Changeset 14009 for NEMO/branches/2020/dev_r2052_ENHANCE-09_rbourdal_massfluxconvection/src/ICE/icedyn_rdgrft.F90

Timestamp:

2020-12-02T15:42:07+01:00 (3 years ago)

Author:

gsamson

Message:

dev_r2052_ENHANCE-09_rbourdal_massfluxconvection update with trunk@r14008

Location:

NEMO/branches/2020/dev_r2052_ENHANCE-09_rbourdal_massfluxconvection

Files:

• . (modified) (1 prop)
• src/ICE/icedyn_rdgrft.F90 (modified) (7 diffs)

NEMO/branches/2020/dev_r2052_ENHANCE-09_rbourdal_massfluxconvection

@@ -8 +8 @@
 
 # SETTE
-^/utils/CI/sette_MPI3_LoopFusion@13943         sette
+^/utils/CI/sette_wave@13990         sette

@@ -8 +8 @@
 
 # SETTE
-^/utils/CI/sette_MPI3_LoopFusion@13943         sette
+^/utils/CI/sette_wave@13990         sette

NEMO/branches/2020/dev_r2052_ENHANCE-09_rbourdal_massfluxconvection/src/ICE/icedyn_rdgrft.F90

@@ -140 +140 @@
       INTEGER , DIMENSION(jpij) ::   iptidx        ! compute ridge/raft or not
       REAL(wp), DIMENSION(jpij) ::   zdivu, zdelt  ! 1D divu_i & delta_i
+      REAL(wp), DIMENSION(jpij) ::   zconv         ! 1D rdg_conv (if EAP rheology)
       !
       INTEGER, PARAMETER ::   jp_itermax = 20    
@@ -175 +176 @@
          ! just needed here
          CALL tab_2d_1d( npti, nptidx(1:npti), zdelt   (1:npti)      , delta_i )
+         CALL tab_2d_1d( npti, nptidx(1:npti), zconv   (1:npti)      , rdg_conv )
          ! needed here and in the iteration loop
          CALL tab_2d_1d( npti, nptidx(1:npti), zdivu   (1:npti)      , divu_i) ! zdivu is used as a work array here (no change in divu_i)
@@ -184 +186 @@
             ! closing_net = rate at which open water area is removed + ice area removed by ridging 
             !                                                        - ice area added in new ridges
-            closing_net(ji) = rn_csrdg * 0.5_wp * ( zdelt(ji) - ABS( zdivu(ji) ) ) - MIN( zdivu(ji), 0._wp )
+            IF( ln_rhg_EVP )  closing_net(ji) = rn_csrdg * 0.5_wp * ( zdelt(ji) - ABS( zdivu(ji) ) ) - MIN( zdivu(ji), 0._wp )
+            IF( ln_rhg_EAP )  closing_net(ji) = zconv(ji)
             !
             IF( zdivu(ji) < 0._wp )   closing_net(ji) = MAX( closing_net(ji), -zdivu(ji) )   ! make sure the closing rate is large enough
@@ -575 +578 @@
                oirft2(ji) = oa_i_2d(ji,jl1)   * afrft * hi_hrft 
 
-               IF ( ln_pnd_LEV ) THEN
+               IF ( ln_pnd_LEV .OR. ln_pnd_TOPO ) THEN
                   aprdg1     = a_ip_2d(ji,jl1) * afrdg
                   aprdg2(ji) = a_ip_2d(ji,jl1) * afrdg * hi_hrdg(ji,jl1)
@@ -612 +615 @@
                sv_i_2d(ji,jl1) = sv_i_2d(ji,jl1) - sirdg1    - sirft(ji)
                oa_i_2d(ji,jl1) = oa_i_2d(ji,jl1) - oirdg1    - oirft1
-               IF ( ln_pnd_LEV ) THEN
+               IF ( ln_pnd_LEV .OR. ln_pnd_TOPO ) THEN
                   a_ip_2d(ji,jl1) = a_ip_2d(ji,jl1) - aprdg1    - aprft1
                   v_ip_2d(ji,jl1) = v_ip_2d(ji,jl1) - vprdg(ji) - vprft(ji)
@@ -709 +712 @@
                   v_s_2d (ji,jl2) = v_s_2d (ji,jl2) + ( vsrdg (ji) * rn_fsnwrdg * fvol(ji)  +  &
                      &                                  vsrft (ji) * rn_fsnwrft * zswitch(ji) )
-                  IF ( ln_pnd_LEV ) THEN
+                  IF ( ln_pnd_LEV .OR. ln_pnd_TOPO ) THEN
                      v_ip_2d (ji,jl2) = v_ip_2d(ji,jl2) + (   vprdg (ji) * rn_fpndrdg * fvol   (ji)   &
                         &                                   + vprft (ji) * rn_fpndrft * zswitch(ji)   )
@@ -776 +779 @@
       !                              !--------------------------------------------------!
          strength(:,:) = rn_pstar * SUM( v_i(:,:,:), dim=3 ) * EXP( -rn_crhg * ( 1._wp - SUM( a_i(:,:,:), dim=3 ) ) )
-         ismooth = 1
+         ismooth = 1    ! original code
+!        ismooth = 0    ! try for EAP stability
          !                           !--------------------------------------------------!
       ELSE                           ! Zero strength                                    !

@@ -8 +8 @@
 
 # SETTE
-^/utils/CI/sette_MPI3_LoopFusion@13943         sette
+^/utils/CI/sette_wave@13990         sette