| 47 | | !---------------------------------------------------------------------------------- |
| 48 | | &namtra_ldf ! lateral diffusion scheme for tracers |
| 49 | | !---------------------------------------------------------------------------------- |
| 50 | | ! ! Operator type: |
| 51 | | ln_traldf_lap = .false. ! laplacian operator |
| 52 | | ln_traldf_blp = .false. ! bilaplacian operator |
| 53 | | ! ! Direction of action: |
| 54 | | ln_traldf_lev = .false. ! iso-level |
| 55 | | ln_traldf_hor = .false. ! horizontal (geopotential) |
| 56 | | ln_traldf_iso = .true. ! iso-neutral |
| 57 | | ln_traldf_triad = .false. ! iso-neutral using Griffies triads |
| 58 | | ! |
| 59 | | ! ! iso-neutral options: |
| 60 | | ln_traldf_msc = .true. ! Method of Stabilizing Correction (both operators) |
| 61 | | rn_slpmax = 0.01 ! slope limit (both operators) |
| 62 | | ln_triad_iso = .false. ! pure horizontal mixing in ML (triad only) |
| 63 | | rn_sw_triad = 1 ! =1 switching triad ; =0 all 4 triads used (triad only) |
| 64 | | ln_botmix_triad = .false. ! lateral mixing on bottom (triad only) |
| 65 | | ! |
| 66 | | ! ! Coefficients: |
| 67 | | nn_aht_ijk_t = 21 ! space/time variation of eddy coef |
| 68 | | ! ! =-20 (=-30) read in eddy_diffusivity_2D.nc (..._3D.nc) file |
| 69 | | ! ! = 0 constant |
| 70 | | ! ! = 10 F(k) =ldf_c1d |
| 71 | | ! ! = 20 F(i,j) =ldf_c2d |
| 72 | | ! ! = 21 F(i,j,t) =Treguier et al. JPO 1997 formulation |
| 73 | | ! ! = 30 F(i,j,k) =ldf_c2d + ldf_c1d |
| 74 | | ! ! = 31 F(i,j,k,t)=F(local velocity) |
| 75 | | rn_aht_0 = 2000. ! lateral eddy diffusivity (lap. operator) [m2/s] |
| 76 | | rn_bht_0 = 1.e+12 ! lateral eddy diffusivity (bilap. operator) [m4/s] |
| 77 | | / |
| 78 | | !---------------------------------------------------------------------------------- |
| 79 | | &namtra_ldfeiv ! eddy induced velocity param. |
| 80 | | !---------------------------------------------------------------------------------- |
| 81 | | ln_ldfeiv =.true. ! use eddy induced velocity parameterization |
| 82 | | ln_ldfeiv_dia =.true. ! diagnose eiv stream function and velocities |
| 83 | | rn_aeiv_0 = 2000. ! eddy induced velocity coefficient [m2/s] |
| 84 | | nn_aei_ijk_t = 21 ! space/time variation of the eiv coeficient |
| 85 | | ! ! =-20 (=-30) read in eddy_induced_velocity_2D.nc (..._3D.nc) file |
| 86 | | ! ! = 0 constant |
| 87 | | ! ! = 10 F(k) =ldf_c1d |
| 88 | | ! ! = 20 F(i,j) =ldf_c2d |
| 89 | | ! ! = 21 F(i,j,t) =Treguier et al. JPO 1997 formulation |
| 90 | | ! ! = 30 F(i,j,k) =ldf_c2d + ldf_c1d |
| 91 | | / |
| | 22 | MODULE zdftmx |
| | 23 | ... |
| | 24 | #if defined key_zdftmx || defined key_esopa |
| | 25 | !!---------------------------------------------------------------------- |
| | 26 | !! 'key_zdftmx' Tidal vertical mixing <<<==OLD version |
| | 27 | !!---------------------------------------------------------------------- |
| | 28 | !! zdf_tmx : global momentum & tracer Kz with tidal induced Kz |
| | 29 | !! tmx_itf : Indonesian momentum & tracer Kz with tidal induced Kz |
| | 30 | !! zdf_tmx_init : initialisation of tidal induced Kz |
| | 31 | !!---------------------------------------------------------------------- |
| | 32 | ... |
| | 33 | LOGICAL, PUBLIC, PARAMETER :: lk_zdftmx = .TRUE. !: tidal mixing flag <<=== same flag |
| | 34 | ... |
| | 35 | #elif defined key_zdftmx_new |
| | 36 | !!---------------------------------------------------------------------- |
| | 37 | !! 'key_zdftmx_new' New Tidal vertical mixing <<<==NEW version |
| | 38 | !!---------------------------------------------------------------------- |
| | 39 | !! zdf_tmx : global momentum & tracer Kz with tidal induced Kz |
| | 40 | !! zdf_tmx_init : initialisation of tidal induced Kz |
| | 41 | !!---------------------------------------------------------------------- |
| | 42 | ... |
| | 43 | LOGICAL, PUBLIC, PARAMETER :: lk_zdftmx = .TRUE. !: tidal mixing flag <<=== same flag |
| | 44 | ... |
| | 45 | #else |
| | 46 | !!---------------------------------------------------------------------- |
| | 47 | !! Default option Dummy module NO Tidal MiXing |
| | 48 | !!---------------------------------------------------------------------- |
| | 49 | ... |
| | 50 | #endif |
| 97 | | '''Pending issues''' : [[BR]]- verify diaptr.F90 : not sure it is OK[[BR]]- add the max grid size in the coordinate file and use it to compute grid dependent diffusivity. This will solve an issue with regional and AGRIF configurations[[BR]]- test all 6 operators.[[BR]]- In field_def.xml add a comment to say where is the routine calling the corresponding iom_put[[BR]]- in the documentation, add a change in the DOCTOR norm: np_ is now a prefix used for PARAMETER |
| 98 | | |
| 99 | | === [[BR]]II.2 — Advective trends (TRA/traadv....) === |
| 100 | | ===>>> ''' OK''' see revision [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5737 5770] & [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5737 5771] ===>> SETTE OK with revision [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5737 5774] & [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5737 5775] |
| 101 | | |
| 102 | | - traadv_muscl2.F90 removed[[BR]]- traadv_muscl.F90 renamed traadv_mus.F90[[BR]]- traadv_cen2.F90 replaced by traadv_cen which provides 2nd and 4th order centered scheme on both horizontal and vertical directions.[[BR]]- name TVD has been changed to the more commonly used FCT (Flux Correction Transport)[[BR]]- FCT offers now 2nd and 4th order centered scheme on both horizontal and vertical directions.[[BR]]- UBS offers now in option either a 2nd order FCT or a 4th order COMPACT scheme in the vertical direction[[BR]]- NB in case of 4th order in the vertical, CEN, UBS and FCT use a compact 4th order scheme[[BR]]- key_esopa removed from traadv.F90[[BR]]- Surface boundary condition in ISF case has been added in all cases (except 4th order COMPACT scheme which have not been tested with ISF) |
| 103 | | |
| 104 | | {{{ |
| 105 | | !----------------------------------------------------------------------- |
| 106 | | &namtra_adv ! advection scheme for tracer |
| 107 | | !----------------------------------------------------------------------- |
| 108 | | ln_traadv_cen = .false. ! 2nd order centered scheme |
| 109 | | nn_cen_h = 4 ! =2/4, horizontal 2nd order CEN / 4th order CEN |
| 110 | | nn_cen_v = 4 ! =2/4, vertical 2nd order CEN / 4th order COMPACT |
| 111 | | ln_traadv_fct = .false. ! FCT scheme |
| 112 | | nn_fct_h = 2 ! =2/4, horizontal 2nd / 4th order |
| 113 | | nn_fct_v = 2 ! =2/4, vertical 2nd / COMPACT 4th order |
| 114 | | nn_fct_zts = 0 ! > 1 , 2nd order FCT scheme with vertical sub-timestepping |
| 115 | | ! ! (number of sub-timestep = nn_fct_zts) |
| 116 | | ln_traadv_mus = .false. ! MUSCL scheme |
| 117 | | ln_mus_ups = .false. ! use upstream scheme near river mouths |
| 118 | | ln_traadv_ubs = .false. ! UBS scheme |
| 119 | | nn_ubs_v = 2 ! =2 , vertical 2nd order FCT |
| 120 | | ln_traadv_qck = .false. ! QUICKEST scheme |
| 121 | | / |
| 122 | | }}} |
| 123 | | '''Unresolved issues/improvement''' on TRAADV: [[BR]]- QCK: cross terms are missing. alternate direction should be added....[[BR]]- Bug in FCT with sub-time-stepping and key_vvl. The change in e3 should be taken into account in the sub-timesteps.[[BR]]- traadv_mus.F90 some rather simple optimization can be added...[[BR]]- traadv_qck.F90 : possibility to add a 4th order COMPACT scheme on the vertical. [[BR]]- 4th order COMPACT have not been tested with ISF. The routine needs probably to be modified. |
| 124 | | |
| 125 | | === [[BR]]II.3 — Miscellaneous === |
| 126 | | * Atmospheric pressure forcing: change to a systematic call of sbc_apr in step.F90 (with or without BDY) and remove its call from sbcmod |
| 127 | | * remove key_vectopt_loop from all the code except in vectopt_loop_substitute.h90 (it is an obsolescent feature only adapted to vector computers) |
| 128 | | * remove all "!CDIR " lines = NEC vector compiler instructions |
| 129 | | |
| 130 | | == [[BR]][[BR]][[BR]]III. Phasing of momentum trends == |
| 131 | | ===>>> ''' OK''' see revision [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5777 5777] & [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5778 5778] and [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5782 5782] with SETTE OK |
| 132 | | |
| 133 | | === [[BR]]III.1 — LDF on dynamics - viscous trends === |
| 134 | | ''operator'': [[BR]]- laplacian operator: re-entrant laplacian for iso-level operators (routine dyn_ldf_lap found in dynldf_lap_blp);[[BR]]- bilaplacian operator: dynldf_blp.F90 module: use of the re-entrant iso-level laplacian (routine dyn_ldf_blp found in dynldf_lap_blp.F90)[[BR]]- suppression of dynnept.F90 to finalize the suppression of Neptune effect param. ;[[BR]]- suppression of dynldf_lap.F90 and dynldf_bilap.F90 replaced by dynldf_lap_blp.F90 (which contains dyn_ldf_lap & dyn_ldf_blp routines) ; dynldf_bilapg.F90 (remove old and approximative rotated bi-laplacian on momentum)[[BR]]- rotb and rotn arrays suppressed (even from the restart file) NB: the viscous operator now uses the full before velocity field (i.e. including the asselin filter)[[BR]]- hdivb array is suppressed. hdivn and hdivb are removed from restart[[BR]]- associate with rotn and rotb suppression comes the suppression of no-slip accurate option (key_noslip_accurate is removed)[[BR]]- divcur.F90 becomes divhor.F90 and only computes the horizontal divergence |
| 135 | | |
| 136 | | [[BR]]''lateral mixing coefficient'':[[BR]]- new user interface (namelist) : |
| 137 | | |
| 138 | | {{{ |
| 139 | | !----------------------------------------------------------------------- |
| 140 | | &namdyn_ldf ! lateral diffusion on momentum |
| 141 | | !----------------------------------------------------------------------- |
| 142 | | ! ! Type of the operator : |
| 143 | | ! ! no diffusion: set ln_dynldf_lap=..._blp=F |
| 144 | | ln_dynldf_lap = .false. ! laplacian operator |
| 145 | | ln_dynldf_blp = .false. ! bilaplacian operator |
| 146 | | ! ! Direction of action : |
| 147 | | ln_dynldf_lev = .false. ! iso-level |
| 148 | | ln_dynldf_hor = .false. ! horizontal (geopotential) |
| 149 | | ln_dynldf_iso = .false. ! iso-neutral |
| 150 | | ! ! Coefficient |
| 151 | | nn_ahm_ijk_t = 0 ! space/time variation of eddy coef |
| 152 | | ! ! =-30 read in eddy_viscosity_3D.nc file |
| 153 | | ! ! =-20 read in eddy_viscosity_3D.nc file |
| 154 | | ! ! = 0 constant |
| 155 | | ! ! = 10 F(k)=c1d |
| 156 | | ! ! = 20 F(i,j)=F(grid spacing)=c2d |
| 157 | | ! ! = 30 F(i,j,k)=c2d*c1d |
| 158 | | ! ! = 31 F(i,j,k)=F(grid spacing and local velocity) |
| 159 | | rn_ahm_0 = 40000. ! horizontal laplacian eddy viscosity [m2/s] |
| 160 | | rn_ahm_b = 0. ! background eddy viscosity for ldf_iso [m2/s] |
| 161 | | rn_bhm_0 = 1.e+12 ! horizontal bilaplacian eddy viscosity [m4/s] |
| 162 | | ! |
| 163 | | ! Caution in 20 and 30 cases the coefficient have to be given for a 1 degree grid (~111km) |
| 164 | | / |
| 165 | | }}} |
| 166 | | [[BR]]- default value of the namelist: ''no operator chosen'': ln_dynldf_lap=dyndf_blp=0 ==>>> No lateral diffusion applied on momentum[[BR]]- create the 2D and 3D ahmt and ahmf file for ORCA_R2 '''===>>> TO BE DONE for ORCA_R1''' . nn_ahm_ijk_t must be set to -20 or -30 for ORCA2 and ORCA1 (read in a file) [[BR]]- both laplacian and bi-laplacian coef. are always 3D arrays defined at T- and F- points. Bi-laplacian eddy coefficient defined as SQRT(bhm) [[BR]]''' ====>>> TO BE DONE: explore the possibility of u- and v-points'''[[BR]]- redesign of space variation of the eddy viscosity: suppression of: ldfdyn_substitute.h90 ; ldfdyn_c1d.h90 , ldfdyn_c2d.h90 and ldfdyn_c3d.h90 (replaced by ldfc1d_c2d.F90, a module share with ldftra.F90) ; ldfdyn_oce.F90 (now included in ldfdyn.F90)[[BR]]- remove ldfdyn_smag.F90 (suppression of smagorinsky option) '''==>>> TO BE re-add in the new framework by someone...'''[[BR]]- suppression of key_esopa in dynldf.F90[[BR]]- suppression of key_dynldf_c1d, key_dynldf_c2d, key_dynldf_c3d[[BR]]- change in all standard namelist_cfg and 1_namelist_cfg [[BR]]- Namelist default values : NO operator ; NO direction ===>>> No lateral mixing applied on momentum ===>>> must be specified in all CONFIG |
| 167 | | |
| 168 | | === [[BR]]III.2 —''' '''ADV on dynamics''' - advective trends''' === |
| 169 | | ===>>> ''' OK''' see revision [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5778 5778] and [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5786 5786] with SETTE OK |
| 170 | | |
| 171 | | ''dynvor.F90 (impact also dynspg_ts.F90)''[[BR]] - remove key_esopa[[BR]] - remove dyn_vor_mix : now successive call of den_vor_ene (Coriolis) and din_vor_ens (relative voricity)[[BR]] - replace rotn by its calculation everywhere in dynvor.F90[[BR]] - remove the use of fmask from standard vorticity calculation in dynvor.F90 but add a namelist parameter (ln_dynvor_msk) to multiply by fmask the vorticity term[[BR]]- add an namelist option to mask or not the vorticity (including Coriolis) '''CAUTION''' : the mask option does not work: set to FALSE by default with comment DO NOT set it to TRUE (see ''' [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5827 5827]''' )[[BR]]- change ln_dynvor_een_old into nn_een_e3f = 0/1 |
| 172 | | |
| 173 | | namdyn_vor becomes: |
| 174 | | |
| 175 | | {{{ |
| 176 | | !----------------------------------------------------------------------- |
| 177 | | &namdyn_vor ! option of physics/algorithm (not control by CPP keys) |
| 178 | | !----------------------------------------------------------------------- |
| 179 | | ln_dynvor_ene = .false. ! enstrophy conserving scheme |
| 180 | | ln_dynvor_ens = .false. ! energy conserving scheme |
| 181 | | ln_dynvor_mix = .false. ! mixed scheme |
| 182 | | ln_dynvor_een = .true. ! energy & enstrophy scheme |
| 183 | | nn_een_e3f = 1 ! e3f = masked averaging of e3t divided by 4 (=0) or by the sum of mask (=1) |
| 184 | | ln_dynvor_msk = .false. ! vorticity multiplied by fmask (=T) or not (=F) (all vorticity schemes) |
| 185 | | / |
| 186 | | }}} |
| 187 | | ''dynadv.F90[[BR]]''- remove key_esopa[[BR]]- introduce parameter in the SELECT CASE |
| 188 | | |
| 189 | | namlist_ref and all CONFIG namelists updated |
| 190 | | |
| 191 | | === [[BR]]III.3 Miscellaneous === |
| 192 | | * key_esopa has been remove from the whole NEMO code '''DONE''' see rev. [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5778 5778] |
| 193 | | * remove key_noslip_accurate from dom_oce.F90 and domsk.F90. '''DONE''' see rev. [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5829 5829] |
| 194 | | * remove duplicate print of "W A R N I N G" and "E R R O R" in ctl_nam routine '''DONE''' see rev. [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5829 5829] |
| 195 | | * remove ll_is_orca and its associated use in domvvl.F90 (no used anymore) '''DONE''' see rev [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5829 5829] |
| 196 | | * remove ttrdmp & strdmp arrays (not used anymore) '''DONE see rev'''.''' [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5830 5830]''' |
| 197 | | * remove the remaining use of ua,va as workspace (changes in trazdf_imp.F90, zdfevd.F90, zdftmx.F90 and oce_trc.F90) '''DONE''' see rev. [https://forge.ipsl.jussieu.fr/nemo/log/branches/2015/dev_r5721_CNRS9_NOC3_LDF?rev=5831 5831] |
| 198 | | |
| 199 | | == [[BR]]IV. Pending issues : need to be solved before v3.7 release == |
| 200 | | '''•''' Update the documentation. |
| 201 | | |
| 202 | | '''•''' ensure the restartability & reproducibility for triad operator. |
| 203 | | |
| 204 | | '''• ''' specification of eddy viscosity/diffusivity coefficients in case of grid-size dependency. |
| 205 | | |
| 206 | | Issue: define the grid-size dependency in such a way that does not require the Equator being inside the domain.[[BR]]Solution: [[BR]]'''- add''' a scalar in the coordinate file which is equal to the grid-size at the equator even if Equator is not in the domain and use this scalar to compute the grid-size dependency of the coefficients. [[BR]]In addition:[[BR]]- '''add''' in NEMOGCM/TOOLS directory a program that read a coordinates.nc file apply a reduction of scale factors in some straits, and create the associated extended coordinates file (coordinates_e1e2u_v.nc)[[BR]]- '''create''' the extended coordinates files form ORCA 2°, 1°, and 0.5°. ===>>> Done for ORCA 2° and 1°, '''1/2° and 1/4° missing...[[BR]]'''- '''explore''' the possibility of defining ahm coef. at u- and v-points. This will improve the velocity dependent case. |
| 207 | | |
| 208 | | '''• '''specification of lateral friction at the coast.[[BR]]Issue: the different values of fmask at the coast have been removed so that this lateral boundary condition doesn't affect the advective term (''' double check that''' !). fmask is still used for laplacian and bilaplacian viscosities. Nevertheless, the magnitude of lateral friction depends on the magnitude of ahm (bhm, reap.). It seems better to define this magnitude [[BR]]Solution: |
| 209 | | |
| 210 | | == [[BR]][[BR]]V. Pending issues : to be solved in 2016 ? == |
| 211 | | '''(V.1)''' Add a proper coding of Smagorinsky eddy viscosity and diffusivity... |
| 212 | | |
| 213 | | '''(V.2)''' It should be possible to remove hdivn ... think about that |
| 214 | | |
| 215 | | ---- |
| 216 | | = [[BR]] Next Step = |
| 217 | | Starting from the '''trunk''' (revision: [https://forge.ipsl.jussieu.fr/nemo/log/trunk/NEMOGCM?rev=5838 5836]), which has been phased with the branch described here, several branches are created which will contain the following item: |
| 218 | | |
| 219 | | • Documentation : create a branch (shared among all developers) to document both the changes in revision [https://forge.ipsl.jussieu.fr/nemo/log/trunk/NEMOGCM?rev=5838 5836] and those in branches starting from this revision. |
| 220 | | |
| 221 | | • Non linear free surface by default ([https://forge.ipsl.jussieu.fr/nemo/browser/branches/2015/dev_r5836_NOC3_vvl_by_default dev_r5836_NOC3_vvl_by_default]). see Wiki page [https://forge.ipsl.jussieu.fr/nemo/wiki/ticket/5836_NOC3_vvl_by_default 5836_NOC3_vvl_by_default] |
| 222 | | |
| 223 | | • ZDF simplification: introduce a vertical physics manager that allows to save MPP communications. remove avmu, avmv. remove all key_zdfxxx (a Gurvan's branch) |
| 224 | | |
| 225 | | • create trptra.F90 which compute the effective velocity for both TRC and TRA (a Gurvan's branch) |
| 226 | | |
| 227 | | • remove all remaining hard coded parts specific to a configuration (especially ORCA2): see a description of the remaining work here: [https://forge.ipsl.jussieu.fr/nemo/wiki/2014WP/2014_SystemSimplification_hard_coding SystemSimplification_hard_coding] |
| 228 | | |
| 229 | | • remove most of the remaining CPP keys (key_trabbl, key_zdf...) |
| 230 | | |
| 231 | | • remove the solver, keeping only split-explicit scheme for free-surface time stepping. (Jérome's branch) |
| 232 | | |
| 233 | | .... |
| 234 | | |
| 235 | | ---- |
| 236 | | = To be CHECKED = |
| 237 | | (not necessary associated with this branch) |
| 238 | | |
| 239 | | * find ''!!gm'' everywhere in the fortran code, and try to solve the issues raised ! |
| 240 | | * check that task_i use ssmask, i.e. that it takes into account the under ice shelf seas. |
| 241 | | * CRS : the new arrays derived from horizontal scale factors MUST be added in CRS. |
| 242 | | * Bug in diawri.F90 when NOT using key_iomput (OK ==>> see ticket #1596) |
| 243 | | |
| 244 | | * Idea for finalization of domhgr.F90 :[[BR]]'''add''' 2 modules (from domhgr.F90), domhgr_read.F90 and domhgr_ana.F90, which contains:[[BR]]- domhgr_read.F90: the CASE jphgr_msh=0 of domhgr.F90 (i.e. read the coordinates file)[[BR]]- domhgr_ana.F90: the CASE jphgr_msh=5 of domhgr.F90 (i.e. the GYRE analytical definition of the coordinates)[[BR]]'''add''' in NEMOGCM/TOOLS a directory containing 3 domhgr_ana.F90 modules associated with (1) a geographical mesh on the sphere with regular (in degree) grid-spacing (jphgr_msh=1) ; (2) f- or beta-plane with regular grid-spacing (jphgr_msh=2 or 3)) ; (3) geographical mesh on the sphere, isotropic MERCATOR type (jphgr_msh=4)[[BR]]'''remove''' from the namelist_ref/namdom all variable related to the horizontal mesh, and add a flag, ln_mesh_read, =T read the coordinates.nc file ; =F analytical mesh (by default GYRE mesh). |
| 245 | | * sbcisf.F90 : use of hard coded staff associated with EOS (in situ temperature and co ...) |
| 246 | | * sbcwave.F90 : lot of modifications has been done, but I'm still uncomfortable with the calculation of stokes drift velocities....[[BR]][[BR]] |
| 247 | | |
| 248 | | ... |
| 249 | | |
| 250 | | ---- |
| | 55 | (3) add in the input file of both ORCA2 and ORCA1 the input files of the new TMX |
