d 0 - frsnow) * i0swFrac fswocn = fswpen * exp(-ksolar*hIce(i,j)) fswint = fswpen - fswocn fswdn = flxSW(i,j) - fswpen C Initialise Atmospheric surf. heat flux with net SW flux at the surface flxAtm(i,j) = flxSW(i,j) C SW flux at sea-ice base left to the ocean flxSW(i,j) = fswocn C Initialise surface Heating with SW contribution sHeat(i,j) = fswdn C-- Compute conductivity terms at layer interfaces. k12(i,j) = 4. _d 0*kIce*kSnow & / (kSnow*hIce(i,j) + 4. _d 0*kIce*hSnow1(i,j)) k32 = 2. _d 0*kIce / hIce(i,j) C-- Compute ice temperatures a1 = cpIce b1 = qIc1(i,j) + (cpWater-cpIce )*Tmlt1 - Lfresh c1 = Lfresh * Tmlt1 tIc1(i,j) = 0.5 _d 0 *(-b1 - SQRT(b1*b1-4. _d 0*a1*c1))/a1 tIc2(i,j) = (Lfresh-qIc2(i,j)) / cpIce #ifdef ALLOW_DBUG_THSICE IF (tIc1(i,j).GT.0. _d 0 ) THEN WRITE(stdUnit,'(A,I12,1PE14.6)') & ' BBerr: Tice(1) > 0 ; it=', myIter, qIc1(i,j) WRITE(stdUnit,'(A,4I5,2F11.4)') & ' BBerr: i,j,bi,bj,Tice = ',i,j,bi,bj,tIc1(i,j),tIc2(i,j) ENDIF IF ( tIc2(i,j).GT.0. _d 0) THEN WRITE(stdUnit,'(A,I12,1PE14.6)') & ' BBerr: Tice(2) > 0 ; it=', myIter, qIc2(i,j) WRITE(stdUnit,'(A,4I5,2F11.4)') & ' BBerr: i,j,bi,bj,Tice = ',i,j,bi,bj,tIc1(i,j),tIc2(i,j) ENDIF IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1010) & 'ThSI_SOLVE4T: k, Ts, Tice=',0,tSrf1(i,j),tIc1(i,j),tIc2(i,j) #endif C-- Compute coefficients used in quadratic formula. a10(i,j) = rhoi*cpIce *hIce(i,j)/(2. _d 0*dt) + & k32*( 4. _d 0*dt*k32 + rhoi*cpIce *hIce(i,j) ) & / ( 6. _d 0*dt*k32 + rhoi*cpIce *hIce(i,j) ) b10(i,j) = -hIce(i,j)* & ( rhoi*cpIce*tIc1(i,j) + rhoi*Lfresh*Tmlt1/tIc1(i,j) ) & /(2. _d 0*dt) & - k32*( 4. _d 0*dt*k32*tFrz(i,j) & +rhoi*cpIce*hIce(i,j)*tIc2(i,j) ) & / ( 6. _d 0*dt*k32 + rhoi*cpIce *hIce(i,j) ) & - fswint c10(i,j) = rhoi*Lfresh*hIce(i,j)*Tmlt1 / (2. _d 0*dt) ELSE iceFlag(i,j) = 0. _d 0 ENDIF ENDDO ENDDO #ifndef ALLOW_AUTODIFF IF ( icount .gt. 0 ) THEN WRITE(stdUnit,'(A,I5,A)') & 'THSICE_SOLVE4TEMP: there are ',icount, & ' case(s) where hIce 0 C, fix Tsfc = 0 and recompute T1 C with different coefficients. DO j = jMin, jMax DO i = iMin, iMax IF ( iceFlag(i,j).GT.0. _d 0 ) THEN flxNet = sHeat(i,j) + flxTexSW(i,j) #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1020) & 'ThSI_SOLVE4T: flxNet,dFlxdT,k12,D=', & flxNet, dFlxdT(i,j), k12(i,j), k12(i,j)-dFlxdT(i,j) #endif a1 = a10(i,j) - k12(i,j)*dFlxdT(i,j) / (k12(i,j)-dFlxdT(i,j)) b1 = b10(i,j) - k12(i,j)*(flxNet-dFlxdT(i,j)*Tsf(i,j)) & /(k12(i,j)-dFlxdT(i,j)) c1 = c10(i,j) tIc1(i,j) = -(b1 + SQRT(b1*b1-4. _d 0*a1*c1))/(2. _d 0*a1) dTsrf1(i,j) = (flxNet + k12(i,j)*(tIc1(i,j)-Tsf(i,j))) & /(k12(i,j)-dFlxdT(i,j)) Tsf(i,j) = Tsf(i,j) + dTsrf1(i,j) C IF ( Tsf(i,j) .GT. 0. _d 0 ) THEN #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1010) & 'ThSI_SOLVE4T: k,ts,t1,dTs=',k,Tsf(i,j),tIc1(i,j),dTsrf1(i,j) #endif a1 = a10(i,j) + k12(i,j) C note: b1 = b10 - k12*Tf0 b1 = b10(i,j) tIc1(i,j) = (-b1 - SQRT(b1*b1-4. _d 0*a1*c1))/(2. _d 0*a1) Tsf(i,j) = 0. _d 0 #ifndef ALLOW_AUTODIFF IF ( useBlkFlx ) THEN #endif /* ALLOW_AUTODIFF */ flxTexSW(i,j) = flx0exSW(i,j) evapT(i,j) = evap00(i,j) dTsrf1(i,j) = 0. _d 0 #ifndef ALLOW_AUTODIFF ELSE flxTexSW(i,j) = flxExSW(i,j,0) dTsrf1(i,j) = 1000. dFlxdT(i,j) = 0. ENDIF #endif /* ALLOW_AUTODIFF */ ENDIF C-- Check for convergence. If no convergence, then repeat. IF (ABS(dTsrf1(i,j)).GE.Terrmax) THEN iceFlag(i,j) = 1. _d 0 ELSE iceFlag(i,j) = 0. _d 0 ENDIF iterate4Tsf = iterate4Tsf .OR. (iceFlag(i,j).GT.0. _d 0) C Convergence test: Make sure Tsfc has converged, within prescribed error. C (Energy conservation is guaranteed within machine roundoff, even C if Tsfc has not converged.) C If no convergence, then repeat. #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1010) & 'ThSI_SOLVE4T: k,ts,t1,dTs=', k,Tsf(i,j),tIc1(i,j),dTsrf1(i,j) IF ( useBlkFlx .AND. k.EQ.nitMaxTsf .AND. & (iceFlag(i,j).GT.0. _d 0) ) THEN WRITE(stdUnit,'(A,4I4,I12,F15.9)') & ' BB: not converge: i,j,it,hi=',i,j,bi,bj,myIter,hIce(i,j) WRITE(stdUnit,*) & 'BB: not converge: Tsf, dTsf=', Tsf(i,j), dTsrf1(i,j) WRITE(stdUnit,*) & 'BB: not converge: flxNet,dFlxT=', flxNet, dFlxdT(i,j) IF ( Tsf(i,j).LT.-70. _d 0 ) THEN WRITE( msgBuf, '(A,2I4,2I3,I10,F12.3)') & 'THSICE_SOLVE4TEMP: Too low Tsf in', i, j, bi, bj, & myIter, Tsf(i,j) CALL PRINT_ERROR( msgBuf , myThid ) STOP 'ABNORMAL END: S/R THSICE_SOLVE4TEMP' ENDIF ENDIF #endif /* ALLOW_DBUG_THSICE */ ENDIF ENDDO ENDDO #ifndef ALLOW_AUTODIFF C--- end if: IF ( iterate4Tsf ) THEN ENDIF #endif /* ALLOW_AUTODIFF */ C--- end loop DO k = 1,iterMax ENDDO C ------ end iteration ------------ C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-| DO j = jMin, jMax DO i = iMin, iMax IF ( icMask(i,j).GT.0. _d 0 ) THEN C-- Compute new bottom layer temperature. k32 = 2. _d 0*kIce / hIce(i,j) tIc2(i,j) = ( 2. _d 0*dt*k32*(tIc1(i,j)+2. _d 0*tFrz(i,j)) & + rhoi*cpIce*hIce(i,j)*tIc2(i,j)) & /(6. _d 0*dt*k32 + rhoi*cpIce*hIce(i,j)) #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1010) & 'ThSI_SOLVE4T: k, Ts, Tice=',k,Tsf(i,j),tIc1(i,j),tIc2(i,j) netSW = flxAtm(i,j) #endif C-- Compute final flux values at surfaces. tSrf1(i,j) = Tsf(i,j) fct = k12(i,j)*(Tsf(i,j)-tIc1(i,j)) flxCnB(i,j) = 4. _d 0*kIce *(tIc2(i,j)-tFrz(i,j))/hIce(i,j) flxNet = sHeat(i,j) + flxTexSW(i,j) flxNet = flxNet + dFlxdT(i,j)*dTsrf1(i,j) #ifndef ALLOW_AUTODIFF IF ( useBlkFlx ) THEN #endif C- needs to update also Evap (Tsf changes) since Latent heat has been updated evpAtm(i,j) = evapT(i,j) + dEvdT(i,j)*dTsrf1(i,j) #ifndef ALLOW_AUTODIFF ELSE C- WARNING: Evap & +Evap*Lfresh are missing ! (but only affects Diagnostics) evpAtm(i,j) = 0. ENDIF #endif C- Update energy flux to Atmos with other than SW contributions; C use latent heat = Lvap (energy=0 for liq. water at 0.oC) flxAtm(i,j) = flxAtm(i,j) + flxTexSW(i,j) & + dFlxdT(i,j)*dTsrf1(i,j) + evpAtm(i,j)*Lfresh C- excess of energy @ surface (used for surface melting): sHeat(i,j) = flxNet - fct #ifdef ALLOW_DBUG_THSICE IF ( dBug(i,j,bi,bj) ) WRITE(stdUnit,1020) & 'ThSI_SOLVE4T: flxNet,fct,Dif,flxCnB=', & flxNet,fct,flxNet-fct,flxCnB(i,j) #endif C-- Compute new enthalpy for each layer. qIc1(i,j) = -cpWater*Tmlt1 + cpIce *(Tmlt1-tIc1(i,j)) & + Lfresh*(1. _d 0-Tmlt1/tIc1(i,j)) qIc2(i,j) = -cpIce *tIc2(i,j) + Lfresh #ifdef ALLOW_DBUG_THSICE C-- Make sure internal ice temperatures do not exceed Tmlt. C (This should not happen for reasonable values of i0swFrac) IF (tIc1(i,j) .GE. Tmlt1) THEN WRITE(stdUnit,'(A,2I4,2I3,1P2E14.6)') & ' BBerr - Bug: IceT(1) > Tmlt',i,j,bi,bj,tIc1(i,j),Tmlt1 ENDIF IF (tIc2(i,j) .GE. 0. _d 0) THEN WRITE(stdUnit,'(A,2I4,2I3,1P2E14.6)') & ' BBerr - Bug: IceT(2) > 0',i,j,bi,bj,tIc2(i,j) ENDIF IF ( dBug(i,j,bi,bj) ) THEN WRITE(stdUnit,1020) 'ThSI_SOLV_4T: Tsf, Tice(1,2), dTsurf=', & Tsf(i,j), tIc1(i,j), tIc2(i,j), dTsrf1(i,j) WRITE(stdUnit,1020) 'ThSI_SOLV_4T: sHeat, flxCndBt, Qice =', & sHeat(i,j), flxCnB(i,j), qIc1(i,j), qIc2(i,j) WRITE(stdUnit,1020) 'ThSI_SOLV_4T: flxA, evpA, fxSW_bf,af=', & flxAtm(i,j), evpAtm(i,j), netSW, flxSW(i,j) ENDIF #endif ELSE C-- ice-free grid point: c tIc1 (i,j) = 0. _d 0 c tIc2 (i,j) = 0. _d 0 dTsrf1(i,j) = 0. _d 0 c sHeat (i,j) = 0. _d 0 c flxCnB(i,j) = 0. _d 0 c flxAtm(i,j) = 0. _d 0 c evpAtm(i,j) = 0. _d 0 ENDIF ENDDO ENDDO #endif /* ALLOW_THSICE */ C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-| RETURN END