[8531] | 1 | MODULE icethd_zdf |
---|
| 2 | !!====================================================================== |
---|
| 3 | !! *** MODULE icethd_zdf *** |
---|
[8534] | 4 | !! sea-ice: vertical heat diffusion in sea ice (computation of temperatures) |
---|
[8531] | 5 | !!====================================================================== |
---|
| 6 | !! History : LIM ! 02-2003 (M. Vancoppenolle) original 1D code |
---|
| 7 | !! ! 06-2005 (M. Vancoppenolle) 3d version |
---|
| 8 | !! ! 11-2006 (X Fettweis) Vectorization by Xavier |
---|
| 9 | !! ! 04-2007 (M. Vancoppenolle) Energy conservation |
---|
| 10 | !! 4.0 ! 2011-02 (G. Madec) dynamical allocation |
---|
| 11 | !! - ! 2012-05 (C. Rousset) add penetration solar flux |
---|
| 12 | !!---------------------------------------------------------------------- |
---|
| 13 | #if defined key_lim3 |
---|
| 14 | !!---------------------------------------------------------------------- |
---|
[8534] | 15 | !! 'key_lim3' ESIM sea-ice model |
---|
[8531] | 16 | !!---------------------------------------------------------------------- |
---|
[8534] | 17 | USE dom_oce ! ocean space and time domain |
---|
[8531] | 18 | USE phycst ! physical constants (ocean directory) |
---|
| 19 | USE ice ! sea-ice: variables |
---|
[8534] | 20 | USE ice1D ! sea-ice: thermodynamics variables |
---|
[8531] | 21 | ! |
---|
| 22 | USE in_out_manager ! I/O manager |
---|
| 23 | USE lib_mpp ! MPP library |
---|
[8534] | 24 | USE lib_fortran ! fortran utilities (glob_sum + no signed zero) |
---|
[8531] | 25 | |
---|
| 26 | IMPLICIT NONE |
---|
| 27 | PRIVATE |
---|
| 28 | |
---|
[8534] | 29 | PUBLIC ice_thd_zdf ! called by icethd |
---|
| 30 | PUBLIC ice_thd_zdf_init ! called by icestp |
---|
[8531] | 31 | |
---|
| 32 | !!** namelist (namthd_zdf) ** |
---|
[8585] | 33 | LOGICAL :: ln_zdf_BL99 ! Heat diffusion follows Bitz and Lipscomb (1999) |
---|
[8531] | 34 | LOGICAL :: ln_cndi_U64 ! thermal conductivity: Untersteiner (1964) |
---|
| 35 | LOGICAL :: ln_cndi_P07 ! thermal conductivity: Pringle et al (2007) |
---|
| 36 | REAL(wp) :: rn_cnd_s ! thermal conductivity of the snow [W/m/K] |
---|
| 37 | REAL(wp) :: rn_kappa_i ! coef. for the extinction of radiation Grenfell et al. (2006) [1/m] |
---|
| 38 | LOGICAL :: ln_dqns_i ! change non-solar surface flux with changing surface temperature (T) or not (F) |
---|
| 39 | |
---|
| 40 | !!---------------------------------------------------------------------- |
---|
| 41 | !! NEMO/ICE 4.0 , NEMO Consortium (2017) |
---|
| 42 | !! $Id: icethd_zdf.F90 8420 2017-08-08 12:18:46Z clem $ |
---|
| 43 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
---|
| 44 | !!---------------------------------------------------------------------- |
---|
| 45 | CONTAINS |
---|
| 46 | |
---|
| 47 | SUBROUTINE ice_thd_zdf |
---|
[8534] | 48 | !!------------------------------------------------------------------- |
---|
[8531] | 49 | !! *** ROUTINE ice_thd_zdf *** |
---|
| 50 | !! ** Purpose : |
---|
| 51 | !! This routine determines the time evolution of snow and sea-ice |
---|
| 52 | !! temperature profiles. |
---|
| 53 | !! ** Method : |
---|
| 54 | !! This is done by solving the heat equation diffusion with |
---|
| 55 | !! a Neumann boundary condition at the surface and a Dirichlet one |
---|
| 56 | !! at the bottom. Solar radiation is partially absorbed into the ice. |
---|
| 57 | !! The specific heat and thermal conductivities depend on ice salinity |
---|
| 58 | !! and temperature to take into account brine pocket melting. The |
---|
| 59 | !! numerical |
---|
| 60 | !! scheme is an iterative Crank-Nicolson on a non-uniform multilayer grid |
---|
| 61 | !! in the ice and snow system. |
---|
| 62 | !! |
---|
| 63 | !! The successive steps of this routine are |
---|
[8534] | 64 | !! 1. initialization of ice-snow layers thicknesses |
---|
| 65 | !! 2. Internal absorbed and transmitted radiation |
---|
| 66 | !! Then iterative procedure begins |
---|
| 67 | !! 3. Thermal conductivity |
---|
[8531] | 68 | !! 4. Kappa factors |
---|
| 69 | !! 5. specific heat in the ice |
---|
| 70 | !! 6. eta factors |
---|
| 71 | !! 7. surface flux computation |
---|
| 72 | !! 8. tridiagonal system terms |
---|
| 73 | !! 9. solving the tridiagonal system with Gauss elimination |
---|
| 74 | !! Iterative procedure ends according to a criterion on evolution |
---|
| 75 | !! of temperature |
---|
[8534] | 76 | !! 10. Fluxes at the interfaces |
---|
[8531] | 77 | !! |
---|
| 78 | !! ** Inputs / Ouputs : (global commons) |
---|
| 79 | !! surface temperature : t_su_1d |
---|
| 80 | !! ice/snow temperatures : t_i_1d, t_s_1d |
---|
[8564] | 81 | !! ice salinities : sz_i_1d |
---|
[8531] | 82 | !! number of layers in the ice/snow: nlay_i, nlay_s |
---|
[8563] | 83 | !! total ice/snow thickness : h_i_1d, h_s_1d |
---|
[8534] | 84 | !!------------------------------------------------------------------- |
---|
[8531] | 85 | INTEGER :: ji, jk ! spatial loop index |
---|
[8562] | 86 | INTEGER :: jm ! current reference number of equation |
---|
| 87 | INTEGER :: jm_mint, jm_maxt |
---|
[8531] | 88 | INTEGER :: iconv ! number of iterations in iterative procedure |
---|
| 89 | INTEGER :: iconv_max = 50 ! max number of iterations in iterative procedure |
---|
| 90 | |
---|
[8562] | 91 | INTEGER, DIMENSION(jpij) :: jm_min ! reference number of top equation |
---|
| 92 | INTEGER, DIMENSION(jpij) :: jm_max ! reference number of bottom equation |
---|
[8531] | 93 | |
---|
| 94 | REAL(wp) :: zg1s = 2._wp ! for the tridiagonal system |
---|
| 95 | REAL(wp) :: zg1 = 2._wp ! |
---|
| 96 | REAL(wp) :: zgamma = 18009._wp ! for specific heat |
---|
| 97 | REAL(wp) :: zbeta = 0.117_wp ! for thermal conductivity (could be 0.13) |
---|
| 98 | REAL(wp) :: zraext_s = 10._wp ! extinction coefficient of radiation in the snow |
---|
| 99 | REAL(wp) :: zkimin = 0.10_wp ! minimum ice thermal conductivity |
---|
| 100 | REAL(wp) :: ztsu_err = 1.e-5_wp ! range around which t_su is considered at 0C |
---|
| 101 | REAL(wp) :: zdti_bnd = 1.e-4_wp ! maximal authorized error on temperature |
---|
| 102 | REAL(wp) :: ztmelt_i ! ice melting temperature |
---|
| 103 | REAL(wp) :: z1_hsu |
---|
| 104 | REAL(wp) :: zdti_max ! current maximal error on temperature |
---|
| 105 | REAL(wp) :: zcpi ! Ice specific heat |
---|
| 106 | REAL(wp) :: zhfx_err, zdq ! diag errors on heat |
---|
| 107 | REAL(wp) :: zfac ! dummy factor |
---|
| 108 | |
---|
| 109 | REAL(wp), DIMENSION(jpij) :: isnow ! switch for presence (1) or absence (0) of snow |
---|
| 110 | REAL(wp), DIMENSION(jpij) :: ztsub ! surface temperature at previous iteration |
---|
| 111 | REAL(wp), DIMENSION(jpij) :: zh_i, z1_h_i ! ice layer thickness |
---|
| 112 | REAL(wp), DIMENSION(jpij) :: zh_s, z1_h_s ! snow layer thickness |
---|
| 113 | REAL(wp), DIMENSION(jpij) :: zfsw ! solar radiation absorbed at the surface |
---|
| 114 | REAL(wp), DIMENSION(jpij) :: zqns_ice_b ! solar radiation absorbed at the surface |
---|
[8562] | 115 | REAL(wp), DIMENSION(jpij) :: zfnet ! surface flux function |
---|
[8531] | 116 | REAL(wp), DIMENSION(jpij) :: zdqns_ice_b ! derivative of the surface flux function |
---|
| 117 | REAL(wp), DIMENSION(jpij) :: zftrice ! solar radiation transmitted through the ice |
---|
| 118 | |
---|
| 119 | REAL(wp), DIMENSION(jpij,nlay_i) :: ztiold ! Old temperature in the ice |
---|
| 120 | REAL(wp), DIMENSION(jpij,nlay_s) :: ztsold ! Old temperature in the snow |
---|
| 121 | REAL(wp), DIMENSION(jpij,nlay_i) :: ztib ! Temporary temperature in the ice to check the convergence |
---|
| 122 | REAL(wp), DIMENSION(jpij,nlay_s) :: ztsb ! Temporary temperature in the snow to check the convergence |
---|
| 123 | REAL(wp), DIMENSION(jpij,0:nlay_i) :: ztcond_i ! Ice thermal conductivity |
---|
| 124 | REAL(wp), DIMENSION(jpij,0:nlay_i) :: zradtr_i ! Radiation transmitted through the ice |
---|
| 125 | REAL(wp), DIMENSION(jpij,0:nlay_i) :: zradab_i ! Radiation absorbed in the ice |
---|
| 126 | REAL(wp), DIMENSION(jpij,0:nlay_i) :: zkappa_i ! Kappa factor in the ice |
---|
| 127 | REAL(wp), DIMENSION(jpij,0:nlay_i) :: zeta_i ! Eta factor in the ice |
---|
| 128 | REAL(wp), DIMENSION(jpij,0:nlay_s) :: zradtr_s ! Radiation transmited through the snow |
---|
| 129 | REAL(wp), DIMENSION(jpij,0:nlay_s) :: zradab_s ! Radiation absorbed in the snow |
---|
| 130 | REAL(wp), DIMENSION(jpij,0:nlay_s) :: zkappa_s ! Kappa factor in the snow |
---|
| 131 | REAL(wp), DIMENSION(jpij,0:nlay_s) :: zeta_s ! Eta factor in the snow |
---|
| 132 | REAL(wp), DIMENSION(jpij,nlay_i+3) :: zindterm ! 'Ind'ependent term |
---|
| 133 | REAL(wp), DIMENSION(jpij,nlay_i+3) :: zindtbis ! Temporary 'ind'ependent term |
---|
| 134 | REAL(wp), DIMENSION(jpij,nlay_i+3) :: zdiagbis ! Temporary 'dia'gonal term |
---|
| 135 | REAL(wp), DIMENSION(jpij,nlay_i+3,3) :: ztrid ! Tridiagonal system terms |
---|
| 136 | REAL(wp), DIMENSION(jpij) :: zq_ini ! diag errors on heat |
---|
| 137 | REAL(wp), DIMENSION(jpij) :: zghe ! G(he), th. conduct enhancement factor, mono-cat |
---|
| 138 | |
---|
| 139 | ! Mono-category |
---|
| 140 | REAL(wp) :: zepsilon ! determines thres. above which computation of G(h) is done |
---|
| 141 | REAL(wp) :: zhe ! dummy factor |
---|
| 142 | REAL(wp) :: zcnd_i ! mean sea ice thermal conductivity |
---|
| 143 | !!------------------------------------------------------------------ |
---|
| 144 | |
---|
| 145 | ! --- diag error on heat diffusion - PART 1 --- ! |
---|
[8565] | 146 | DO ji = 1, npti |
---|
[8563] | 147 | zq_ini(ji) = ( SUM( e_i_1d(ji,1:nlay_i) ) * h_i_1d(ji) * r1_nlay_i + & |
---|
| 148 | & SUM( e_s_1d(ji,1:nlay_s) ) * h_s_1d(ji) * r1_nlay_s ) |
---|
[8531] | 149 | END DO |
---|
| 150 | |
---|
[8534] | 151 | !------------------ |
---|
| 152 | ! 1) Initialization |
---|
| 153 | !------------------ |
---|
[8565] | 154 | DO ji = 1, npti |
---|
[8563] | 155 | isnow(ji)= 1._wp - MAX( 0._wp , SIGN(1._wp, - h_s_1d(ji) ) ) ! is there snow or not |
---|
[8531] | 156 | ! layer thickness |
---|
[8563] | 157 | zh_i(ji) = h_i_1d(ji) * r1_nlay_i |
---|
| 158 | zh_s(ji) = h_s_1d(ji) * r1_nlay_s |
---|
[8531] | 159 | END DO |
---|
| 160 | ! |
---|
[8565] | 161 | WHERE( zh_i(1:npti) >= epsi10 ) ; z1_h_i(1:npti) = 1._wp / zh_i(1:npti) |
---|
| 162 | ELSEWHERE ; z1_h_i(1:npti) = 0._wp |
---|
[8531] | 163 | END WHERE |
---|
| 164 | |
---|
[8565] | 165 | WHERE( zh_s(1:npti) >= epsi10 ) ; z1_h_s(1:npti) = 1._wp / zh_s(1:npti) |
---|
| 166 | ELSEWHERE ; z1_h_s(1:npti) = 0._wp |
---|
[8531] | 167 | END WHERE |
---|
| 168 | ! |
---|
| 169 | ! temperatures |
---|
[8565] | 170 | ztsub (1:npti) = t_su_1d(1:npti) ! temperature at the previous iteration |
---|
| 171 | ztsold (1:npti,:) = t_s_1d(1:npti,:) ! Old snow temperature |
---|
| 172 | ztiold (1:npti,:) = t_i_1d(1:npti,:) ! Old ice temperature |
---|
| 173 | t_su_1d(1:npti) = MIN( t_su_1d(1:npti), rt0 - ztsu_err ) ! necessary |
---|
[8531] | 174 | ! |
---|
[8534] | 175 | !------------- |
---|
| 176 | ! 2) Radiation |
---|
| 177 | !------------- |
---|
[8531] | 178 | z1_hsu = 1._wp / 0.1_wp ! threshold for the computation of i0 |
---|
[8565] | 179 | DO ji = 1, npti |
---|
[8534] | 180 | ! --- Computation of i0 --- ! |
---|
[8531] | 181 | ! i0 describes the fraction of solar radiation which does not contribute |
---|
| 182 | ! to the surface energy budget but rather penetrates inside the ice. |
---|
| 183 | ! We assume that no radiation is transmitted through the snow |
---|
| 184 | ! If there is no no snow |
---|
| 185 | ! zfsw = (1-i0).qsr_ice is absorbed at the surface |
---|
| 186 | ! zftrice = io.qsr_ice is below the surface |
---|
| 187 | ! ftr_ice = io.qsr_ice.exp(-k(h_i)) transmitted below the ice |
---|
| 188 | ! fr1_i0_1d = i0 for a thin ice cover, fr1_i0_2d = i0 for a thick ice cover |
---|
[8563] | 189 | zfac = MAX( 0._wp , 1._wp - ( h_i_1d(ji) * z1_hsu ) ) |
---|
[8531] | 190 | i0(ji) = ( 1._wp - isnow(ji) ) * ( fr1_i0_1d(ji) + zfac * fr2_i0_1d(ji) ) |
---|
| 191 | |
---|
[8534] | 192 | ! --- Solar radiation absorbed / transmitted at the surface --- ! |
---|
| 193 | ! Derivative of the non solar flux |
---|
[8531] | 194 | zfsw (ji) = qsr_ice_1d(ji) * ( 1 - i0(ji) ) ! Shortwave radiation absorbed at surface |
---|
| 195 | zftrice(ji) = qsr_ice_1d(ji) * i0(ji) ! Solar radiation transmitted below the surface layer |
---|
| 196 | zdqns_ice_b(ji) = dqns_ice_1d(ji) ! derivative of incoming nonsolar flux |
---|
| 197 | zqns_ice_b (ji) = qns_ice_1d(ji) ! store previous qns_ice_1d value |
---|
| 198 | END DO |
---|
| 199 | |
---|
[8534] | 200 | ! --- Transmission/absorption of solar radiation in the ice --- ! |
---|
[8565] | 201 | zradtr_s(1:npti,0) = zftrice(1:npti) |
---|
[8531] | 202 | DO jk = 1, nlay_s |
---|
[8565] | 203 | DO ji = 1, npti |
---|
[8531] | 204 | ! ! radiation transmitted below the layer-th snow layer |
---|
| 205 | zradtr_s(ji,jk) = zradtr_s(ji,0) * EXP( - zraext_s * zh_s(ji) * REAL(jk) ) |
---|
| 206 | ! ! radiation absorbed by the layer-th snow layer |
---|
| 207 | zradab_s(ji,jk) = zradtr_s(ji,jk-1) - zradtr_s(ji,jk) |
---|
| 208 | END DO |
---|
| 209 | END DO |
---|
| 210 | |
---|
[8565] | 211 | zradtr_i(1:npti,0) = zradtr_s(1:npti,nlay_s) * isnow(1:npti) + zftrice(1:npti) * ( 1._wp - isnow(1:npti) ) |
---|
[8531] | 212 | DO jk = 1, nlay_i |
---|
[8565] | 213 | DO ji = 1, npti |
---|
[8531] | 214 | ! ! radiation transmitted below the layer-th ice layer |
---|
| 215 | zradtr_i(ji,jk) = zradtr_i(ji,0) * EXP( - rn_kappa_i * zh_i(ji) * REAL(jk) ) |
---|
| 216 | ! ! radiation absorbed by the layer-th ice layer |
---|
| 217 | zradab_i(ji,jk) = zradtr_i(ji,jk-1) - zradtr_i(ji,jk) |
---|
| 218 | END DO |
---|
| 219 | END DO |
---|
| 220 | |
---|
[8565] | 221 | ftr_ice_1d(1:npti) = zradtr_i(1:npti,nlay_i) ! record radiation transmitted below the ice |
---|
[8531] | 222 | ! |
---|
| 223 | iconv = 0 ! number of iterations |
---|
| 224 | zdti_max = 1000._wp ! maximal value of error on all points |
---|
[8562] | 225 | ! !============================! |
---|
[8534] | 226 | DO WHILE ( zdti_max > zdti_bnd .AND. iconv < iconv_max ) ! Iterative procedure begins ! |
---|
[8562] | 227 | ! !============================! |
---|
[8531] | 228 | iconv = iconv + 1 |
---|
| 229 | ! |
---|
[8565] | 230 | ztib(1:npti,:) = t_i_1d(1:npti,:) |
---|
| 231 | ztsb(1:npti,:) = t_s_1d(1:npti,:) |
---|
[8531] | 232 | ! |
---|
[8534] | 233 | !-------------------------------- |
---|
| 234 | ! 3) Sea ice thermal conductivity |
---|
| 235 | !-------------------------------- |
---|
[8531] | 236 | IF( ln_cndi_U64 ) THEN !-- Untersteiner (1964) formula: k = k0 + beta.S/T |
---|
| 237 | ! |
---|
[8565] | 238 | DO ji = 1, npti |
---|
[8564] | 239 | ztcond_i(ji,0) = rcdic + zbeta * sz_i_1d(ji,1) / MIN( -epsi10, t_i_1d(ji,1) - rt0 ) |
---|
| 240 | ztcond_i(ji,nlay_i) = rcdic + zbeta * sz_i_1d(ji,nlay_i) / MIN( -epsi10, t_bo_1d(ji) - rt0 ) |
---|
[8531] | 241 | END DO |
---|
| 242 | DO jk = 1, nlay_i-1 |
---|
[8565] | 243 | DO ji = 1, npti |
---|
[8564] | 244 | ztcond_i(ji,jk) = rcdic + zbeta * 0.5_wp * ( sz_i_1d(ji,jk) + sz_i_1d(ji,jk+1) ) / & |
---|
[8531] | 245 | & MIN( -epsi10, 0.5_wp * (t_i_1d(ji,jk) + t_i_1d(ji,jk+1)) - rt0 ) |
---|
| 246 | END DO |
---|
| 247 | END DO |
---|
| 248 | ! |
---|
| 249 | ELSEIF( ln_cndi_P07 ) THEN !-- Pringle et al formula: k = k0 + beta1.S/T - beta2.T |
---|
| 250 | ! |
---|
[8565] | 251 | DO ji = 1, npti |
---|
[8564] | 252 | ztcond_i(ji,0) = rcdic + 0.09_wp * sz_i_1d(ji,1) / MIN( -epsi10, t_i_1d(ji,1) - rt0 ) & |
---|
[8531] | 253 | & - 0.011_wp * ( t_i_1d(ji,1) - rt0 ) |
---|
[8564] | 254 | ztcond_i(ji,nlay_i) = rcdic + 0.09_wp * sz_i_1d(ji,nlay_i) / MIN( -epsi10, t_bo_1d(ji) - rt0 ) & |
---|
[8531] | 255 | & - 0.011_wp * ( t_bo_1d(ji) - rt0 ) |
---|
| 256 | END DO |
---|
| 257 | DO jk = 1, nlay_i-1 |
---|
[8565] | 258 | DO ji = 1, npti |
---|
[8564] | 259 | ztcond_i(ji,jk) = rcdic + 0.09_wp * 0.5_wp * ( sz_i_1d(ji,jk) + sz_i_1d(ji,jk+1) ) / & |
---|
[8531] | 260 | & MIN( -epsi10, 0.5_wp * (t_i_1d(ji,jk) + t_i_1d(ji,jk+1)) - rt0 ) & |
---|
| 261 | & - 0.011_wp * ( 0.5_wp * (t_i_1d(ji,jk) + t_i_1d(ji,jk+1)) - rt0 ) |
---|
| 262 | END DO |
---|
| 263 | END DO |
---|
| 264 | ! |
---|
| 265 | ENDIF |
---|
[8565] | 266 | ztcond_i(1:npti,:) = MAX( zkimin, ztcond_i(1:npti,:) ) |
---|
[8531] | 267 | ! |
---|
[8534] | 268 | !--- G(he) : enhancement of thermal conductivity in mono-category case |
---|
[8531] | 269 | ! Computation of effective thermal conductivity G(h) |
---|
| 270 | ! Used in mono-category case only to simulate an ITD implicitly |
---|
| 271 | ! Fichefet and Morales Maqueda, JGR 1997 |
---|
[8565] | 272 | zghe(1:npti) = 1._wp |
---|
[8562] | 273 | ! |
---|
[8531] | 274 | SELECT CASE ( nn_monocat ) |
---|
| 275 | |
---|
| 276 | CASE ( 1 , 3 ) |
---|
| 277 | |
---|
| 278 | zepsilon = 0.1_wp |
---|
[8565] | 279 | DO ji = 1, npti |
---|
[8562] | 280 | zcnd_i = SUM( ztcond_i(ji,:) ) / REAL( nlay_i+1, wp ) ! Mean sea ice thermal conductivity |
---|
[8563] | 281 | zhe = ( rn_cnd_s * h_i_1d(ji) + zcnd_i * h_s_1d(ji) ) / ( rn_cnd_s + zcnd_i ) ! Effective thickness he (zhe) |
---|
[8531] | 282 | IF( zhe >= zepsilon * 0.5_wp * EXP(1._wp) ) THEN |
---|
[8562] | 283 | zghe(ji) = MIN( 2._wp, 0.5_wp * ( 1._wp + LOG( 2._wp * zhe / zepsilon ) ) ) ! G(he) |
---|
[8531] | 284 | ENDIF |
---|
| 285 | END DO |
---|
| 286 | |
---|
| 287 | END SELECT |
---|
| 288 | ! |
---|
[8534] | 289 | !----------------- |
---|
| 290 | ! 4) kappa factors |
---|
| 291 | !----------------- |
---|
[8531] | 292 | !--- Snow |
---|
| 293 | DO jk = 0, nlay_s-1 |
---|
[8565] | 294 | DO ji = 1, npti |
---|
[8562] | 295 | zkappa_s(ji,jk) = zghe(ji) * rn_cnd_s * z1_h_s(ji) |
---|
[8531] | 296 | END DO |
---|
| 297 | END DO |
---|
[8565] | 298 | DO ji = 1, npti ! Snow-ice interface |
---|
[8531] | 299 | zfac = 0.5_wp * ( ztcond_i(ji,0) * zh_s(ji) + rn_cnd_s * zh_i(ji) ) |
---|
| 300 | IF( zfac > epsi10 ) THEN |
---|
| 301 | zkappa_s(ji,nlay_s) = zghe(ji) * rn_cnd_s * ztcond_i(ji,0) / zfac |
---|
| 302 | ELSE |
---|
| 303 | zkappa_s(ji,nlay_s) = 0._wp |
---|
| 304 | ENDIF |
---|
| 305 | END DO |
---|
| 306 | |
---|
| 307 | !--- Ice |
---|
| 308 | DO jk = 0, nlay_i |
---|
[8565] | 309 | DO ji = 1, npti |
---|
[8531] | 310 | zkappa_i(ji,jk) = zghe(ji) * ztcond_i(ji,jk) * z1_h_i(ji) |
---|
| 311 | END DO |
---|
| 312 | END DO |
---|
[8565] | 313 | DO ji = 1, npti ! Snow-ice interface |
---|
[8562] | 314 | zkappa_i(ji,0) = zkappa_s(ji,nlay_s) * isnow(ji) + zkappa_i(ji,0) * ( 1._wp - isnow(ji) ) |
---|
[8531] | 315 | END DO |
---|
| 316 | ! |
---|
[8534] | 317 | !-------------------------------------- |
---|
| 318 | ! 5) Sea ice specific heat, eta factors |
---|
| 319 | !-------------------------------------- |
---|
[8531] | 320 | DO jk = 1, nlay_i |
---|
[8565] | 321 | DO ji = 1, npti |
---|
[8564] | 322 | zcpi = cpic + zgamma * sz_i_1d(ji,jk) / MAX( ( t_i_1d(ji,jk) - rt0 ) * ( ztiold(ji,jk) - rt0 ), epsi10 ) |
---|
[8531] | 323 | zeta_i(ji,jk) = rdt_ice * r1_rhoic * z1_h_i(ji) / MAX( epsi10, zcpi ) |
---|
| 324 | END DO |
---|
| 325 | END DO |
---|
| 326 | |
---|
| 327 | DO jk = 1, nlay_s |
---|
[8565] | 328 | DO ji = 1, npti |
---|
[8562] | 329 | zeta_s(ji,jk) = rdt_ice * r1_rhosn * r1_cpic * z1_h_s(ji) |
---|
[8531] | 330 | END DO |
---|
| 331 | END DO |
---|
| 332 | ! |
---|
[8534] | 333 | !---------------------------- |
---|
| 334 | ! 6) surface flux computation |
---|
| 335 | !---------------------------- |
---|
[8531] | 336 | IF ( ln_dqns_i ) THEN |
---|
[8565] | 337 | DO ji = 1, npti |
---|
[8531] | 338 | ! update of the non solar flux according to the update in T_su |
---|
| 339 | qns_ice_1d(ji) = qns_ice_1d(ji) + dqns_ice_1d(ji) * ( t_su_1d(ji) - ztsub(ji) ) |
---|
| 340 | END DO |
---|
| 341 | ENDIF |
---|
| 342 | |
---|
[8565] | 343 | DO ji = 1, npti |
---|
[8562] | 344 | zfnet(ji) = zfsw(ji) + qns_ice_1d(ji) ! incoming = net absorbed solar radiation + non solar total flux (LWup, LWdw, SH, LH) |
---|
[8531] | 345 | END DO |
---|
| 346 | ! |
---|
[8534] | 347 | !---------------------------- |
---|
| 348 | ! 7) tridiagonal system terms |
---|
| 349 | !---------------------------- |
---|
[8531] | 350 | !!layer denotes the number of the layer in the snow or in the ice |
---|
[8562] | 351 | !!jm denotes the reference number of the equation in the tridiagonal |
---|
[8531] | 352 | !!system, terms of tridiagonal system are indexed as following : |
---|
| 353 | !!1 is subdiagonal term, 2 is diagonal and 3 is superdiagonal one |
---|
| 354 | |
---|
| 355 | !!ice interior terms (top equation has the same form as the others) |
---|
[8565] | 356 | ztrid (1:npti,:,:) = 0._wp |
---|
| 357 | zindterm(1:npti,:) = 0._wp |
---|
| 358 | zindtbis(1:npti,:) = 0._wp |
---|
| 359 | zdiagbis(1:npti,:) = 0._wp |
---|
[8531] | 360 | |
---|
[8562] | 361 | DO jm = nlay_s + 2, nlay_s + nlay_i |
---|
[8565] | 362 | DO ji = 1, npti |
---|
[8562] | 363 | jk = jm - nlay_s - 1 |
---|
| 364 | ztrid(ji,jm,1) = - zeta_i(ji,jk) * zkappa_i(ji,jk-1) |
---|
| 365 | ztrid(ji,jm,2) = 1.0 + zeta_i(ji,jk) * ( zkappa_i(ji,jk-1) + zkappa_i(ji,jk) ) |
---|
| 366 | ztrid(ji,jm,3) = - zeta_i(ji,jk) * zkappa_i(ji,jk) |
---|
| 367 | zindterm(ji,jm) = ztiold(ji,jk) + zeta_i(ji,jk) * zradab_i(ji,jk) |
---|
[8531] | 368 | END DO |
---|
| 369 | ENDDO |
---|
| 370 | |
---|
[8562] | 371 | jm = nlay_s + nlay_i + 1 |
---|
[8565] | 372 | DO ji = 1, npti |
---|
[8531] | 373 | !!ice bottom term |
---|
[8562] | 374 | ztrid(ji,jm,1) = - zeta_i(ji,nlay_i)*zkappa_i(ji,nlay_i-1) |
---|
| 375 | ztrid(ji,jm,2) = 1.0 + zeta_i(ji,nlay_i) * ( zkappa_i(ji,nlay_i) * zg1 + zkappa_i(ji,nlay_i-1) ) |
---|
| 376 | ztrid(ji,jm,3) = 0.0 |
---|
| 377 | zindterm(ji,jm) = ztiold(ji,nlay_i) + zeta_i(ji,nlay_i) * & |
---|
| 378 | & ( zradab_i(ji,nlay_i) + zkappa_i(ji,nlay_i) * zg1 * t_bo_1d(ji) ) |
---|
[8531] | 379 | ENDDO |
---|
| 380 | |
---|
| 381 | |
---|
[8565] | 382 | DO ji = 1, npti |
---|
[8534] | 383 | ! !---------------------! |
---|
[8563] | 384 | IF ( h_s_1d(ji) > 0.0 ) THEN ! snow-covered cells ! |
---|
[8534] | 385 | ! !---------------------! |
---|
[8562] | 386 | ! snow interior terms (bottom equation has the same form as the others) |
---|
| 387 | DO jm = 3, nlay_s + 1 |
---|
| 388 | jk = jm - 1 |
---|
| 389 | ztrid(ji,jm,1) = - zeta_s(ji,jk) * zkappa_s(ji,jk-1) |
---|
| 390 | ztrid(ji,jm,2) = 1.0 + zeta_s(ji,jk) * ( zkappa_s(ji,jk-1) + zkappa_s(ji,jk) ) |
---|
| 391 | ztrid(ji,jm,3) = - zeta_s(ji,jk)*zkappa_s(ji,jk) |
---|
| 392 | zindterm(ji,jm) = ztsold(ji,jk) + zeta_s(ji,jk) * zradab_s(ji,jk) |
---|
[8531] | 393 | END DO |
---|
| 394 | |
---|
[8562] | 395 | ! case of only one layer in the ice (ice equation is altered) |
---|
[8531] | 396 | IF ( nlay_i == 1 ) THEN |
---|
[8562] | 397 | ztrid(ji,nlay_s+2,3) = 0.0 |
---|
| 398 | zindterm(ji,nlay_s+2) = zindterm(ji,nlay_s+2) + zkappa_i(ji,1) * t_bo_1d(ji) |
---|
[8531] | 399 | ENDIF |
---|
| 400 | |
---|
[8534] | 401 | IF ( t_su_1d(ji) < rt0 ) THEN !-- case 1 : no surface melting |
---|
[8531] | 402 | |
---|
[8562] | 403 | jm_min(ji) = 1 |
---|
| 404 | jm_max(ji) = nlay_i + nlay_s + 1 |
---|
[8531] | 405 | |
---|
[8562] | 406 | ! surface equation |
---|
[8531] | 407 | ztrid(ji,1,1) = 0.0 |
---|
| 408 | ztrid(ji,1,2) = zdqns_ice_b(ji) - zg1s * zkappa_s(ji,0) |
---|
| 409 | ztrid(ji,1,3) = zg1s * zkappa_s(ji,0) |
---|
[8562] | 410 | zindterm(ji,1) = zdqns_ice_b(ji) * t_su_1d(ji) - zfnet(ji) |
---|
[8531] | 411 | |
---|
[8562] | 412 | ! first layer of snow equation |
---|
| 413 | ztrid(ji,2,1) = - zkappa_s(ji,0) * zg1s * zeta_s(ji,1) |
---|
| 414 | ztrid(ji,2,2) = 1.0 + zeta_s(ji,1) * ( zkappa_s(ji,1) + zkappa_s(ji,0) * zg1s ) |
---|
| 415 | ztrid(ji,2,3) = - zeta_s(ji,1)* zkappa_s(ji,1) |
---|
| 416 | zindterm(ji,2) = ztsold(ji,1) + zeta_s(ji,1) * zradab_s(ji,1) |
---|
[8531] | 417 | |
---|
[8534] | 418 | ELSE !-- case 2 : surface is melting |
---|
[8531] | 419 | ! |
---|
[8562] | 420 | jm_min(ji) = 2 |
---|
| 421 | jm_max(ji) = nlay_i + nlay_s + 1 |
---|
[8531] | 422 | |
---|
[8562] | 423 | ! first layer of snow equation |
---|
| 424 | ztrid(ji,2,1) = 0.0 |
---|
| 425 | ztrid(ji,2,2) = 1.0 + zeta_s(ji,1) * ( zkappa_s(ji,1) + zkappa_s(ji,0) * zg1s ) |
---|
| 426 | ztrid(ji,2,3) = - zeta_s(ji,1)*zkappa_s(ji,1) |
---|
[8531] | 427 | zindterm(ji,2) = ztsold(ji,1) + zeta_s(ji,1) * & |
---|
[8562] | 428 | & ( zradab_s(ji,1) + zkappa_s(ji,0) * zg1s * t_su_1d(ji) ) |
---|
[8531] | 429 | ENDIF |
---|
[8534] | 430 | ! !---------------------! |
---|
| 431 | ELSE ! cells without snow ! |
---|
| 432 | ! !---------------------! |
---|
[8531] | 433 | ! |
---|
[8534] | 434 | IF ( t_su_1d(ji) < rt0 ) THEN !-- case 1 : no surface melting |
---|
[8531] | 435 | ! |
---|
[8562] | 436 | jm_min(ji) = nlay_s + 1 |
---|
| 437 | jm_max(ji) = nlay_i + nlay_s + 1 |
---|
[8531] | 438 | |
---|
[8562] | 439 | ! surface equation |
---|
| 440 | ztrid(ji,jm_min(ji),1) = 0.0 |
---|
| 441 | ztrid(ji,jm_min(ji),2) = zdqns_ice_b(ji) - zkappa_i(ji,0)*zg1 |
---|
| 442 | ztrid(ji,jm_min(ji),3) = zkappa_i(ji,0)*zg1 |
---|
| 443 | zindterm(ji,jm_min(ji)) = zdqns_ice_b(ji)*t_su_1d(ji) - zfnet(ji) |
---|
[8531] | 444 | |
---|
[8562] | 445 | ! first layer of ice equation |
---|
| 446 | ztrid(ji,jm_min(ji)+1,1) = - zkappa_i(ji,0) * zg1 * zeta_i(ji,1) |
---|
| 447 | ztrid(ji,jm_min(ji)+1,2) = 1.0 + zeta_i(ji,1) * ( zkappa_i(ji,1) + zkappa_i(ji,0) * zg1 ) |
---|
| 448 | ztrid(ji,jm_min(ji)+1,3) = - zeta_i(ji,1) * zkappa_i(ji,1) |
---|
| 449 | zindterm(ji,jm_min(ji)+1) = ztiold(ji,1) + zeta_i(ji,1) * zradab_i(ji,1) |
---|
[8531] | 450 | |
---|
[8562] | 451 | ! case of only one layer in the ice (surface & ice equations are altered) |
---|
[8531] | 452 | IF ( nlay_i == 1 ) THEN |
---|
[8562] | 453 | ztrid(ji,jm_min(ji),1) = 0.0 |
---|
| 454 | ztrid(ji,jm_min(ji),2) = zdqns_ice_b(ji) - zkappa_i(ji,0) * 2.0 |
---|
| 455 | ztrid(ji,jm_min(ji),3) = zkappa_i(ji,0) * 2.0 |
---|
| 456 | ztrid(ji,jm_min(ji)+1,1) = -zkappa_i(ji,0) * 2.0 * zeta_i(ji,1) |
---|
| 457 | ztrid(ji,jm_min(ji)+1,2) = 1.0 + zeta_i(ji,1) * ( zkappa_i(ji,0) * 2.0 + zkappa_i(ji,1) ) |
---|
| 458 | ztrid(ji,jm_min(ji)+1,3) = 0.0 |
---|
| 459 | zindterm(ji,jm_min(ji)+1) = ztiold(ji,1) + zeta_i(ji,1) * & |
---|
| 460 | & ( zradab_i(ji,1) + zkappa_i(ji,1) * t_bo_1d(ji) ) |
---|
[8531] | 461 | ENDIF |
---|
| 462 | |
---|
[8534] | 463 | ELSE !-- case 2 : surface is melting |
---|
[8531] | 464 | |
---|
[8562] | 465 | jm_min(ji) = nlay_s + 2 |
---|
| 466 | jm_max(ji) = nlay_i + nlay_s + 1 |
---|
[8531] | 467 | |
---|
[8562] | 468 | ! first layer of ice equation |
---|
| 469 | ztrid(ji,jm_min(ji),1) = 0.0 |
---|
| 470 | ztrid(ji,jm_min(ji),2) = 1.0 + zeta_i(ji,1) * ( zkappa_i(ji,1) + zkappa_i(ji,0) * zg1 ) |
---|
| 471 | ztrid(ji,jm_min(ji),3) = - zeta_i(ji,1) * zkappa_i(ji,1) |
---|
| 472 | zindterm(ji,jm_min(ji)) = ztiold(ji,1) + zeta_i(ji,1) * & |
---|
| 473 | & ( zradab_i(ji,1) + zkappa_i(ji,0) * zg1 * t_su_1d(ji) ) |
---|
[8531] | 474 | |
---|
[8562] | 475 | ! case of only one layer in the ice (surface & ice equations are altered) |
---|
[8531] | 476 | IF ( nlay_i == 1 ) THEN |
---|
[8562] | 477 | ztrid(ji,jm_min(ji),1) = 0.0 |
---|
| 478 | ztrid(ji,jm_min(ji),2) = 1.0 + zeta_i(ji,1) * ( zkappa_i(ji,0) * 2.0 + zkappa_i(ji,1) ) |
---|
| 479 | ztrid(ji,jm_min(ji),3) = 0.0 |
---|
| 480 | zindterm(ji,jm_min(ji)) = ztiold(ji,1) + zeta_i(ji,1) * ( zradab_i(ji,1) + zkappa_i(ji,1) * t_bo_1d(ji) ) & |
---|
| 481 | & + t_su_1d(ji) * zeta_i(ji,1) * zkappa_i(ji,0) * 2.0 |
---|
[8531] | 482 | ENDIF |
---|
| 483 | |
---|
| 484 | ENDIF |
---|
| 485 | ENDIF |
---|
[8562] | 486 | ! |
---|
| 487 | zindtbis(ji,jm_min(ji)) = zindterm(ji,jm_min(ji)) |
---|
| 488 | zdiagbis(ji,jm_min(ji)) = ztrid(ji,jm_min(ji),2) |
---|
| 489 | ! |
---|
[8531] | 490 | END DO |
---|
| 491 | ! |
---|
[8534] | 492 | !------------------------------ |
---|
| 493 | ! 8) tridiagonal system solving |
---|
| 494 | !------------------------------ |
---|
[8531] | 495 | ! Solve the tridiagonal system with Gauss elimination method. |
---|
[8562] | 496 | ! Thomas algorithm, from Computational fluid Dynamics, J.D. ANDERSON, McGraw-Hill 1984 |
---|
| 497 | jm_maxt = 0 |
---|
| 498 | jm_mint = nlay_i+5 |
---|
[8565] | 499 | DO ji = 1, npti |
---|
[8562] | 500 | jm_mint = MIN(jm_min(ji),jm_mint) |
---|
| 501 | jm_maxt = MAX(jm_max(ji),jm_maxt) |
---|
[8531] | 502 | END DO |
---|
| 503 | |
---|
[8562] | 504 | DO jk = jm_mint+1, jm_maxt |
---|
[8565] | 505 | DO ji = 1, npti |
---|
[8562] | 506 | jm = min(max(jm_min(ji)+1,jk),jm_max(ji)) |
---|
| 507 | zdiagbis(ji,jm) = ztrid(ji,jm,2) - ztrid(ji,jm,1) * ztrid(ji,jm-1,3) / zdiagbis(ji,jm-1) |
---|
| 508 | zindtbis(ji,jm) = zindterm(ji,jm) - ztrid(ji,jm,1) * zindtbis(ji,jm-1) / zdiagbis(ji,jm-1) |
---|
[8531] | 509 | END DO |
---|
| 510 | END DO |
---|
| 511 | |
---|
[8565] | 512 | DO ji = 1, npti |
---|
[8531] | 513 | ! ice temperatures |
---|
[8562] | 514 | t_i_1d(ji,nlay_i) = zindtbis(ji,jm_max(ji)) / zdiagbis(ji,jm_max(ji)) |
---|
[8531] | 515 | END DO |
---|
| 516 | |
---|
[8562] | 517 | DO jm = nlay_i + nlay_s, nlay_s + 2, -1 |
---|
[8565] | 518 | DO ji = 1, npti |
---|
[8562] | 519 | jk = jm - nlay_s - 1 |
---|
| 520 | t_i_1d(ji,jk) = ( zindtbis(ji,jm) - ztrid(ji,jm,3) * t_i_1d(ji,jk+1) ) / zdiagbis(ji,jm) |
---|
[8531] | 521 | END DO |
---|
| 522 | END DO |
---|
| 523 | |
---|
[8565] | 524 | DO ji = 1, npti |
---|
[8531] | 525 | ! snow temperatures |
---|
[8563] | 526 | IF( h_s_1d(ji) > 0._wp ) THEN |
---|
[8562] | 527 | t_s_1d(ji,nlay_s) = ( zindtbis(ji,nlay_s+1) - ztrid(ji,nlay_s+1,3) * t_i_1d(ji,1) ) & |
---|
| 528 | & / zdiagbis(ji,nlay_s+1) |
---|
[8531] | 529 | ENDIF |
---|
| 530 | ! surface temperature |
---|
| 531 | ztsub(ji) = t_su_1d(ji) |
---|
| 532 | IF( t_su_1d(ji) < rt0 ) THEN |
---|
[8562] | 533 | t_su_1d(ji) = ( zindtbis(ji,jm_min(ji)) - ztrid(ji,jm_min(ji),3) * & |
---|
| 534 | & ( isnow(ji) * t_s_1d(ji,1) + ( 1._wp - isnow(ji) ) * t_i_1d(ji,1) ) ) / zdiagbis(ji,jm_min(ji)) |
---|
[8531] | 535 | ENDIF |
---|
| 536 | END DO |
---|
| 537 | ! |
---|
[8534] | 538 | !-------------------------------------------------------------- |
---|
| 539 | ! 9) Has the scheme converged ?, end of the iterative procedure |
---|
| 540 | !-------------------------------------------------------------- |
---|
[8531] | 541 | ! check that nowhere it has started to melt |
---|
| 542 | ! zdti_max is a measure of error, it has to be under zdti_bnd |
---|
| 543 | zdti_max = 0._wp |
---|
[8565] | 544 | DO ji = 1, npti |
---|
[8531] | 545 | t_su_1d(ji) = MAX( MIN( t_su_1d(ji) , rt0 ) , rt0 - 100._wp ) |
---|
| 546 | zdti_max = MAX( zdti_max, ABS( t_su_1d(ji) - ztsub(ji) ) ) |
---|
| 547 | END DO |
---|
| 548 | |
---|
| 549 | DO jk = 1, nlay_s |
---|
[8565] | 550 | DO ji = 1, npti |
---|
[8531] | 551 | t_s_1d(ji,jk) = MAX( MIN( t_s_1d(ji,jk), rt0 ), rt0 - 100._wp ) |
---|
| 552 | zdti_max = MAX( zdti_max, ABS( t_s_1d(ji,jk) - ztsb(ji,jk) ) ) |
---|
| 553 | END DO |
---|
| 554 | END DO |
---|
| 555 | |
---|
| 556 | DO jk = 1, nlay_i |
---|
[8565] | 557 | DO ji = 1, npti |
---|
[8564] | 558 | ztmelt_i = -tmut * sz_i_1d(ji,jk) + rt0 |
---|
[8531] | 559 | t_i_1d(ji,jk) = MAX( MIN( t_i_1d(ji,jk), ztmelt_i ), rt0 - 100._wp ) |
---|
| 560 | zdti_max = MAX( zdti_max, ABS( t_i_1d(ji,jk) - ztib(ji,jk) ) ) |
---|
| 561 | END DO |
---|
| 562 | END DO |
---|
| 563 | |
---|
| 564 | ! Compute spatial maximum over all errors |
---|
| 565 | ! note that this could be optimized substantially by iterating only the non-converging points |
---|
| 566 | IF( lk_mpp ) CALL mpp_max( zdti_max, kcom=ncomm_ice ) |
---|
| 567 | |
---|
| 568 | END DO ! End of the do while iterative procedure |
---|
| 569 | |
---|
| 570 | IF( ln_icectl .AND. lwp ) THEN |
---|
| 571 | WRITE(numout,*) ' zdti_max : ', zdti_max |
---|
| 572 | WRITE(numout,*) ' iconv : ', iconv |
---|
| 573 | ENDIF |
---|
| 574 | ! |
---|
[8534] | 575 | !----------------------------- |
---|
| 576 | ! 10) Fluxes at the interfaces |
---|
| 577 | !----------------------------- |
---|
[8565] | 578 | DO ji = 1, npti |
---|
[8531] | 579 | ! ! surface ice conduction flux |
---|
[8562] | 580 | fc_su(ji) = - isnow(ji) * zkappa_s(ji,0) * zg1s * (t_s_1d(ji,1) - t_su_1d(ji)) & |
---|
| 581 | & - ( 1._wp - isnow(ji) ) * zkappa_i(ji,0) * zg1 * (t_i_1d(ji,1) - t_su_1d(ji)) |
---|
[8531] | 582 | ! ! bottom ice conduction flux |
---|
[8562] | 583 | fc_bo_i(ji) = - zkappa_i(ji,nlay_i) * ( zg1*(t_bo_1d(ji) - t_i_1d(ji,nlay_i)) ) |
---|
[8531] | 584 | END DO |
---|
| 585 | |
---|
| 586 | ! --- computes sea ice energy of melting compulsory for icethd_dh --- ! |
---|
| 587 | CALL ice_thd_enmelt |
---|
| 588 | |
---|
| 589 | ! --- diagnose the change in non-solar flux due to surface temperature change --- ! |
---|
| 590 | IF ( ln_dqns_i ) THEN |
---|
[8565] | 591 | DO ji = 1, npti |
---|
[8531] | 592 | hfx_err_dif_1d(ji) = hfx_err_dif_1d(ji) - ( qns_ice_1d(ji) - zqns_ice_b(ji) ) * a_i_1d(ji) |
---|
| 593 | END DO |
---|
| 594 | END IF |
---|
| 595 | |
---|
| 596 | ! --- diag conservation imbalance on heat diffusion - PART 2 --- ! |
---|
| 597 | ! hfx_dif = Heat flux used to warm/cool ice in W.m-2 |
---|
| 598 | ! zhfx_err = correction on the diagnosed heat flux due to non-convergence of the algorithm used to solve heat equation |
---|
[8565] | 599 | DO ji = 1, npti |
---|
[8563] | 600 | zdq = - zq_ini(ji) + ( SUM( e_i_1d(ji,1:nlay_i) ) * h_i_1d(ji) * r1_nlay_i + & |
---|
| 601 | & SUM( e_s_1d(ji,1:nlay_s) ) * h_s_1d(ji) * r1_nlay_s ) |
---|
[8531] | 602 | |
---|
| 603 | IF( t_su_1d(ji) < rt0 ) THEN ! case T_su < 0degC |
---|
| 604 | zhfx_err = ( qns_ice_1d(ji) + qsr_ice_1d(ji) - zradtr_i(ji,nlay_i) - fc_bo_i(ji) + zdq * r1_rdtice ) * a_i_1d(ji) |
---|
| 605 | ELSE ! case T_su = 0degC |
---|
| 606 | zhfx_err = ( fc_su(ji) + i0(ji) * qsr_ice_1d(ji) - zradtr_i(ji,nlay_i) - fc_bo_i(ji) + zdq * r1_rdtice ) * a_i_1d(ji) |
---|
| 607 | ENDIF |
---|
| 608 | hfx_dif_1d(ji) = hfx_dif_1d(ji) - zdq * r1_rdtice * a_i_1d(ji) |
---|
| 609 | |
---|
| 610 | ! total heat that is sent to the ocean (i.e. not used in the heat diffusion equation) |
---|
| 611 | hfx_err_dif_1d(ji) = hfx_err_dif_1d(ji) + zhfx_err |
---|
| 612 | |
---|
| 613 | END DO |
---|
| 614 | |
---|
| 615 | ! --- Diagnostics SIMIP --- ! |
---|
[8565] | 616 | DO ji = 1, npti |
---|
[8531] | 617 | !--- Conduction fluxes (positive downwards) |
---|
[8562] | 618 | diag_fc_bo_1d(ji) = diag_fc_bo_1d(ji) + fc_bo_i(ji) * a_i_1d(ji) / at_i_1d(ji) |
---|
| 619 | diag_fc_su_1d(ji) = diag_fc_su_1d(ji) + fc_su(ji) * a_i_1d(ji) / at_i_1d(ji) |
---|
[8531] | 620 | |
---|
| 621 | !--- Snow-ice interfacial temperature (diagnostic SIMIP) |
---|
| 622 | zfac = rn_cnd_s * zh_i(ji) + ztcond_i(ji,1) * zh_s(ji) |
---|
| 623 | IF( zh_s(ji) >= 1.e-3 .AND. zfac > epsi10 ) THEN |
---|
[8562] | 624 | t_si_1d(ji) = ( rn_cnd_s * zh_i(ji) * t_s_1d(ji,1) + & |
---|
[8531] | 625 | & ztcond_i(ji,1) * zh_s(ji) * t_i_1d(ji,1) ) / zfac |
---|
| 626 | ELSE |
---|
| 627 | t_si_1d(ji) = t_su_1d(ji) |
---|
| 628 | ENDIF |
---|
| 629 | END DO |
---|
| 630 | ! |
---|
| 631 | END SUBROUTINE ice_thd_zdf |
---|
| 632 | |
---|
| 633 | |
---|
| 634 | SUBROUTINE ice_thd_enmelt |
---|
[8534] | 635 | !!------------------------------------------------------------------- |
---|
[8531] | 636 | !! *** ROUTINE ice_thd_enmelt *** |
---|
| 637 | !! |
---|
| 638 | !! ** Purpose : Computes sea ice energy of melting q_i (J.m-3) from temperature |
---|
| 639 | !! |
---|
| 640 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
---|
| 641 | !!------------------------------------------------------------------- |
---|
| 642 | INTEGER :: ji, jk ! dummy loop indices |
---|
| 643 | REAL(wp) :: ztmelts ! local scalar |
---|
| 644 | !!------------------------------------------------------------------- |
---|
| 645 | ! |
---|
| 646 | DO jk = 1, nlay_i ! Sea ice energy of melting |
---|
[8565] | 647 | DO ji = 1, npti |
---|
[8564] | 648 | ztmelts = - tmut * sz_i_1d(ji,jk) |
---|
[8531] | 649 | t_i_1d(ji,jk) = MIN( t_i_1d(ji,jk), ztmelts + rt0 ) ! Force t_i_1d to be lower than melting point |
---|
| 650 | ! (sometimes dif scheme produces abnormally high temperatures) |
---|
| 651 | e_i_1d(ji,jk) = rhoic * ( cpic * ( ztmelts - ( t_i_1d(ji,jk) - rt0 ) ) & |
---|
| 652 | & + lfus * ( 1._wp - ztmelts / ( t_i_1d(ji,jk) - rt0 ) ) & |
---|
| 653 | & - rcp * ztmelts ) |
---|
| 654 | END DO |
---|
| 655 | END DO |
---|
| 656 | DO jk = 1, nlay_s ! Snow energy of melting |
---|
[8565] | 657 | DO ji = 1, npti |
---|
[8531] | 658 | e_s_1d(ji,jk) = rhosn * ( cpic * ( rt0 - t_s_1d(ji,jk) ) + lfus ) |
---|
| 659 | END DO |
---|
| 660 | END DO |
---|
| 661 | ! |
---|
| 662 | END SUBROUTINE ice_thd_enmelt |
---|
| 663 | |
---|
| 664 | |
---|
| 665 | SUBROUTINE ice_thd_zdf_init |
---|
| 666 | !!----------------------------------------------------------------------- |
---|
| 667 | !! *** ROUTINE ice_thd_zdf_init *** |
---|
| 668 | !! |
---|
| 669 | !! ** Purpose : Physical constants and parameters associated with |
---|
| 670 | !! ice thermodynamics |
---|
| 671 | !! |
---|
| 672 | !! ** Method : Read the namthd_zdf namelist and check the parameters |
---|
| 673 | !! called at the first timestep (nit000) |
---|
| 674 | !! |
---|
| 675 | !! ** input : Namelist namthd_zdf |
---|
| 676 | !!------------------------------------------------------------------- |
---|
| 677 | INTEGER :: ios ! Local integer output status for namelist read |
---|
| 678 | !! |
---|
[8585] | 679 | NAMELIST/namthd_zdf/ ln_zdf_BL99, ln_cndi_U64, ln_cndi_P07, rn_cnd_s, rn_kappa_i, ln_dqns_i |
---|
[8531] | 680 | !!------------------------------------------------------------------- |
---|
| 681 | ! |
---|
| 682 | REWIND( numnam_ice_ref ) ! Namelist namthd_zdf in reference namelist : Ice thermodynamics |
---|
| 683 | READ ( numnam_ice_ref, namthd_zdf, IOSTAT = ios, ERR = 901) |
---|
| 684 | 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namthd_zdf in reference namelist', lwp ) |
---|
| 685 | |
---|
| 686 | REWIND( numnam_ice_cfg ) ! Namelist namthd_zdf in configuration namelist : Ice thermodynamics |
---|
| 687 | READ ( numnam_ice_cfg, namthd_zdf, IOSTAT = ios, ERR = 902 ) |
---|
| 688 | 902 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namthd_zdf in configuration namelist', lwp ) |
---|
| 689 | IF(lwm) WRITE ( numoni, namthd_zdf ) |
---|
| 690 | ! |
---|
| 691 | ! |
---|
| 692 | IF(lwp) THEN ! control print |
---|
| 693 | WRITE(numout,*) 'ice_thd_zdf_init: Ice vertical heat diffusion' |
---|
| 694 | WRITE(numout,*) '~~~~~~~~~~~~~~~~' |
---|
| 695 | WRITE(numout,*) ' Namelist namthd_zdf:' |
---|
[8585] | 696 | WRITE(numout,*) ' Diffusion follows a Bitz and Lipscomb (1999) ln_zdf_BL99 = ', ln_zdf_BL99 |
---|
[8531] | 697 | WRITE(numout,*) ' thermal conductivity in the ice (Untersteiner 1964) ln_cndi_U64 = ', ln_cndi_U64 |
---|
| 698 | WRITE(numout,*) ' thermal conductivity in the ice (Pringle et al 2007) ln_cndi_P07 = ', ln_cndi_P07 |
---|
| 699 | WRITE(numout,*) ' thermal conductivity in the snow rn_cnd_s = ', rn_cnd_s |
---|
| 700 | WRITE(numout,*) ' extinction radiation parameter in sea ice rn_kappa_i = ', rn_kappa_i |
---|
| 701 | WRITE(numout,*) ' change the surface non-solar flux with Tsu or not ln_dqns_i = ', ln_dqns_i |
---|
| 702 | ENDIF |
---|
| 703 | ! |
---|
| 704 | IF ( ( ln_cndi_U64 .AND. ln_cndi_P07 ) .OR. ( .NOT.ln_cndi_U64 .AND. .NOT.ln_cndi_P07 ) ) THEN |
---|
[8534] | 705 | CALL ctl_stop( 'ice_thd_zdf_init: choose one and only one formulation for thermal conduction (ln_cndi_U64 or ln_cndi_P07)' ) |
---|
[8531] | 706 | ENDIF |
---|
| 707 | ! |
---|
| 708 | END SUBROUTINE ice_thd_zdf_init |
---|
| 709 | |
---|
| 710 | #else |
---|
| 711 | !!---------------------------------------------------------------------- |
---|
[8534] | 712 | !! Default option Dummy Module No ESIM sea-ice model |
---|
[8531] | 713 | !!---------------------------------------------------------------------- |
---|
| 714 | #endif |
---|
| 715 | |
---|
| 716 | !!====================================================================== |
---|
| 717 | END MODULE icethd_zdf |
---|