MODULE limthd_ent !!====================================================================== !! *** MODULE limthd_ent *** !! Redistribution of Enthalpy in the ice !! on the new vertical grid !! after vertical growth/decay !!====================================================================== !! History : LIM ! 2003-05 (M. Vancoppenolle) Original code in 1D !! ! 2005-07 (M. Vancoppenolle) 3D version !! ! 2006-11 (X. Fettweis) Vectorized !! 3.0 ! 2008-03 (M. Vancoppenolle) Energy conservation and clean code !! 3.4 ! 2011-02 (G. Madec) dynamical allocation !! - ! 2014-05 (C. Rousset) complete rewriting !!---------------------------------------------------------------------- #if defined key_lim3 !!---------------------------------------------------------------------- !! 'key_lim3' LIM3 sea-ice model !!---------------------------------------------------------------------- !! lim_thd_ent : ice redistribution of enthalpy !!---------------------------------------------------------------------- USE par_oce ! ocean parameters USE dom_oce ! domain variables USE domain ! USE phycst ! physical constants USE sbc_oce ! Surface boundary condition: ocean fields USE ice ! LIM variables USE thd_ice ! LIM thermodynamics USE limvar ! LIM variables USE in_out_manager ! I/O manager USE lib_mpp ! MPP library USE wrk_nemo ! work arrays USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) IMPLICIT NONE PRIVATE PUBLIC lim_thd_ent ! called by limthd and limthd_lac !!---------------------------------------------------------------------- !! NEMO/LIM3 4.0 , UCL - NEMO Consortium (2011) !! $Id: limthd_ent.F90 4990 2014-12-15 16:42:49Z timgraham $ !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) !!---------------------------------------------------------------------- CONTAINS SUBROUTINE lim_thd_ent( kideb, kiut, qnew ) !!------------------------------------------------------------------- !! *** ROUTINE lim_thd_ent *** !! !! ** Purpose : !! This routine computes new vertical grids in the ice, !! and consistently redistributes temperatures. !! Redistribution is made so as to ensure to energy conservation !! !! !! ** Method : linear conservative remapping !! !! ** Steps : 1) cumulative integrals of old enthalpies/thicknesses !! 2) linear remapping on the new layers !! !! ------------ cum0(0) ------------- cum1(0) !! NEW ------------- !! ------------ cum0(1) ==> ------------- !! ... ------------- !! ------------ ------------- !! ------------ cum0(nlay_i+2) ------------- cum1(nlay_i) !! !! !! References : Bitz & Lipscomb, JGR 99; Vancoppenolle et al., GRL, 2005 !!------------------------------------------------------------------- INTEGER , INTENT(in) :: kideb, kiut ! Start/End point on which the the computation is applied REAL(wp), INTENT(inout), DIMENSION(:,:) :: qnew ! new enthlapies (J.m-3, remapped) INTEGER :: ji ! dummy loop indices INTEGER :: jk0, jk1 ! old/new layer indices ! REAL(wp), POINTER, DIMENSION(:,:) :: zqh_cum0, zh_cum0 ! old cumulative enthlapies and layers interfaces REAL(wp), POINTER, DIMENSION(:,:) :: zqh_cum1, zh_cum1 ! new cumulative enthlapies and layers interfaces REAL(wp), POINTER, DIMENSION(:) :: zhnew ! new layers thicknesses !!------------------------------------------------------------------- CALL wrk_alloc( jpij, nlay_i+3, zqh_cum0, zh_cum0, kjstart = 0 ) CALL wrk_alloc( jpij, nlay_i+1, zqh_cum1, zh_cum1, kjstart = 0 ) CALL wrk_alloc( jpij, zhnew ) !-------------------------------------------------------------------------- ! 1) Cumulative integral of old enthalpy * thickness and layers interfaces !-------------------------------------------------------------------------- zqh_cum0(:,0:nlay_i+2) = 0._wp zh_cum0 (:,0:nlay_i+2) = 0._wp DO jk0 = 1, nlay_i+2 DO ji = kideb, kiut zqh_cum0(ji,jk0) = zqh_cum0(ji,jk0-1) + qh_i_old(ji,jk0-1) zh_cum0 (ji,jk0) = zh_cum0 (ji,jk0-1) + h_i_old (ji,jk0-1) ENDDO ENDDO !------------------------------------ ! 2) Interpolation on the new layers !------------------------------------ ! new layer thickesses DO ji = kideb, kiut zhnew(ji) = SUM( h_i_old(ji,0:nlay_i+1) ) * r1_nlay_i ENDDO ! new layers interfaces zh_cum1(:,0:nlay_i) = 0._wp DO jk1 = 1, nlay_i DO ji = kideb, kiut zh_cum1(ji,jk1) = zh_cum1(ji,jk1-1) + zhnew(ji) ENDDO ENDDO zqh_cum1(:,0:nlay_i) = 0._wp ! new cumulative q*h => linear interpolation DO jk0 = 1, nlay_i+1 DO jk1 = 1, nlay_i-1 DO ji = kideb, kiut IF( zh_cum1(ji,jk1) <= zh_cum0(ji,jk0) .AND. zh_cum1(ji,jk1) > zh_cum0(ji,jk0-1) ) THEN zqh_cum1(ji,jk1) = ( zqh_cum0(ji,jk0-1) * ( zh_cum0(ji,jk0) - zh_cum1(ji,jk1 ) ) + & & zqh_cum0(ji,jk0 ) * ( zh_cum1(ji,jk1) - zh_cum0(ji,jk0-1) ) ) & & / ( zh_cum0(ji,jk0) - zh_cum0(ji,jk0-1) ) ENDIF ENDDO ENDDO ENDDO ! to ensure that total heat content is strictly conserved, set: zqh_cum1(:,nlay_i) = zqh_cum0(:,nlay_i+2) ! new enthalpies DO jk1 = 1, nlay_i DO ji = kideb, kiut rswitch = MAX( 0._wp , SIGN( 1._wp , zhnew(ji) - epsi20 ) ) qnew(ji,jk1) = rswitch * ( zqh_cum1(ji,jk1) - zqh_cum1(ji,jk1-1) ) / MAX( zhnew(ji), epsi20 ) ENDDO ENDDO ! --- diag error on heat remapping --- ! ! comment: if input h_i_old and qh_i_old are already multiplied by a_i (as in limthd_lac), ! then we should not (* a_i) again but not important since this is just to check that remap error is ~0 DO ji = kideb, kiut hfx_err_rem_1d(ji) = hfx_err_rem_1d(ji) + a_i_1d(ji) * r1_rdtice * & & ( SUM( qnew(ji,1:nlay_i) ) * zhnew(ji) - SUM( qh_i_old(ji,0:nlay_i+1) ) ) END DO ! CALL wrk_dealloc( jpij, nlay_i+3, zqh_cum0, zh_cum0, kjstart = 0 ) CALL wrk_dealloc( jpij, nlay_i+1, zqh_cum1, zh_cum1, kjstart = 0 ) CALL wrk_dealloc( jpij, zhnew ) ! END SUBROUTINE lim_thd_ent #else !!---------------------------------------------------------------------- !! Default option NO LIM3 sea-ice model !!---------------------------------------------------------------------- CONTAINS SUBROUTINE lim_thd_ent ! Empty routine END SUBROUTINE lim_thd_ent #endif !!====================================================================== END MODULE limthd_ent