MODULE ad_biology_mod ! !git $Id$ !svn $Id: ad_npzd_Franks.h 1151 2023-02-09 03:08:53Z arango $ !================================================== Hernan G. Arango === ! Copyright (c) 2002-2023 The ROMS/TOMS Group Andrew M. Moore ! ! Licensed under a MIT/X style license ! ! See License_ROMS.md ! !======================================================================= ! ! ! Nutrient-Phytoplankton-Zooplankton-Detritus Model. ! ! ! ! This routine computes the biological sources and sinks and adds ! ! then the global biological fields. ! ! ! ! Reference: ! ! ! ! Franks et al, 1986: Behavior of simple plankton model with ! ! food-level acclimation by herbivores, Marine Biology, 91, ! ! 121-129. ! ! ! !======================================================================= ! implicit none ! PRIVATE PUBLIC :: ad_biology ! CONTAINS ! !*********************************************************************** SUBROUTINE ad_biology (ng,tile) !*********************************************************************** ! USE mod_param USE mod_grid USE mod_ncparam USE mod_ocean USE mod_stepping ! ! Imported variable declarations. ! integer, intent(in) :: ng, tile ! ! Local variable declarations. ! character (len=*), parameter :: MyFile = & & __FILE__ ! #include "tile.h" ! ! Set header file name. ! #ifdef DISTRIBUTE IF (Lbiofile(iADM)) THEN #else IF (Lbiofile(iADM).and.(tile.eq.0)) THEN #endif Lbiofile(iADM)=.FALSE. BIONAME(iADM)=MyFile END IF ! #ifdef PROFILE CALL wclock_on (ng, iADM, 15, __LINE__, MyFile) #endif CALL ad_npzd_franks_tile (ng, tile, & & LBi, UBi, LBj, UBj, N(ng), NT(ng), & & IminS, ImaxS, JminS, JmaxS, & & nstp(ng), nnew(ng), & #ifdef MASKING & GRID(ng) % rmask, & #endif & GRID(ng) % Hz, & & GRID(ng) % ad_Hz, & & GRID(ng) % z_r, & & GRID(ng) % ad_z_r, & & GRID(ng) % z_w, & & GRID(ng) % ad_z_w, & & OCEAN(ng) % t, & & OCEAN(ng) % ad_t) #ifdef PROFILE CALL wclock_off (ng, iADM, 15, __LINE__, MyFile) #endif RETURN END SUBROUTINE ad_biology ! !----------------------------------------------------------------------- SUBROUTINE ad_npzd_franks_tile (ng, tile, & & LBi, UBi, LBj, UBj, UBk, UBt, & & IminS, ImaxS, JminS, JmaxS, & & nstp, nnew, & #ifdef MASKING & rmask, & #endif & Hz, ad_Hz, z_r, ad_z_r, & & z_w, ad_z_w, t, ad_t) !----------------------------------------------------------------------- ! USE mod_param USE mod_biology USE mod_ncparam USE mod_scalars ! ! Imported variable declarations. ! integer, intent(in) :: ng, tile integer, intent(in) :: LBi, UBi, LBj, UBj, UBk, UBt integer, intent(in) :: IminS, ImaxS, JminS, JmaxS integer, intent(in) :: nstp, nnew #ifdef ASSUMED_SHAPE # ifdef MASKING real(r8), intent(in) :: rmask(LBi:,LBj:) # endif real(r8), intent(in) :: Hz(LBi:,LBj:,:) real(r8), intent(in) :: z_r(LBi:,LBj:,:) real(r8), intent(in) :: z_w(LBi:,LBj:,0:) real(r8), intent(inout) :: t(LBi:,LBj:,:,:,:) real(r8), intent(inout) :: ad_Hz(LBi:,LBj:,:) real(r8), intent(inout) :: ad_z_r(LBi:,LBj:,:) real(r8), intent(inout) :: ad_z_w(LBi:,LBj:,0:) real(r8), intent(inout) :: ad_t(LBi:,LBj:,:,:,:) #else # ifdef MASKING real(r8), intent(in) :: rmask(LBi:UBi,LBj:UBj) # endif real(r8), intent(in) :: Hz(LBi:UBi,LBj:UBj,UBk) real(r8), intent(in) :: z_r(LBi:UBi,LBj:UBj,UBk) real(r8), intent(in) :: z_w(LBi:UBi,LBj:UBj,0:UBk) real(r8), intent(inout) :: t(LBi:UBi,LBj:UBj,UBk,3,UBt) real(r8), intent(inout) :: ad_Hz(LBi:UBi,LBj:UBj,UBk) real(r8), intent(inout) :: ad_z_r(LBi:UBi,LBj:UBj,UBk) real(r8), intent(inout) :: ad_z_w(LBi:UBi,LBj:UBj,0:UBk) real(r8), intent(inout) :: ad_t(LBi:UBi,LBj:UBj,UBk,3,UBt) #endif ! ! Local variable declarations. ! integer, parameter :: Nsink = 1 integer :: Iter, i, ibio, isink, itrc, itrmx, j, k, ks integer :: Iteradj integer, dimension(Nsink) :: idsink real(r8), parameter :: eps = 1.0e-16_r8 real(r8) :: cff, cff1, cff2, cff3, dtdays real(r8) :: ad_cff, ad_cff1 real(r8) :: adfac, adfac1, adfac2, adfac3 real(r8) :: cffL, cffR, cu, dltL, dltR real(r8) :: ad_cffL, ad_cffR, ad_cu, ad_dltL, ad_dltR real(r8), dimension(Nsink) :: Wbio real(r8), dimension(Nsink) :: ad_Wbio integer, dimension(IminS:ImaxS,N(ng)) :: ksource real(r8), dimension(IminS:ImaxS,N(ng),NT(ng)) :: Bio real(r8), dimension(IminS:ImaxS,N(ng),NT(ng)) :: Bio1 real(r8), dimension(IminS:ImaxS,N(ng),NT(ng)) :: Bio_old real(r8), dimension(IminS:ImaxS,N(ng),NT(ng)) :: ad_Bio real(r8), dimension(IminS:ImaxS,N(ng),NT(ng)) :: ad_Bio_old real(r8), dimension(IminS:ImaxS,0:N(ng)) :: FC real(r8), dimension(IminS:ImaxS,0:N(ng)) :: ad_FC real(r8), dimension(IminS:ImaxS,N(ng)) :: Hz_inv real(r8), dimension(IminS:ImaxS,N(ng)) :: Hz_inv2 real(r8), dimension(IminS:ImaxS,N(ng)) :: Hz_inv3 real(r8), dimension(IminS:ImaxS,N(ng)) :: WL real(r8), dimension(IminS:ImaxS,N(ng)) :: WR real(r8), dimension(IminS:ImaxS,N(ng)) :: bL real(r8), dimension(IminS:ImaxS,N(ng)) :: bL1 real(r8), dimension(IminS:ImaxS,N(ng)) :: bR real(r8), dimension(IminS:ImaxS,N(ng)) :: bR1 real(r8), dimension(IminS:ImaxS,N(ng)) :: qc real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_Hz_inv real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_Hz_inv2 real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_Hz_inv3 real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_WL real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_WR real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_bL real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_bR real(r8), dimension(IminS:ImaxS,N(ng)) :: ad_qc #include "set_bounds.h" ! !----------------------------------------------------------------------- ! Add biological Source/Sink terms. !----------------------------------------------------------------------- ! ! Avoid computing source/sink terms if no biological iterations. ! IF (BioIter(ng).le.0) RETURN ! ! Set time-stepping according to the number of iterations. ! dtdays=dt(ng)*sec2day/REAL(BioIter(ng),r8) ! ! Set vertical sinking indentification vector. ! idsink(1)=iSDet ! Small detritus ! ! Set vertical sinking velocity vector in the same order as the ! identification vector, IDSINK. ! Wbio(1)=wDet(ng) ! Small detritus ! J_LOOP : DO j=Jstr,Jend ! !----------------------------------------------------------------------- ! Initialize adjoint private variables. !----------------------------------------------------------------------- ! ad_dltL=0.0_r8 ad_dltR=0.0_r8 ad_cu=0.0_r8 ad_cff=0.0_r8 ad_cff1=0.0_r8 ad_cffL=0.0_r8 ad_cffR=0.0_r8 adfac=0.0_r8 adfac1=0.0_r8 adfac2=0.0_r8 adfac3=0.0_r8 ad_wDet(ng)=0.0_r8 ad_Wbio(1)=0.0_r8 ! DO k=1,N(ng) DO i=IminS,ImaxS ad_Hz_inv(i,k)=0.0_r8 ad_Hz_inv2(i,k)=0.0_r8 ad_Hz_inv3(i,k)=0.0_r8 ad_WL(i,k)=0.0_r8 ad_WR(i,k)=0.0_r8 ad_bL(i,k)=0.0_r8 ad_bR(i,k)=0.0_r8 ad_qc(i,k)=0.0_r8 END DO END DO DO k=0,N(ng) DO i=IminS,ImaxS ad_FC(i,k)=0.0_r8 END DO END DO ! ! Clear ad_Bio and Bio arrays. ! DO itrc=1,NBT ibio=idbio(itrc) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,ibio)=0.0_r8 Bio1(i,k,ibio)=0.0_r8 ad_Bio(i,k,ibio)=0.0_r8 ad_Bio_old(i,k,ibio)=0.0_r8 END DO END DO END DO ! ! Compute inverse thickness to avoid repeated divisions. ! DO k=1,N(ng) DO i=Istr,Iend Hz_inv(i,k)=1.0_r8/Hz(i,j,k) END DO END DO DO k=1,N(ng)-1 DO i=Istr,Iend Hz_inv2(i,k)=1.0_r8/(Hz(i,j,k)+Hz(i,j,k+1)) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend Hz_inv3(i,k)=1.0_r8/(Hz(i,j,k-1)+Hz(i,j,k)+Hz(i,j,k+1)) END DO END DO ! ! Compute required basic state variables Bio_old and Bio. ! ! Extract biological variables from tracer arrays, place them into ! scratch arrays, and restrict their values to be positive definite. ! At input, all tracers (index nnew) from predictor step have ! transport units (m Tunits) since we do not have yet the new ! values for zeta and Hz. These are known after the 2D barotropic ! time-stepping. In this routine, this is not a problem because ! we only use index nstp in the right-hand-side equations. ! DO itrc=1,NBT ibio=idbio(itrc) DO k=1,N(ng) DO i=Istr,Iend Bio_old(i,k,ibio)=t(i,j,k,nstp,ibio) END DO END DO END DO ! ! Determine Correction for negativity. ! DO k=1,N(ng) DO i=Istr,Iend cff1=MAX(0.0_r8,eps-Bio_old(i,k,iNO3_))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iPhyt))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iZoop))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iSDet)) ! ! If correction needed, determine the largest pool to debit. ! IF (cff1.gt.0.0) THEN itrmx=idbio(1) cff=t(i,j,k,nstp,itrmx) DO ibio=idbio(2),idbio(NBT) IF (t(i,j,k,nstp,ibio).gt.cff) THEN itrmx=ibio cff=t(i,j,k,nstp,ibio) END IF END DO ! ! Update new values. ! DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=MAX(eps,Bio_old(i,k,ibio))- & & cff1*(SIGN(0.5_r8, & & REAL(itrmx-ibio,r8)**2)+ & & SIGN(0.5_r8, & & -REAL(itrmx-ibio,r8)**2)) END DO ELSE DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=Bio_old(i,k,ibio) END DO END IF END DO END DO ! !======================================================================= ! Start internal iterations to achieve convergence of the nonlinear ! backward-implicit solution. !======================================================================= ! ! During the iterative procedure a series of fractional time steps are ! performed in a chained mode (splitting by different biological ! conversion processes) in sequence of the main food chain. In all ! stages the concentration of the component being consumed is treated ! in a fully implicit manner, so the algorithm guarantees non-negative ! values, no matter how strong the concentration of active consuming ! component (Phytoplankton or Zooplankton). The overall algorithm, ! as well as any stage of it, is formulated in conservative form ! (except explicit sinking) in sense that the sum of concentration of ! all components is conserved. ! ! In the implicit algorithm, we have for example (N: nutrient, ! P: phytoplankton), ! ! N(new) = N(old) - uptake * P(old) uptake = mu * N / (Kn + N) ! {Michaelis-Menten} ! below, we set ! The N in the numerator of ! cff = mu * P(old) / (Kn + N(old)) uptake is treated implicitly ! as N(new) ! ! so the time-stepping of the equations becomes: ! ! N(new) = N(old) / (1 + cff) (1) when substracting a sink term, ! consuming, divide by (1 + cff) ! and ! ! P(new) = P(old) + cff * N(new) (2) when adding a source term, ! growing, add (cff * source) ! ! Notice that if you substitute (1) in (2), you will get: ! ! P(new) = P(old) + cff * N(old) / (1 + cff) (3) ! ! If you add (1) and (3), you get ! ! N(new) + P(new) = N(old) + P(old) ! ! implying conservation regardless how "cff" is computed. Therefore, ! this scheme is unconditionally stable regardless of the conversion ! rate. It does not generate negative values since the constituent ! to be consumed is always treated implicitly. It is also biased ! toward damping oscillations. ! ! The iterative loop below is to iterate toward an universal Backward- ! Euler treatment of all terms. So if there are oscillations in the ! system, they are only physical oscillations. These iterations, ! however, do not improve the accuaracy of the solution. ! DO Iter=1,BioIter(ng) ! ! Nutrient uptake by phytoplankton. ! cff1=dtdays*Vm_NO3(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iPhyt)* & & cff1*EXP(K_ext(ng)*z_r(i,j,k))/ & & (K_NO3(ng)+Bio(i,k,iNO3_)) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)/ & & (1.0_r8+cff) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)+ & & Bio(i,k,iNO3_)*cff END DO END DO ! ! Phytoplankton grazing by Zooplankton and mortality to Detritus ! (rate: PhyMR). ! cff1=dtdays*ZooGR(ng) cff2=dtdays*PhyMR(ng) cff3=K_phy(ng)*K_phy(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iZoop)*Bio(i,k,iPhyt)*cff1/ & & (cff3+Bio(i,k,iPhyt)*Bio(i,k,iPhyt)) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)/ & & (1.0_r8+cff+cff2) Bio(i,k,iZoop)=Bio(i,k,iZoop)+ & & Bio(i,k,iPhyt)*cff*(1.0_r8-ZooGA(ng)) Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iPhyt)* & & (cff2+cff*(ZooGA(ng)-ZooEC(ng))) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iPhyt)*cff*ZooEC(ng) END DO END DO ! ! Zooplankton excretion to nutrients and mortality to Detritus. ! cff1=1.0_r8/(1.0_r8+dtdays*(ZooMR(ng)+ZooMD(ng))) cff2=dtdays*ZooMR(ng) cff3=dtdays*ZooMD(ng) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iZoop)=Bio(i,k,iZoop)*cff1 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iZoop)*cff2 Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iZoop)*cff3 END DO END DO ! ! Detritus breakdown to nutrients. ! cff1=dtdays*DetRR(ng) cff2=1.0_r8/(1.0_r8+cff1) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iSDet)=Bio(i,k,iSDet)*cff2 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iSDet)*cff1 END DO END DO ! !----------------------------------------------------------------------- ! Vertical sinking terms. !----------------------------------------------------------------------- ! ! Reconstruct vertical profile of selected biological constituents ! "Bio(:,:,isink)" in terms of a set of parabolic segments within each ! grid box. Then, compute semi-Lagrangian flux due to sinking. ! DO isink=1,Nsink ibio=idsink(isink) ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL IF ((dltR*dltL).lt.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO i=Istr,Iend FC(i,k-1)=0.0_r8 WL(i,k)=z_w(i,j,k-1)+cff WR(i,k)=Hz(i,j,k)*qc(i,k) ksource(i,k)=k END DO END DO DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN ksource(i,k)=ks+1 FC(i,k-1)=FC(i,k-1)+WR(i,ks) END IF END DO END DO END DO ! ! Finalize computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) FC(i,k-1)=FC(i,k-1)+ & & Hz(i,j,ks)*cu* & & (bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))) END DO END DO DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,ibio)=qc(i,k)+(FC(i,k)-FC(i,k-1))*Hz_inv(i,k) END DO END DO END DO END DO ! !----------------------------------------------------------------------- ! Update global tracer variables: Add increment due to BGC processes ! to tracer array in time index "nnew". Index "nnew" is solution after ! advection and mixing and has transport units (m Tunits) hence the ! increment is multiplied by Hz. Notice that we need to subtract ! original values "Bio_old" at the top of the routine to just account ! for the concentractions affected by BGC processes. This also takes ! into account any constraints (non-negative concentrations, carbon ! concentration range) specified before entering BGC kernel. If "Bio" ! were unchanged by BGC processes, the increment would be exactly ! zero. Notice that final tracer values, t(:,:,:,nnew,:) are not ! bounded >=0 so that we can preserve total inventory of nutrients ! when advection causes tracer concentration to go negative. !----------------------------------------------------------------------- ! DO itrc=1,NBT ibio=idbio(itrc) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,ibio)-Bio_old(i,k,ibio) !^ tl_t(i,j,k,nnew,ibio)=tl_t(i,j,k,nnew,ibio)+ & !^ & tl_cff*Hz(i,j,k)+cff*tl_Hz(i,j,k) !^ ad_Hz(i,j,k)=ad_Hz(i,j,k)+cff*ad_t(i,j,k,nnew,ibio) ad_cff=ad_cff+Hz(i,j,k)*ad_t(i,j,k,nnew,ibio) !^ tl_cff=tl_Bio(i,k,ibio)-tl_Bio_old(i,k,ibio) !^ ad_Bio_old(i,k,ibio)=ad_Bio_old(i,k,ibio)-ad_cff ad_Bio(i,k,ibio)=ad_Bio(i,k,ibio)+ad_cff ad_cff=0.0_r8 END DO END DO END DO ! !======================================================================= ! Start adjoint internal iterations to achieve convergence of the ! nonlinear backward-implicit solution. !======================================================================= ! ! During the iterative procedure a series of fractional time steps are ! performed in a chained mode (splitting by different biological ! conversion processes) in sequence of the main food chain. In all ! stages the concentration of the component being consumed is treated ! in fully implicit manner, so the algorithm guarantees non-negative ! values, no matter how strong s the concentration of active consuming ! component (Phytoplankton or Zooplankton). The overall algorithm, ! as well as any stage of it, is formulated in conservative form ! (except explicit sinking) in sense that the sum of concentration of ! all components is conserved. ! ITER_LOOP: DO Iter=BioIter(ng),1,-1 ! !----------------------------------------------------------------------- ! Adjoint vertical sinking terms. !----------------------------------------------------------------------- ! ! Reconstruct vertical profile of selected biological constituents ! "Bio(:,:,isink)" in terms of a set of parabolic segments within each ! grid box. Then, compute semi-Lagrangian flux due to sinking. ! ! ! Compute appropriate basic state arrays III. ! ! Determine Correction for negativity. ! DO k=1,N(ng) DO i=Istr,Iend cff1=MAX(0.0_r8,eps-Bio_old(i,k,iNO3_))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iPhyt))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iZoop))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iSDet)) ! ! If correction needed, determine the largest pool to debit. ! IF (cff1.gt.0.0) THEN itrmx=idbio(1) cff=t(i,j,k,nstp,itrmx) DO ibio=idbio(2),idbio(NBT) IF (t(i,j,k,nstp,ibio).gt.cff) THEN itrmx=ibio cff=t(i,j,k,nstp,ibio) END IF END DO ! ! Update new values. ! DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=MAX(eps,Bio_old(i,k,ibio))- & & cff1*(SIGN(0.5_r8, & & REAL(itrmx-ibio,r8)**2)+ & & SIGN(0.5_r8, & & -REAL(itrmx-ibio,r8)**2)) END DO ELSE DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=Bio_old(i,k,ibio) END DO END IF END DO END DO ! !======================================================================= ! Start internal iterations to achieve convergence of the nonlinear ! backward-implicit solution. !======================================================================= ! DO Iteradj=1,Iter ! ! Nutrient uptake by phytoplankton. ! cff1=dtdays*Vm_NO3(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iPhyt)* & & cff1*EXP(K_ext(ng)*z_r(i,j,k))/ & & (K_NO3(ng)+Bio(i,k,iNO3_)) Bio1(i,k,iNO3_)=Bio(i,k,iNO3_) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)/ & & (1.0_r8+cff) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)+ & & Bio(i,k,iNO3_)*cff END DO END DO ! ! Phytoplankton grazing by Zooplankton and mortality to Detritus ! (rate: PhyMR). ! cff1=dtdays*ZooGR(ng) cff2=dtdays*PhyMR(ng) cff3=K_phy(ng)*K_phy(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iZoop)*Bio(i,k,iPhyt)*cff1/ & & (cff3+Bio(i,k,iPhyt)*Bio(i,k,iPhyt)) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)/ & & (1.0_r8+cff+cff2) Bio1(i,k,iZoop)=Bio(i,k,iZoop) Bio(i,k,iZoop)=Bio(i,k,iZoop)+ & & Bio(i,k,iPhyt)*cff*(1.0_r8-ZooGA(ng)) Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iPhyt)* & & (cff2+cff*(ZooGA(ng)-ZooEC(ng))) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iPhyt)*cff*ZooEC(ng) END DO END DO ! ! Zooplankton excretion to nutrients and mortality to Detritus. ! cff1=1.0_r8/(1.0_r8+dtdays*(ZooMR(ng)+ZooMD(ng))) cff2=dtdays*ZooMR(ng) cff3=dtdays*ZooMD(ng) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iZoop)=Bio(i,k,iZoop)*cff1 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iZoop)*cff2 Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iZoop)*cff3 END DO END DO ! ! Detritus breakdown to nutrients. ! cff1=dtdays*DetRR(ng) cff2=1.0_r8/(1.0_r8+cff1) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iSDet)=Bio(i,k,iSDet)*cff2 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iSDet)*cff1 END DO END DO ! IF (Iteradj.ne.Iter) THEN ! !----------------------------------------------------------------------- ! Vertical sinking terms. !----------------------------------------------------------------------- ! ! Reconstruct vertical profile of selected biological constituents ! "Bio(:,:,isink)" in terms of a set of parabolic segments within each ! grid box. Then, compute semi-Lagrangian flux due to sinking. ! DO isink=1,Nsink ibio=idsink(isink) ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL IF ((dltR*dltL).lt.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO i=Istr,Iend FC(i,k-1)=0.0_r8 WL(i,k)=z_w(i,j,k-1)+cff WR(i,k)=Hz(i,j,k)*qc(i,k) ksource(i,k)=k END DO END DO DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN ksource(i,k)=ks+1 FC(i,k-1)=FC(i,k-1)+WR(i,ks) END IF END DO END DO END DO ! ! Finalize computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) FC(i,k-1)=FC(i,k-1)+ & & Hz(i,j,ks)*cu* & & (bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))) END DO END DO DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,ibio)=qc(i,k)+ & & (FC(i,k)-FC(i,k-1))*Hz_inv(i,k) END DO END DO END DO END IF END DO ! ! End compute basic state arrays III. ! ! SINK_LOOP: DO isink=1,Nsink ibio=idsink(isink) ! ! Compute required flux arrays. ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL IF ((dltR*dltL).lt.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO i=Istr,Iend FC(i,k-1)=0.0_r8 WL(i,k)=z_w(i,j,k-1)+cff WR(i,k)=Hz(i,j,k)*qc(i,k) ksource(i,k)=k END DO END DO DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN ksource(i,k)=ks+1 FC(i,k-1)=FC(i,k-1)+WR(i,ks) END IF END DO END DO END DO ! ! Finalize computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) FC(i,k-1)=FC(i,k-1)+ & & Hz(i,j,ks)*cu* & & (bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))) END DO END DO DO k=1,N(ng) DO i=Istr,Iend !^ tl_Bio(i,k,ibio)=tl_qc(i,k)+ & !^ & (tl_FC(i,k)-tl_FC(i,k-1))*Hz_inv(i,k)+ & !^ & (FC(i,k)-FC(i,k-1))*tl_Hz_inv(i,k) !^ adfac=Hz_inv(i,k)*ad_Bio(i,k,ibio) ad_FC(i,k-1)=ad_FC(i,k-1)-adfac ad_FC(i,k )=ad_FC(i,k )+adfac ad_Hz_inv(i,k)=ad_Hz_inv(i,k)+ & & (FC(i,k)-FC(i,k-1))*ad_Bio(i,k,ibio) ad_qc(i,k)=ad_qc(i,k)+ad_Bio(i,k,ibio) ad_Bio(i,k,ibio)=0.0_r8 END DO END DO ! ! Adjoint of final computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) !^ tl_FC(i,k-1)=tl_FC(i,k-1)+ & !^ & (tl_Hz(i,j,ks)*cu+Hz(i,j,ks)*tl_cu)* & !^ & (bL(i,ks)+ & !^ & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & !^ & (1.5_r8-cu)* & !^ & (bR(i,ks)+bL(i,ks)- & !^ & 2.0_r8*qc(i,ks))))+ & !^ & Hz(i,j,ks)*cu* & !^ & (tl_bL(i,ks)+ & !^ & tl_cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & !^ & (1.5_r8-cu)* & !^ & (bR(i,ks)+bL(i,ks)- & !^ & 2.0_r8*qc(i,ks)))+ & !^ & cu*(0.5_r8*(tl_bR(i,ks)-tl_bL(i,ks))+ & !^ & tl_cu* & !^ & (bR(i,ks)+bL(i,ks)-2.0_r8*qc(i,ks))- & !^ & (1.5_r8-cu)* & !^ & (tl_bR(i,ks)+tl_bL(i,ks)- & !^ & 2.0_r8*tl_qc(i,ks)))) !^ adfac=(bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks))))*ad_FC(i,k-1) adfac1=Hz(i,j,ks)*cu*ad_FC(i,k-1) adfac2=adfac1*cu adfac3=adfac2*(1.5_r8-cu) ad_Hz(i,j,ks)=ad_Hz(i,j,ks)+cu*adfac ad_cu=ad_cu+Hz(i,j,ks)*adfac ad_bL(i,ks)=ad_bL(i,ks)+adfac1 ad_cu=ad_cu+ & & adfac1*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))+ & & adfac2*(bR(i,ks)+bL(i,ks)-2.0_r8*qc(i,ks)) ad_bR(i,ks)=ad_bR(i,ks)+0.5_r8*adfac2-adfac3 ad_bL(i,ks)=ad_bL(i,ks)-0.5_r8*adfac2-adfac3 ad_qc(i,ks)=ad_qc(i,ks)+2.0_r8*adfac3 !^ tl_cu=(0.5_r8+SIGN(0.5_r8, & !^ & (1.0_r8-(WL(i,k)-z_w(i,j,ks-1))* & !^ & Hz_inv(i,ks))))* & !^ & ((tl_WL(i,k)-tl_z_w(i,j,ks-1))*Hz_inv(i,ks)+ & !^ & (WL(i,k)-z_w(i,j,ks-1))*tl_Hz_inv(i,ks)) !^ adfac=(0.5_r8+SIGN(0.5_r8, & & (1.0_r8-(WL(i,k)-z_w(i,j,ks-1))* & & Hz_inv(i,ks))))*ad_cu adfac1=adfac*Hz_inv(i,ks) ad_WL(i,k)=ad_WL(i,k)+adfac1 ad_z_w(i,j,ks-1)=ad_z_w(i,j,ks-1)-adfac1 ad_Hz_inv(i,ks)=ad_Hz_inv(i,ks)+ & & (WL(i,k)-z_w(i,j,ks-1))*adfac ad_cu=0.0_r8 END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN !^ tl_FC(i,k-1)=tl_FC(i,k-1)+tl_WR(i,ks) !^ ad_WR(i,ks)=ad_WR(i,ks)+ad_FC(i,k-1) END IF END DO END DO END DO DO k=1,N(ng) DO i=Istr,Iend !^ tl_WR(i,k)=tl_Hz(i,j,k)*qc(i,k)+Hz(i,j,k)*tl_qc(i,k) !^ ad_Hz(i,j,k)=ad_Hz(i,j,k)+qc(i,k)*ad_WR(i,k) ad_qc(i,k)=ad_qc(i,k)+Hz(i,j,k)*ad_WR(i,k) ad_WR(i,k)=0.0_r8 !^ tl_WL(i,k)=tl_z_w(i,j,k-1)+tl_cff !^ ad_z_w(i,j,k-1)=ad_z_w(i,j,k-1)+ad_WL(i,k) ad_cff=ad_cff+ad_WL(i,k) ad_WL(i,k)=0.0_r8 !^ tl_FC(i,k-1)=0.0_r8 !^ ad_FC(i,k-1)=0.0_r8 END DO END DO !^ tl_cff=dtdays*SIGN(1.0_r8,Wbio(isink))*tl_Wbio(isink) !^ ad_Wbio(isink)=ad_Wbio(isink)+ & & dtdays*SIGN(1.0_r8,Wbio(isink))*ad_cff ad_cff=0.0_r8 ! ! Compute appropriate values of bR and bL. ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL !^ tl_bL(i,k)=tl_qc(i,k)-tl_dltL !^ ad_qc(i,k)=ad_qc(i,k)+ad_bL(i,k) ad_dltL=ad_dltL-ad_bL(i,k) ad_bL(i,k)=0.0_r8 !^ tl_bR(i,k)=tl_qc(i,k)+tl_dltR !^ ad_qc(i,k)=ad_qc(i,k)+ad_bR(i,k) ad_dltR=ad_dltR+ad_bR(i,k) ad_bR(i,k)=0.0_r8 IF ((dltR*dltL).lt.0.0_r8) THEN !^ tl_dltR=0.0_r8 !^ ad_dltR=0.0_r8 !^ tl_dltL=0.0_r8 !^ ad_dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN !^ tl_dltR=tl_cffL !^ ad_cffL=ad_cffL+ad_dltR ad_dltR=0.0_r8 ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN !^ tl_dltL=tl_cffR !^ ad_cffR=ad_cffR+ad_dltL ad_dltL=0.0_r8 END IF !^ tl_cffL=2.0_r8*tl_dltL !^ ad_dltL=ad_dltL+2.0_r8*ad_cffL ad_cffL=0.0_r8 !^ tl_cffR=2.0_r8*tl_dltR !^ ad_dltR=ad_dltR+2.0_r8*ad_cffR ad_cffR=0.0_r8 !^ tl_dltL=tl_qc(i,k)-tl_bL(i,k) !^ ad_qc(i,k)=ad_qc(i,k)+ad_dltL ad_bL(i,k)=ad_bL(i,k)-ad_dltL ad_dltL=0.0_r8 !^ tl_dltR=tl_bR(i,k)-tl_qc(i,k) !^ ad_bR(i,k)=ad_bR(i,k)+ad_dltR ad_qc(i,k)=ad_qc(i,k)-ad_dltR ad_dltR=0.0_r8 END DO END DO DO i=Istr,Iend #if defined LINEAR_CONTINUATION !^ tl_bR(i,1)=tl_bL(i,2) !^ ad_bL(i,2)=ad_bL(i,2)+ad_bR(i,1) ad_bR(i,1)=0.0_r8 !^ tl_bL(i,1)=2.0_r8*tl_qc(i,1)-tl_bR(i,1) !^ ad_qc(i,1)=ad_qc(i,1)+2.0_r8*ad_bL(i,1) ad_bR(i,1)=ad_bR(i,1)-ad_bL(i,1) ad_bL(i,1)=0.0_r8 #elif defined NEUMANN !^ tl_bR(i,1)=tl_bL(i,2) !^ ad_bL(i,2)=ad_bL(i,2)+ad_bR(i,1) ad_bR(i,1)=0.0_r8 !^ tl_bL(i,1)=1.5_r8*tl_qc(i,1)-0.5_r8*tl_bR(i,1) !^ ad_qc(i,1)=ad_qc(i,1)+1.5_r8*ad_bL(i,1) ad_bR(i,1)=ad_bR(i,1)-0.5_r8*ad_bL(i,1) ad_bL(i,1)=0.0_r8 #else !^ tl_bL(i,2)=tl_qc(i,1) ! bottom grid boxes are !^ tl_bR(i,1)=tl_qc(i,1) ! re-assumed to be !^ tl_bL(i,1)=tl_qc(i,1) ! piecewise constant. !^ ad_qc(i,1)=ad_qc(i,1)+ad_bL(i,1)+ & & ad_bR(i,1)+ & & ad_bL(i,2) ad_bL(i,1)=0.0_r8 ad_bR(i,1)=0.0_r8 ad_bL(i,2)=0.0_r8 #endif #if defined LINEAR_CONTINUATION !^ tl_bL(i,N(ng))=tl_bR(i,N(ng)-1) !^ ad_bR(i,N(ng)-1)=ad_bR(i,N(ng)-1)+ad_bL(i,N(ng)) ad_bL(i,N(ng))=0.0_r8 !^ tl_bR(i,N(ng))=2.0_r8*tl_qc(i,N(ng))-tl_bL(i,N(ng)) !^ ad_qc(i,N(ng))=ad_qc(i,N(ng))+2.0_r8*ad_bR(i,N(ng)) ad_bL(i,N(ng))=ad_bL(i,N(ng))-ad_bR(i,N(ng)) ad_bR(i,N(ng))=0.0_r8 #elif defined NEUMANN !^ tl_bL(i,N(ng))=tl_bR(i,N(ng)-1) !^ ad_bR(i,N(ng)-1)=ad_bR(i,N(ng)-1)+ad_bL(i,N(ng)) ad_bL(i,N(ng))=0.0_r8 !^ tl_bR(i,N(ng))=1.5_r8*tl_qc(i,N(ng))-0.5_r8*tl_bL(i,N(ng)) !^ ad_qc(i,N(ng))=ad_qc(i,N(ng))+1.5_r8*ad_bR(i,N(ng)) ad_bL(i,N(ng))=ad_bL(i,N(ng))-0.5_r8*ad_bR(i,N(ng)) ad_bR(i,N(ng))=0.0_r8 #else !^ tl_bR(i,N(ng))=tl_qc(i,N(ng)) ! default strictly monotonic !^ tl_bL(i,N(ng))=tl_qc(i,N(ng)) ! conditions !^ tl_bR(i,N(ng)-1)=tl_qc(i,N(ng)) !^ ad_qc(i,N(ng))=ad_qc(i,N(ng))+ad_bR(i,N(ng)-1)+ & & ad_bL(i,N(ng))+ & & ad_bR(i,N(ng)) ad_bR(i,N(ng)-1)=0.0_r8 ad_bL(i,N(ng))=0.0_r8 ad_bR(i,N(ng))=0.0_r8 #endif END DO ! ! Compute WR and WL arrays appropriate for this part of the code. ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR1(i,k)=bR(i,k) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL1(i,k+1)=bL(i,k+1) bL(i,k+1)=bR(i,k) !^ tl_bL(i,k+1)=tl_bR(i,k) !^ ad_bR(i,k)=ad_bR(i,k)+ad_bL(i,k+1) ad_bL(i,k+1)=0.0_r8 !^ tl_bR(i,k)=(tl_dltR*bR1(i,k )+dltR*tl_bR(i,k )+ & !^ & tl_dltL*bL1(i,k+1)+dltL*tl_bL(i,k+1))/ & !^ & (dltR+dltL)- & !^ & (tl_dltR+tl_dltL)*bR(i,k)/(dltR+dltL) !^ adfac=ad_bR(i,k)/(dltR+dltL) adfac1=ad_bR(i,k)*bR(i,k)/(dltR+dltL) ad_dltR=ad_dltR+adfac*bR1(i,k) ad_dltL=ad_dltL+adfac*bL1(i,k+1) ad_bL(i,k+1)=ad_bL(i,k+1)+dltL*adfac ad_dltR=ad_dltR-adfac1 ad_dltL=ad_dltL-adfac1 ad_bR(i,k)=dltR*adfac !^ tl_dltR=(0.5_r8-SIGN(0.5_r8,cff-WR(i,k+1)))* & !^ & tl_WR(i,k+1) !^ ad_WR(i,k+1)=ad_WR(i,k+1)+ & & (0.5_r8-SIGN(0.5_r8,cff-WR(i,k+1)))* & & ad_dltR ad_dltR=0.0_r8 !^ tl_dltL=(0.5_r8-SIGN(0.5_r8,cff-WL(i,k )))* & !^ & tl_WL(i,k ) ad_WL(i,k )=ad_WL(i,k )+ & & (0.5_r8-SIGN(0.5_r8,cff-WL(i,k )))* & & ad_dltL ad_dltL=0.0_r8 END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend ! ! Compute appropriate dltL and dltr. ! dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) !^ tl_WL(i,k)=2.0_r8*(dltR-2.0_r8*dltL)* & !^ & (tl_dltR-2.0_r8*tl_dltL) !^ adfac=ad_WL(i,k)*2.0_r8*(dltR-2.0_r8*dltL) ad_dltR=ad_dltR+adfac ad_dltL=ad_dltL-2.0_r8*adfac ad_WL(i,k)=0.0_r8 !^ tl_WR(i,k)=2.0_r8*(2.0_r8*dltR-dltL)* & !^ & (2.0_r8*tl_dltR-tl_dltL) !^ adfac=ad_WR(i,k)*2.0_r8*(2.0_r8*dltR-dltL) ad_dltR=ad_dltR+2.0_r8*adfac ad_dltL=ad_dltL-adfac ad_WR(i,k)=0.0_r8 !^ tl_bL(i,k)=tl_qc(i,k)-tl_dltL !^ ad_qc(i,k)=ad_qc(i,k)+ad_bL(i,k) ad_dltL=ad_dltL-ad_bL(i,k) ad_bL(i,k)=0.0_r8 !^ tl_bR(i,k)=tl_qc(i,k)+tl_dltR !^ ad_qc(i,k)=ad_qc(i,k)+ad_bR(i,k) ad_dltR=ad_dltR+ad_bR(i,k) ad_bR(i,k)=0.0_r8 ! ! Compute appropriate dltL and dltr. ! dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF cff=(dltR-dltL)*Hz_inv3(i,k) !^ tl_dltL=tl_dltL+tl_cff*Hz(i,j,k-1)+cff*tl_Hz(i,j,k-1) !^ ad_cff=ad_cff+ad_dltL*Hz(i,j,k-1) ad_Hz(i,j,k-1)=ad_Hz(i,j,k-1)+cff*ad_dltL !^ tl_dltR=tl_dltR-tl_cff*Hz(i,j,k+1)-cff*tl_Hz(i,j,k+1) !^ ad_cff=ad_cff-ad_dltR*Hz(i,j,k+1) ad_Hz(i,j,k+1)=ad_Hz(i,j,k+1)-cff*ad_dltR !^ tl_cff=(tl_dltR-tl_dltL)*Hz_inv3(i,k)+ & !^ & (dltR-dltL)*tl_Hz_inv3(i,k) !^ adfac=ad_cff*Hz_inv3(i,k) ad_dltR=ad_dltR+adfac ad_dltL=ad_dltL-adfac ad_Hz_inv3(i,k)=ad_Hz_inv3(i,k)+(dltR-dltL)*ad_cff ad_cff=0.0_r8 ! ! Compute appropriate dltL and dltr. ! dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) IF ((dltR*dltL).le.0.0_r8) THEN !^ tl_dltR=0.0_r8 !^ ad_dltR=0.0_r8 !^ tl_dltL=0.0_r8 !^ ad_dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN !^ tl_dltR=tl_cffL !^ ad_cffL=ad_cffL+ad_dltR ad_dltR=0.0_r8 ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN !^ tl_dltL=tl_cffR !^ ad_cffR=ad_cffR+ad_dltL ad_dltL=0.0_r8 END IF !^ tl_cffL=tl_cff*FC(i,k-1)+cff*tl_FC(i,k-1) !^ ad_cff=ad_cff+ad_cffL*FC(i,k-1) ad_FC(i,k-1)=ad_FC(i,k-1)+cff*ad_cffL ad_cffL=0.0_r8 !^ tl_cffR=tl_cff*FC(i,k)+cff*tl_FC(i,k) !^ ad_cff=ad_cff+ad_cffR*FC(i,k) ad_FC(i,k)=ad_FC(i,k)+cff*ad_cffR ad_cffR=0.0_r8 !^ tl_cff=tl_Hz(i,j,k-1)+2.0_r8*tl_Hz(i,j,k)+tl_Hz(i,j,k+1) !^ ad_Hz(i,j,k-1)=ad_Hz(i,j,k-1)+ad_cff ad_Hz(i,j,k)=ad_Hz(i,j,k)+2.0_r8*ad_cff ad_Hz(i,j,k+1)=ad_Hz(i,j,k+1)+ad_cff ad_cff=0.0_r8 !^ tl_dltL=tl_Hz(i,j,k)*FC(i,k-1)+Hz(i,j,k)*tl_FC(i,k-1) !^ ad_Hz(i,j,k)=ad_Hz(i,j,k)+ad_dltL*FC(i,k-1) ad_FC(i,k-1)=ad_FC(i,k-1)+ad_dltL*Hz(i,j,k) ad_dltL=0.0_r8 !^ tl_dltR=tl_Hz(i,j,k)*FC(i,k)+Hz(i,j,k)*tl_FC(i,k) !^ ad_Hz(i,j,k)=ad_Hz(i,j,k)+ad_dltR*FC(i,k) ad_FC(i,k)=ad_FC(i,k)+ad_dltR*Hz(i,j,k) ad_dltR=0.0_r8 END DO END DO DO k=N(ng)-1,1,-1 DO i=Istr,Iend !^ tl_FC(i,k)=(tl_qc(i,k+1)-tl_qc(i,k))*Hz_inv2(i,k)+ & !^ & (qc(i,k+1)-qc(i,k))*tl_Hz_inv2(i,k) !^ adfac=ad_FC(i,k)*Hz_inv2(i,k) ad_qc(i,k+1)=ad_qc(i,k+1)+adfac ad_qc(i,k)=ad_qc(i,k)-adfac ad_Hz_inv2(i,k)=ad_Hz_inv2(i,k)+(qc(i,k+1)-qc(i,k))* & & ad_FC(i,k) ad_FC(i,k)=0.0_r8 END DO END DO DO k=1,N(ng) DO i=Istr,Iend !^ tl_qc(i,k)=tl_Bio(i,k,ibio) !^ ad_Bio(i,k,ibio)=ad_Bio(i,k,ibio)+ad_qc(i,k) ad_qc(i,k)=0.0_r8 END DO END DO END DO SINK_LOOP ! ! Compute appropriate basic state arrays II. ! ! Determine Correction for negativity. ! DO k=1,N(ng) DO i=Istr,Iend cff1=MAX(0.0_r8,eps-Bio_old(i,k,iNO3_))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iPhyt))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iZoop))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iSDet)) ! ! If correction needed, determine the largest pool to debit. ! IF (cff1.gt.0.0) THEN itrmx=idbio(1) cff=t(i,j,k,nstp,itrmx) DO ibio=idbio(2),idbio(NBT) IF (t(i,j,k,nstp,ibio).gt.cff) THEN itrmx=ibio cff=t(i,j,k,nstp,ibio) END IF END DO ! ! Update new values. ! DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=MAX(eps,Bio_old(i,k,ibio))- & & cff1*(SIGN(0.5_r8, & & REAL(itrmx-ibio,r8)**2)+ & & SIGN(0.5_r8, & & -REAL(itrmx-ibio,r8)**2)) END DO ELSE DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=Bio_old(i,k,ibio) END DO END IF END DO END DO ! !======================================================================= ! Start internal iterations to achieve convergence of the nonlinear ! backward-implicit solution. !======================================================================= ! DO Iteradj=1,Iter ! ! Nutrient uptake by phytoplankton. ! cff1=dtdays*Vm_NO3(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iPhyt)* & & cff1*EXP(K_ext(ng)*z_r(i,j,k))/ & & (K_NO3(ng)+Bio(i,k,iNO3_)) Bio1(i,k,iNO3_)=Bio(i,k,iNO3_) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)/ & & (1.0_r8+cff) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)+ & & Bio(i,k,iNO3_)*cff END DO END DO ! ! Phytoplankton grazing by Zooplankton and mortality to Detritus ! (rate: PhyMR). ! cff1=dtdays*ZooGR(ng) cff2=dtdays*PhyMR(ng) cff3=K_phy(ng)*K_phy(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iZoop)*Bio(i,k,iPhyt)*cff1/ & & (cff3+Bio(i,k,iPhyt)*Bio(i,k,iPhyt)) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)/ & & (1.0_r8+cff+cff2) Bio1(i,k,iZoop)=Bio(i,k,iZoop) Bio(i,k,iZoop)=Bio(i,k,iZoop)+ & & Bio(i,k,iPhyt)*cff*(1.0_r8-ZooGA(ng)) Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iPhyt)* & & (cff2+cff*(ZooGA(ng)-ZooEC(ng))) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iPhyt)*cff*ZooEC(ng) END DO END DO ! IF (Iteradj.ne.Iter) THEN ! ! Zooplankton excretion to nutrients and mortality to Detritus. ! cff1=1.0_r8/(1.0_r8+dtdays*(ZooMR(ng)+ZooMD(ng))) cff2=dtdays*ZooMR(ng) cff3=dtdays*ZooMD(ng) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iZoop)=Bio(i,k,iZoop)*cff1 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iZoop)*cff2 Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iZoop)*cff3 END DO END DO ! ! Detritus breakdown to nutrients. ! cff1=dtdays*DetRR(ng) cff2=1.0_r8/(1.0_r8+cff1) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iSDet)=Bio(i,k,iSDet)*cff2 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iSDet)*cff1 END DO END DO ! !----------------------------------------------------------------------- ! Vertical sinking terms. !----------------------------------------------------------------------- ! ! Reconstruct vertical profile of selected biological constituents ! "Bio(:,:,isink)" in terms of a set of parabolic segments within each ! grid box. Then, compute semi-Lagrangian flux due to sinking. ! DO isink=1,Nsink ibio=idsink(isink) ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL IF ((dltR*dltL).lt.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO i=Istr,Iend FC(i,k-1)=0.0_r8 WL(i,k)=z_w(i,j,k-1)+cff WR(i,k)=Hz(i,j,k)*qc(i,k) ksource(i,k)=k END DO END DO DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN ksource(i,k)=ks+1 FC(i,k-1)=FC(i,k-1)+WR(i,ks) END IF END DO END DO END DO ! ! Finalize computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) FC(i,k-1)=FC(i,k-1)+ & & Hz(i,j,ks)*cu* & & (bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))) END DO END DO DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,ibio)=qc(i,k)+ & & (FC(i,k)-FC(i,k-1))*Hz_inv(i,k) END DO END DO END DO END IF END DO ! ! End compute basic state arrays II. ! ! Adjoint Detritus breakdown to nutrients. ! cff1=dtdays*DetRR(ng) cff2=1.0_r8/(1.0_r8+cff1) DO k=1,N(ng) DO i=Istr,Iend !^ tl_Bio(i,k,iNO3_)=tl_Bio(i,k,iNO3_)+ & !^ & tl_Bio(i,k,iSDet)*cff1 !^ ad_Bio(i,k,iSDet)=ad_Bio(i,k,iSDet)+ & & cff1*ad_Bio(i,k,iNO3_) !^ tl_Bio(i,k,iSDet)=tl_Bio(i,k,iSDet)*cff2 !^ ad_Bio(i,k,iSDet)=cff2*ad_Bio(i,k,iSDet) END DO END DO ! ! Adjoint Zooplankton excretion to nutrients and mortality to Detritus. ! cff1=1.0_r8/(1.0_r8+dtdays*(ZooMR(ng)+ZooMD(ng))) cff2=dtdays*ZooMR(ng) cff3=dtdays*ZooMD(ng) DO k=1,N(ng) DO i=Istr,Iend !^ tl_Bio(i,k,iSDet)=tl_Bio(i,k,iSDet)+ & !^ & tl_Bio(i,k,iZoop)*cff3 !^ ad_Bio(i,k,iZoop)=ad_Bio(i,k,iZoop)+ & & cff3*ad_Bio(i,k,iSDet) !^ tl_Bio(i,k,iNO3_)=tl_Bio(i,k,iNO3_)+ & !^ & tl_Bio(i,k,iZoop)*cff2 !^ ad_Bio(i,k,iZoop)=ad_Bio(i,k,iZoop)+ & & cff2*ad_Bio(i,k,iNO3_) !^ tl_Bio(i,k,iZoop)=tl_Bio(i,k,iZoop)*cff1 !^ ad_Bio(i,k,iZoop)=cff1*ad_Bio(i,k,iZoop) END DO END DO ! ! Phytoplankton grazing by Zooplankton and mortality to Detritus ! (rate: PhyMR). ! cff1=dtdays*ZooGR(ng) cff2=dtdays*PhyMR(ng) cff3=K_phy(ng)*K_phy(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio1(i,k,iZoop)*Bio1(i,k,iPhyt)*cff1/ & & (cff3+Bio1(i,k,iPhyt)*Bio1(i,k,iPhyt)) !^ tl_Bio(i,k,iNO3_)=tl_Bio(i,k,iNO3_)+ & !^ & tl_Bio(i,k,iPhyt)*cff*ZooEC(ng)+ & !^ & Bio(i,k,iPhyt)*tl_cff*ZooEC(ng) !^ ad_cff=ad_cff+ & & Bio(i,k,iPhyt)*ZooEC(ng)*ad_Bio(i,k,iNO3_) ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)+ & & cff*ZooEC(ng)*ad_Bio(i,k,iNO3_) !^ tl_Bio(i,k,iSDet)=tl_Bio(i,k,iSDet)+ & !^ & tl_Bio(i,k,iPhyt)* & !^ & (cff2+cff*(ZooGA(ng)-ZooEC(ng)))+ & !^ & Bio(i,k,iPhyt)* & !^ & tl_cff*(ZooGA(ng)-ZooEC(ng)) !^ ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)+ & & (cff2+cff*(ZooGA(ng)-ZooEC(ng)))* & & ad_Bio(i,k,iSDet) ad_cff=ad_cff+ & & Bio(i,k,iPhyt)*(ZooGA(ng)-ZooEC(ng))* & & ad_Bio(i,k,iSDet) !^ tl_Bio(i,k,iZoop)=tl_Bio(i,k,iZoop)+ & !^ & tl_Bio(i,k,iPhyt)* & !^ & cff*(1.0_r8-ZooGA(ng))+ & !^ & Bio(i,k,iPhyt)* & !^ & tl_cff*(1.0_r8-ZooGA(ng)) !^ ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)+ & & cff*(1.0_r8-ZooGA(ng))* & & ad_Bio(i,k,iZoop) ad_cff=ad_cff+ & & Bio(i,k,iPhyt)*(1.0_r8-ZooGA(ng))* & & ad_Bio(i,k,iZoop) !^ tl_Bio(i,k,iPhyt)=(tl_Bio(i,k,iPhyt)- & !^ & tl_cff*Bio(i,k,iPhyt))/ & !^ & (1.0_r8+cff+cff2) !^ adfac=ad_Bio(i,k,iPhyt)/(1.0_r8+cff+cff2) ad_cff=ad_cff-Bio(i,k,iPhyt)*adfac ad_Bio(i,k,iPhyt)=adfac !^ tl_cff=((tl_Bio(i,k,iZoop)*Bio1(i,k,iPhyt)+ & !^ & Bio1(i,k,iZoop)*tl_Bio(i,k,iPhyt))*cff1- & !^ & 2.0_r8*Bio1(i,k,iPhyt)*tl_Bio(i,k,iPhyt)*cff)/ & !^ & (cff3+Bio1(i,k,iPhyt)*Bio1(i,k,iPhyt)) !^ adfac=ad_cff/(cff3+Bio1(i,k,iPhyt)*Bio1(i,k,iPhyt)) adfac1=adfac*cff1 ad_Bio(i,k,iZoop)=ad_Bio(i,k,iZoop)+ & & Bio1(i,k,iPhyt)*adfac1 ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)+ & & Bio1(i,k,iZoop)*adfac1 ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)- & & 2.0_r8*Bio1(i,k,iPhyt)*cff*adfac ad_cff=0.0_r8 END DO END DO ! ! Compute appropriate basic state arrays I. ! ! Determine Correction for negativity. ! DO k=1,N(ng) DO i=Istr,Iend cff1=MAX(0.0_r8,eps-Bio_old(i,k,iNO3_))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iPhyt))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iZoop))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iSDet)) ! ! If correction needed, determine the largest pool to debit. ! IF (cff1.gt.0.0) THEN itrmx=idbio(1) cff=t(i,j,k,nstp,itrmx) DO ibio=idbio(2),idbio(NBT) IF (t(i,j,k,nstp,ibio).gt.cff) THEN itrmx=ibio cff=t(i,j,k,nstp,ibio) END IF END DO ! ! Update new values. ! DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=MAX(eps,Bio_old(i,k,ibio))- & & cff1*(SIGN(0.5_r8, & & REAL(itrmx-ibio,r8)**2)+ & & SIGN(0.5_r8, & & -REAL(itrmx-ibio,r8)**2)) END DO ELSE DO itrc=1,NBT ibio=idbio(itrc) Bio(i,k,ibio)=Bio_old(i,k,ibio) END DO END IF END DO END DO ! !======================================================================= ! Start internal iterations to achieve convergence of the nonlinear ! backward-implicit solution. !======================================================================= ! DO Iteradj=1,Iter ! ! Nutrient uptake by phytoplankton. ! cff1=dtdays*Vm_NO3(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iPhyt)* & & cff1*EXP(K_ext(ng)*z_r(i,j,k))/ & & (K_NO3(ng)+Bio(i,k,iNO3_)) Bio1(i,k,iNO3_)=Bio(i,k,iNO3_) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)/ & & (1.0_r8+cff) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)+ & & Bio(i,k,iNO3_)*cff END DO END DO ! IF (Iteradj.ne.Iter) THEN ! ! Phytoplankton grazing by Zooplankton and mortality to Detritus ! (rate: PhyMR). ! cff1=dtdays*ZooGR(ng) cff2=dtdays*PhyMR(ng) cff3=K_phy(ng)*K_phy(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio(i,k,iZoop)*Bio(i,k,iPhyt)*cff1/ & & (cff3+Bio(i,k,iPhyt)*Bio(i,k,iPhyt)) Bio1(i,k,iPhyt)=Bio(i,k,iPhyt) Bio(i,k,iPhyt)=Bio(i,k,iPhyt)/ & & (1.0_r8+cff+cff2) Bio1(i,k,iZoop)=Bio(i,k,iZoop) Bio(i,k,iZoop)=Bio(i,k,iZoop)+ & & Bio(i,k,iPhyt)*cff*(1.0_r8-ZooGA(ng)) Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iPhyt)* & & (cff2+cff*(ZooGA(ng)-ZooEC(ng))) Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iPhyt)*cff*ZooEC(ng) END DO END DO ! ! Zooplankton excretion to nutrients and mortality to Detritus. ! cff1=1.0_r8/(1.0_r8+dtdays*(ZooMR(ng)+ZooMD(ng))) cff2=dtdays*ZooMR(ng) cff3=dtdays*ZooMD(ng) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iZoop)=Bio(i,k,iZoop)*cff1 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iZoop)*cff2 Bio(i,k,iSDet)=Bio(i,k,iSDet)+ & & Bio(i,k,iZoop)*cff3 END DO END DO ! ! Detritus breakdown to nutrients. ! cff1=dtdays*DetRR(ng) cff2=1.0_r8/(1.0_r8+cff1) DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,iSDet)=Bio(i,k,iSDet)*cff2 Bio(i,k,iNO3_)=Bio(i,k,iNO3_)+ & & Bio(i,k,iSDet)*cff1 END DO END DO ! !----------------------------------------------------------------------- ! Vertical sinking terms. !----------------------------------------------------------------------- ! ! Reconstruct vertical profile of selected biological constituents ! "Bio(:,:,isink)" in terms of a set of parabolic segments within each ! grid box. Then, compute semi-Lagrangian flux due to sinking. ! DO isink=1,Nsink ibio=idsink(isink) ! ! Copy concentration of biological particulates into scratch array ! "qc" (q-central, restrict it to be positive) which is hereafter ! interpreted as a set of grid-box averaged values for biogeochemical ! constituent concentration. ! DO k=1,N(ng) DO i=Istr,Iend qc(i,k)=Bio(i,k,ibio) END DO END DO ! DO k=N(ng)-1,1,-1 DO i=Istr,Iend FC(i,k)=(qc(i,k+1)-qc(i,k))*Hz_inv2(i,k) END DO END DO DO k=2,N(ng)-1 DO i=Istr,Iend dltR=Hz(i,j,k)*FC(i,k) dltL=Hz(i,j,k)*FC(i,k-1) cff=Hz(i,j,k-1)+2.0_r8*Hz(i,j,k)+Hz(i,j,k+1) cffR=cff*FC(i,k) cffL=cff*FC(i,k-1) ! ! Apply PPM monotonicity constraint to prevent oscillations within the ! grid box. ! IF ((dltR*dltL).le.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF ! ! Compute right and left side values (bR,bL) of parabolic segments ! within grid box Hz(k); (WR,WL) are measures of quadratic variations. ! ! NOTE: Although each parabolic segment is monotonic within its grid ! box, monotonicity of the whole profile is not guaranteed, ! because bL(k+1)-bR(k) may still have different sign than ! qc(i,k+1)-qc(i,k). This possibility is excluded, ! after bL and bR are reconciled using WENO procedure. ! cff=(dltR-dltL)*Hz_inv3(i,k) dltR=dltR-cff*Hz(i,j,k+1) dltL=dltL+cff*Hz(i,j,k-1) bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL WR(i,k)=(2.0_r8*dltR-dltL)**2 WL(i,k)=(dltR-2.0_r8*dltL)**2 END DO END DO cff=1.0E-14_r8 DO k=2,N(ng)-2 DO i=Istr,Iend dltL=MAX(cff,WL(i,k )) dltR=MAX(cff,WR(i,k+1)) bR(i,k)=(dltR*bR(i,k)+dltL*bL(i,k+1))/(dltR+dltL) bL(i,k+1)=bR(i,k) END DO END DO DO i=Istr,Iend FC(i,N(ng))=0.0_r8 ! NO-flux boundary condition #if defined LINEAR_CONTINUATION bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=2.0_r8*qc(i,N(ng))-bL(i,N(ng)) #elif defined NEUMANN bL(i,N(ng))=bR(i,N(ng)-1) bR(i,N(ng))=1.5*qc(i,N(ng))-0.5_r8*bL(i,N(ng)) #else bR(i,N(ng))=qc(i,N(ng)) ! default strictly monotonic bL(i,N(ng))=qc(i,N(ng)) ! conditions bR(i,N(ng)-1)=qc(i,N(ng)) #endif #if defined LINEAR_CONTINUATION bR(i,1)=bL(i,2) bL(i,1)=2.0_r8*qc(i,1)-bR(i,1) #elif defined NEUMANN bR(i,1)=bL(i,2) bL(i,1)=1.5_r8*qc(i,1)-0.5_r8*bR(i,1) #else bL(i,2)=qc(i,1) ! bottom grid boxes are bR(i,1)=qc(i,1) ! re-assumed to be bL(i,1)=qc(i,1) ! piecewise constant. #endif END DO ! ! Apply monotonicity constraint again, since the reconciled interfacial ! values may cause a non-monotonic behavior of the parabolic segments ! inside the grid box. ! DO k=1,N(ng) DO i=Istr,Iend dltR=bR(i,k)-qc(i,k) dltL=qc(i,k)-bL(i,k) cffR=2.0_r8*dltR cffL=2.0_r8*dltL IF ((dltR*dltL).lt.0.0_r8) THEN dltR=0.0_r8 dltL=0.0_r8 ELSE IF (ABS(dltR).gt.ABS(cffL)) THEN dltR=cffL ELSE IF (ABS(dltL).gt.ABS(cffR)) THEN dltL=cffR END IF bR(i,k)=qc(i,k)+dltR bL(i,k)=qc(i,k)-dltL END DO END DO ! ! After this moment reconstruction is considered complete. The next ! stage is to compute vertical advective fluxes, FC. It is expected ! that sinking may occurs relatively fast, the algorithm is designed ! to be free of CFL criterion, which is achieved by allowing ! integration bounds for semi-Lagrangian advective flux to use as ! many grid boxes in upstream direction as necessary. ! ! In the two code segments below, WL is the z-coordinate of the ! departure point for grid box interface z_w with the same indices; ! FC is the finite volume flux; ksource(:,k) is index of vertical ! grid box which contains the departure point (restricted by N(ng)). ! During the search: also add in content of whole grid boxes ! participating in FC. ! cff=dtdays*ABS(Wbio(isink)) DO k=1,N(ng) DO i=Istr,Iend FC(i,k-1)=0.0_r8 WL(i,k)=z_w(i,j,k-1)+cff WR(i,k)=Hz(i,j,k)*qc(i,k) ksource(i,k)=k END DO END DO DO k=1,N(ng) DO ks=k,N(ng)-1 DO i=Istr,Iend IF (WL(i,k).gt.z_w(i,j,ks)) THEN ksource(i,k)=ks+1 FC(i,k-1)=FC(i,k-1)+WR(i,ks) END IF END DO END DO END DO ! ! Finalize computation of flux: add fractional part. ! DO k=1,N(ng) DO i=Istr,Iend ks=ksource(i,k) cu=MIN(1.0_r8,(WL(i,k)-z_w(i,j,ks-1))*Hz_inv(i,ks)) FC(i,k-1)=FC(i,k-1)+ & & Hz(i,j,ks)*cu* & & (bL(i,ks)+ & & cu*(0.5_r8*(bR(i,ks)-bL(i,ks))- & & (1.5_r8-cu)* & & (bR(i,ks)+bL(i,ks)- & & 2.0_r8*qc(i,ks)))) END DO END DO DO k=1,N(ng) DO i=Istr,Iend Bio(i,k,ibio)=qc(i,k)+ & & (FC(i,k)-FC(i,k-1))*Hz_inv(i,k) END DO END DO END DO END IF END DO ! ! End of compute basic state arrays I. ! cff1=dtdays*Vm_NO3(ng) DO k=1,N(ng) DO i=Istr,Iend cff=Bio1(i,k,iPhyt)* & & cff1*EXP(K_ext(ng)*z_r(i,j,k))/ & & (K_NO3(ng)+Bio1(i,k,iNO3_)) !^ tl_Bio(i,k,iPhyt)=tl_Bio(i,k,iPhyt)+ & !^ & tl_Bio(i,k,iNO3_)*cff+ & !^ & Bio(i,k,iNO3_)*tl_cff !^ ad_Bio(i,k,iNO3_)=ad_Bio(i,k,iNO3_)+ & & ad_Bio(i,k,iPhyt)*cff ad_cff=ad_cff+Bio(i,k,iNO3_)*ad_Bio(i,k,iPhyt) !^ tl_Bio(i,k,iNO3_)=(tl_Bio(i,k,iNO3_)- & !^ & tl_cff*Bio(i,k,iNO3_))/ & !^ & (1.0_r8+cff) !^ adfac=ad_Bio(i,k,iNO3_)/(1.0_r8+cff) ad_cff=ad_cff-Bio(i,k,iNO3_)*adfac ad_Bio(i,k,iNO3_)=adfac !^ tl_cff=(tl_Bio(i,k,iPhyt)* & !^ & cff1*EXP(K_ext(ng)*z_r(i,j,k))- & !^ & tl_Bio(i,k,iNO3_)*cff)/ & !^ & (K_NO3(ng)+Bio1(i,k,iNO3_))+ & !^ & K_ext(ng)*tl_z_r(i,j,k)*cff !^ adfac=ad_cff/(K_NO3(ng)+Bio1(i,k,iNO3_)) ad_Bio(i,k,iPhyt)=ad_Bio(i,k,iPhyt)+ & & adfac*cff1*EXP(K_ext(ng)*z_r(i,j,k)) ad_Bio(i,k,iNO3_)=ad_Bio(i,k,iNO3_)-adfac*cff ad_z_r(i,j,k)=ad_z_r(i,j,k)+K_ext(ng)*ad_cff*cff ad_cff=0.0_r8 END DO END DO END DO ITER_LOOP ! ! Adjoint Correction for negativity. ! ! Extract biological variables from tracer arrays, place them into ! scratch arrays, and restrict their values to be positive definite. ! At input, all tracers (index nnew) from predictor step have ! transport units (m Tunits) since we do not have yet the new ! values for zeta and Hz. These are known after the 2D barotropic ! time-stepping. In this routine, this is not a problem because ! we only use index nstp in the right-hand-side equations. ! DO itrc=1,NBT ibio=idbio(itrc) DO k=1,N(ng) DO i=Istr,Iend Bio_old(i,k,ibio)=t(i,j,k,nstp,ibio) END DO END DO END DO ! DO k=1,N(ng) DO i=Istr,Iend cff1=MAX(0.0_r8,eps-Bio_old(i,k,iNO3_))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iPhyt))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iZoop))+ & & MAX(0.0_r8,eps-Bio_old(i,k,iSDet)) ! ! If correction needed, determine the largest pool to debit. ! IF (cff1.gt.0.0) THEN itrmx=idbio(1) cff=t(i,j,k,nstp,itrmx) DO ibio=idbio(2),idbio(NBT) IF (t(i,j,k,nstp,ibio).gt.cff) THEN itrmx=ibio cff=t(i,j,k,nstp,ibio) END IF END DO ! DO itrc=1,NBT ibio=idbio(itrc) !^ tl_Bio(i,k,ibio)=(0.5_r8- & !^ & SIGN(0.5_r8,eps-Bio_old(i,k,ibio)))* & !^ & tl_Bio_old(i,k,ibio)- & !^ & tl_cff1* & !^ & (SIGN(0.5_r8, REAL(itrmx-ibio,r8)**2)+ & !^ & SIGN(0.5_r8,-REAL(itrmx-ibio,r8)**2)) !^ ad_Bio_old(i,k,ibio)=ad_Bio_old(i,k,ibio)+ & & (0.5_r8- & & SIGN(0.5_r8, & & eps-Bio_old(i,k,ibio)))* & & ad_Bio(i,k,ibio) ad_cff1=ad_cff1- & & ad_Bio(i,k,ibio)* & & (SIGN(0.5_r8, REAL(itrmx-ibio,r8)**2)+ & & SIGN(0.5_r8,-REAL(itrmx-ibio,r8)**2)) ad_Bio(i,k,ibio)=0.0_r8 END DO ELSE DO itrc=1,NBT ibio=idbio(itrc) !^ tl_Bio(i,k,ibio)=tl_Bio_old(i,k,ibio) !^ ad_Bio_old(i,k,ibio)=ad_Bio_old(i,k,ibio)+ & & ad_Bio(i,k,ibio) ad_Bio(i,k,ibio)=0.0_r8 END DO END IF !^ tl_cff1=-(0.5_r8-SIGN(0.5_r8,Bio_old(i,k,iNO3_)-eps))* & !^ & tl_Bio_old(i,k,iNO3_)- & !^ & (0.5_r8-SIGN(0.5_r8,Bio_old(i,k,iPhyt)-eps))* & !^ & tl_Bio_old(i,k,iPhyt)- & !^ & (0.5_r8-SIGN(0.5_r8,Bio_old(i,k,iZoop)-eps))* & !^ & tl_Bio_old(i,k,iZoop)- & !^ & (0.5_r8-SIGN(0.5_r8,Bio_old(i,k,iSDet)-eps))* & !^ & tl_Bio_old(i,k,iSDet) !^ ad_Bio_old(i,k,iNO3_)=ad_Bio_old(i,k,iNO3_)- & & (0.5_r8- & & SIGN(0.5_r8, & & Bio_old(i,k,iNO3_)-eps))*ad_cff1 ad_Bio_old(i,k,iPhyt)=ad_Bio_old(i,k,iPhyt)- & & (0.5_r8- & & SIGN(0.5_r8, & & Bio_old(i,k,iPhyt)-eps))*ad_cff1 ad_Bio_old(i,k,iZoop)=ad_Bio_old(i,k,iZoop)- & & (0.5_r8- & & SIGN(0.5_r8, & & Bio_old(i,k,iZoop)-eps))*ad_cff1 ad_Bio_old(i,k,iSDet)=ad_Bio_old(i,k,iSDet)- & & (0.5_r8- & & SIGN(0.5_r8, & & Bio_old(i,k,iSDet)-eps))*ad_cff1 ad_cff1=0.0_r8 END DO END DO ! DO itrc=1,NBT ibio=idbio(itrc) DO k=1,N(ng) DO i=Istr,Iend !^ tl_Bio_old(i,k,ibio)=tl_t(i,j,k,nstp,ibio) !^ ad_t(i,j,k,nstp,ibio)=ad_t(i,j,k,nstp,ibio)+ & & ad_Bio_old(i,k,ibio) ad_Bio_old(i,k,ibio)=0.0_r8 END DO END DO END DO ! ! Adjoint inverse thickness to avoid repeated divisions. ! DO k=2,N(ng)-1 DO i=Istr,Iend !^ tl_Hz_inv3(i,k)=-Hz_inv3(i,k)*Hz_inv3(i,k)* & !^ & (tl_Hz(i,j,k-1)+tl_Hz(i,j,k)+ & !^ & tl_Hz(i,j,k+1)) !^ adfac=-Hz_inv3(i,k)*Hz_inv3(i,k)*ad_Hz_inv3(i,k) ad_Hz(i,j,k-1)=ad_Hz(i,j,k-1)+adfac ad_Hz(i,j,k )=ad_Hz(i,j,k )+adfac ad_Hz(i,j,k+1)=ad_Hz(i,j,k+1)+adfac ad_Hz_inv3(i,k)=0.0_r8 END DO END DO DO k=1,N(ng)-1 DO i=Istr,Iend !^ tl_Hz_inv2(i,k)=-Hz_inv2(i,k)*Hz_inv2(i,k)* & !^ & (tl_Hz(i,j,k)+tl_Hz(i,j,k+1)) !^ adfac=-Hz_inv2(i,k)*Hz_inv2(i,k)*ad_Hz_inv2(i,k) ad_Hz(i,j,k )=ad_Hz(i,j,k )+adfac ad_Hz(i,j,k+1)=ad_Hz(i,j,k+1)+adfac ad_Hz_inv2(i,k)=0.0_r8 END DO END DO DO k=1,N(ng) DO i=Istr,Iend !^ tl_Hz_inv(i,k)=-Hz_inv(i,k)*Hz_inv(i,k)*tl_Hz(i,j,k) !^ ad_Hz(i,j,k)=ad_Hz(i,j,k)- & & Hz_inv(i,k)*Hz_inv(i,k)*ad_Hz_inv(i,k) ad_Hz_inv(i,k)=0.0_r8 END DO END DO END DO J_LOOP ! ! Adjoint vertical sinking velocity vector. ! !^ tl_Wbio(1)=tl_wDet(ng) ! Small detritus !^ ad_wDet(ng)=ad_wDet(ng)+ad_Wbio(1) ad_Wbio(1)=0.0_r8 RETURN END SUBROUTINE ad_npzd_franks_tile END MODULE ad_biology_mod