[1992] | 1 | |
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[1403] | 2 | ! $Id: aaam_bud.F90 5116 2024-07-24 12:54:37Z evignon $ |
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[644] | 3 | |
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[1992] | 4 | SUBROUTINE aaam_bud(iam, nlon, nlev, rjour, rsec, rea, rg, ome, plat, plon, & |
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| 5 | phis, dragu, liftu, phyu, dragv, liftv, phyv, p, u, v, aam, torsfc) |
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[644] | 6 | |
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[1992] | 7 | USE dimphy |
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[5110] | 8 | USE lmdz_grid_phy, ONLY: nbp_lon, nbp_lat, klon_glo |
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[5111] | 9 | USE lmdz_abort_physic, ONLY: abort_physic |
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[1992] | 10 | IMPLICIT NONE |
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| 11 | ! ====================================================================== |
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| 12 | ! Auteur(s): F.Lott (LMD/CNRS) date: 20031020 |
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| 13 | ! Object: Compute different terms of the axial AAAM Budget. |
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| 14 | ! No outputs, every AAM quantities are written on the IAM |
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| 15 | ! File. |
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[1403] | 16 | |
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[1992] | 17 | ! Modif : I.Musat (LMD/CNRS) date : 20041020 |
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| 18 | ! Outputs : axial components of wind AAM "aam" and total surface torque |
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| 19 | ! "torsfc", |
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| 20 | ! but no write in the iam file. |
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[1403] | 21 | |
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[1992] | 22 | ! WARNING: Only valid for regular rectangular grids. |
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| 23 | ! REMARK: CALL DANS PHYSIQ AFTER lift_noro: |
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| 24 | ! CALL aaam_bud (27,klon,klev,rjourvrai,gmtime, |
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| 25 | ! C ra,rg,romega, |
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| 26 | ! C rlat,rlon,pphis, |
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| 27 | ! C zustrdr,zustrli,zustrph, |
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| 28 | ! C zvstrdr,zvstrli,zvstrph, |
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| 29 | ! C paprs,u,v) |
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[1403] | 30 | |
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[1992] | 31 | ! ====================================================================== |
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| 32 | ! Explicit Arguments: |
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| 33 | ! ================== |
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| 34 | ! iam-----input-I-File number where AAMs and torques are written |
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| 35 | ! It is a formatted file that has been opened |
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| 36 | ! in physiq.F |
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| 37 | ! nlon----input-I-Total number of horizontal points that get into physics |
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| 38 | ! nlev----input-I-Number of vertical levels |
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| 39 | ! rjour -R-Jour compte depuis le debut de la simu (run.def) |
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| 40 | ! rsec -R-Seconde de la journee |
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| 41 | ! rea -R-Earth radius |
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| 42 | ! rg -R-gravity constant |
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| 43 | ! ome -R-Earth rotation rate |
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| 44 | ! plat ---input-R-Latitude en degres |
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| 45 | ! plon ---input-R-Longitude en degres |
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| 46 | ! phis ---input-R-Geopotential at the ground |
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| 47 | ! dragu---input-R-orodrag stress (zonal) |
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| 48 | ! liftu---input-R-orolift stress (zonal) |
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| 49 | ! phyu----input-R-Stress total de la physique (zonal) |
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| 50 | ! dragv---input-R-orodrag stress (Meridional) |
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| 51 | ! liftv---input-R-orolift stress (Meridional) |
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| 52 | ! phyv----input-R-Stress total de la physique (Meridional) |
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| 53 | ! p-------input-R-Pressure (Pa) at model half levels |
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| 54 | ! u-------input-R-Horizontal wind (m/s) |
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| 55 | ! v-------input-R-Meridional wind (m/s) |
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| 56 | ! aam-----output-R-Axial Wind AAM (=raam(3)) |
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| 57 | ! torsfc--output-R-Total surface torque (=tmou(3)+tsso(3)+tbls(3)) |
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[644] | 58 | |
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[1992] | 59 | ! Implicit Arguments: |
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| 60 | ! =================== |
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[644] | 61 | |
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[2346] | 62 | ! nbp_lon--common-I: Number of longitude intervals |
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| 63 | ! (nbp_lat-1)--common-I: Number of latitude intervals |
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[1992] | 64 | ! klon-common-I: Number of points seen by the physics |
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[2346] | 65 | ! nbp_lon*(nbp_lat-2)+2 for instance |
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[1992] | 66 | ! klev-common-I: Number of vertical layers |
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| 67 | ! ====================================================================== |
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| 68 | ! Local Variables: |
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| 69 | ! ================ |
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| 70 | ! dlat-----R: Latitude increment (Radians) |
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| 71 | ! dlon-----R: Longitude increment (Radians) |
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| 72 | ! raam ---R: Wind AAM (3 Components, 1 & 2 Equatoriales; 3 Axiale) |
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| 73 | ! oaam ---R: Mass AAM (3 Components, 1 & 2 Equatoriales; 3 Axiale) |
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| 74 | ! tmou-----R: Resolved Mountain torque (3 components) |
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| 75 | ! tsso-----R: Parameterised Moutain drag torque (3 components) |
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| 76 | ! tbls-----R: Parameterised Boundary layer torque (3 components) |
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[644] | 77 | |
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[1992] | 78 | ! LOCAL ARRAY: |
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| 79 | ! =========== |
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| 80 | ! zs ---R: Topographic height |
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| 81 | ! ps ---R: Surface Pressure |
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| 82 | ! ub ---R: Barotropic wind zonal |
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| 83 | ! vb ---R: Barotropic wind meridional |
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| 84 | ! zlat ---R: Latitude in radians |
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| 85 | ! zlon ---R: Longitude in radians |
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| 86 | ! ====================================================================== |
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[644] | 87 | |
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[1992] | 88 | ! ARGUMENTS |
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[644] | 89 | |
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[1992] | 90 | INTEGER iam, nlon, nlev |
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| 91 | REAL, INTENT (IN) :: rjour, rsec, rea, rg, ome |
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| 92 | REAL plat(nlon), plon(nlon), phis(nlon) |
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| 93 | REAL dragu(nlon), liftu(nlon), phyu(nlon) |
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| 94 | REAL dragv(nlon), liftv(nlon), phyv(nlon) |
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| 95 | REAL p(nlon, nlev+1), u(nlon, nlev), v(nlon, nlev) |
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[644] | 96 | |
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[1992] | 97 | ! Variables locales: |
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[644] | 98 | |
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[1992] | 99 | INTEGER i, j, k, l |
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| 100 | REAL xpi, hadley, hadday |
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| 101 | REAL dlat, dlon |
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| 102 | REAL raam(3), oaam(3), tmou(3), tsso(3), tbls(3) |
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| 103 | INTEGER iax |
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| 104 | ! IM ajout aam, torsfc |
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| 105 | ! aam = composante axiale du Wind AAM raam |
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| 106 | ! torsfc = composante axiale de (tmou+tsso+tbls) |
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| 107 | REAL aam, torsfc |
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[644] | 108 | |
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[1992] | 109 | REAL zs(801, 401), ps(801, 401) |
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| 110 | REAL ub(801, 401), vb(801, 401) |
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| 111 | REAL ssou(801, 401), ssov(801, 401) |
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| 112 | REAL blsu(801, 401), blsv(801, 401) |
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| 113 | REAL zlon(801), zlat(401) |
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[644] | 114 | |
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[1992] | 115 | CHARACTER (LEN=20) :: modname = 'aaam_bud' |
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| 116 | CHARACTER (LEN=80) :: abort_message |
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[644] | 117 | |
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| 118 | |
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| 119 | |
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[1992] | 120 | ! PUT AAM QUANTITIES AT ZERO: |
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[644] | 121 | |
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[2346] | 122 | IF (nbp_lon+1>801 .OR. nbp_lat>401) THEN |
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[1992] | 123 | abort_message = 'Pb de dimension dans aaam_bud' |
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[2311] | 124 | CALL abort_physic(modname, abort_message, 1) |
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[1992] | 125 | END IF |
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[644] | 126 | |
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[1992] | 127 | xpi = acos(-1.) |
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| 128 | hadley = 1.E18 |
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| 129 | hadday = 1.E18*24.*3600. |
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[5081] | 130 | IF(klon_glo==1) THEN |
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[2350] | 131 | dlat = xpi |
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| 132 | ELSE |
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| 133 | dlat = xpi/real(nbp_lat-1) |
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| 134 | ENDIF |
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[2346] | 135 | dlon = 2.*xpi/real(nbp_lon) |
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[644] | 136 | |
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[1992] | 137 | DO iax = 1, 3 |
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| 138 | oaam(iax) = 0. |
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| 139 | raam(iax) = 0. |
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| 140 | tmou(iax) = 0. |
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| 141 | tsso(iax) = 0. |
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| 142 | tbls(iax) = 0. |
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| 143 | END DO |
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[644] | 144 | |
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[1992] | 145 | ! MOUNTAIN HEIGHT, PRESSURE AND BAROTROPIC WIND: |
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[644] | 146 | |
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[1992] | 147 | ! North pole values (j=1): |
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[644] | 148 | |
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[1992] | 149 | l = 1 |
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[644] | 150 | |
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[1992] | 151 | ub(1, 1) = 0. |
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| 152 | vb(1, 1) = 0. |
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| 153 | DO k = 1, nlev |
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| 154 | ub(1, 1) = ub(1, 1) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 155 | vb(1, 1) = vb(1, 1) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 156 | END DO |
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[644] | 157 | |
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[1992] | 158 | zlat(1) = plat(l)*xpi/180. |
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[644] | 159 | |
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[2346] | 160 | DO i = 1, nbp_lon + 1 |
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[644] | 161 | |
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[1992] | 162 | zs(i, 1) = phis(l)/rg |
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| 163 | ps(i, 1) = p(l, 1) |
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| 164 | ub(i, 1) = ub(1, 1) |
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| 165 | vb(i, 1) = vb(1, 1) |
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| 166 | ssou(i, 1) = dragu(l) + liftu(l) |
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| 167 | ssov(i, 1) = dragv(l) + liftv(l) |
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| 168 | blsu(i, 1) = phyu(l) - dragu(l) - liftu(l) |
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| 169 | blsv(i, 1) = phyv(l) - dragv(l) - liftv(l) |
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[644] | 170 | |
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[1992] | 171 | END DO |
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[644] | 172 | |
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| 173 | |
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[2346] | 174 | DO j = 2, nbp_lat-1 |
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[644] | 175 | |
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[1992] | 176 | ! Values at Greenwich (Periodicity) |
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[644] | 177 | |
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[2346] | 178 | zs(nbp_lon+1, j) = phis(l+1)/rg |
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| 179 | ps(nbp_lon+1, j) = p(l+1, 1) |
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| 180 | ssou(nbp_lon+1, j) = dragu(l+1) + liftu(l+1) |
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| 181 | ssov(nbp_lon+1, j) = dragv(l+1) + liftv(l+1) |
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| 182 | blsu(nbp_lon+1, j) = phyu(l+1) - dragu(l+1) - liftu(l+1) |
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| 183 | blsv(nbp_lon+1, j) = phyv(l+1) - dragv(l+1) - liftv(l+1) |
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| 184 | zlon(nbp_lon+1) = -plon(l+1)*xpi/180. |
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[1992] | 185 | zlat(j) = plat(l+1)*xpi/180. |
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[644] | 186 | |
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[2346] | 187 | ub(nbp_lon+1, j) = 0. |
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| 188 | vb(nbp_lon+1, j) = 0. |
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[1992] | 189 | DO k = 1, nlev |
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[2346] | 190 | ub(nbp_lon+1, j) = ub(nbp_lon+1, j) + u(l+1, k)*(p(l+1,k)-p(l+1,k+1))/rg |
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| 191 | vb(nbp_lon+1, j) = vb(nbp_lon+1, j) + v(l+1, k)*(p(l+1,k)-p(l+1,k+1))/rg |
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[1992] | 192 | END DO |
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[644] | 193 | |
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| 194 | |
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[2346] | 195 | DO i = 1, nbp_lon |
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[644] | 196 | |
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[1992] | 197 | l = l + 1 |
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| 198 | zs(i, j) = phis(l)/rg |
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| 199 | ps(i, j) = p(l, 1) |
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| 200 | ssou(i, j) = dragu(l) + liftu(l) |
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| 201 | ssov(i, j) = dragv(l) + liftv(l) |
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| 202 | blsu(i, j) = phyu(l) - dragu(l) - liftu(l) |
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| 203 | blsv(i, j) = phyv(l) - dragv(l) - liftv(l) |
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| 204 | zlon(i) = plon(l)*xpi/180. |
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[644] | 205 | |
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[1992] | 206 | ub(i, j) = 0. |
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| 207 | vb(i, j) = 0. |
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| 208 | DO k = 1, nlev |
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| 209 | ub(i, j) = ub(i, j) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 210 | vb(i, j) = vb(i, j) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 211 | END DO |
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[644] | 212 | |
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[1992] | 213 | END DO |
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[644] | 214 | |
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[1992] | 215 | END DO |
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[644] | 216 | |
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| 217 | |
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[1992] | 218 | ! South Pole |
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[644] | 219 | |
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[2346] | 220 | IF (nbp_lat-1>1) THEN |
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[1992] | 221 | l = l + 1 |
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[2346] | 222 | ub(1, nbp_lat) = 0. |
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| 223 | vb(1, nbp_lat) = 0. |
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[1992] | 224 | DO k = 1, nlev |
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[2346] | 225 | ub(1, nbp_lat) = ub(1, nbp_lat) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 226 | vb(1, nbp_lat) = vb(1, nbp_lat) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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[1992] | 227 | END DO |
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[2346] | 228 | zlat(nbp_lat) = plat(l)*xpi/180. |
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[644] | 229 | |
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[2346] | 230 | DO i = 1, nbp_lon + 1 |
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| 231 | zs(i, nbp_lat) = phis(l)/rg |
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| 232 | ps(i, nbp_lat) = p(l, 1) |
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| 233 | ssou(i, nbp_lat) = dragu(l) + liftu(l) |
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| 234 | ssov(i, nbp_lat) = dragv(l) + liftv(l) |
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| 235 | blsu(i, nbp_lat) = phyu(l) - dragu(l) - liftu(l) |
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| 236 | blsv(i, nbp_lat) = phyv(l) - dragv(l) - liftv(l) |
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| 237 | ub(i, nbp_lat) = ub(1, nbp_lat) |
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| 238 | vb(i, nbp_lat) = vb(1, nbp_lat) |
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[1992] | 239 | END DO |
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| 240 | END IF |
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[644] | 241 | |
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| 242 | |
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[1992] | 243 | ! MOMENT ANGULAIRE |
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[644] | 244 | |
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[2346] | 245 | DO j = 1, nbp_lat-1 |
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| 246 | DO i = 1, nbp_lon |
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[1992] | 247 | |
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| 248 | raam(1) = raam(1) - rea**3*dlon*dlat*0.5*(cos(zlon(i))*sin(zlat(j))*cos & |
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| 249 | (zlat(j))*ub(i,j)+cos(zlon(i))*sin(zlat(j+1))*cos(zlat(j+ & |
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| 250 | 1))*ub(i,j+1)) + rea**3*dlon*dlat*0.5*(sin(zlon(i))*cos(zlat(j))*vb(i & |
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| 251 | ,j)+sin(zlon(i))*cos(zlat(j+1))*vb(i,j+1)) |
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| 252 | |
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| 253 | oaam(1) = oaam(1) - ome*rea**4*dlon*dlat/rg*0.5*(cos(zlon(i))*cos(zlat( & |
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| 254 | j))**2*sin(zlat(j))*ps(i,j)+cos(zlon(i))*cos(zlat(j+ & |
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| 255 | 1))**2*sin(zlat(j+1))*ps(i,j+1)) |
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| 256 | |
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| 257 | raam(2) = raam(2) - rea**3*dlon*dlat*0.5*(sin(zlon(i))*sin(zlat(j))*cos & |
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| 258 | (zlat(j))*ub(i,j)+sin(zlon(i))*sin(zlat(j+1))*cos(zlat(j+ & |
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| 259 | 1))*ub(i,j+1)) - rea**3*dlon*dlat*0.5*(cos(zlon(i))*cos(zlat(j))*vb(i & |
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| 260 | ,j)+cos(zlon(i))*cos(zlat(j+1))*vb(i,j+1)) |
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| 261 | |
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| 262 | oaam(2) = oaam(2) - ome*rea**4*dlon*dlat/rg*0.5*(sin(zlon(i))*cos(zlat( & |
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| 263 | j))**2*sin(zlat(j))*ps(i,j)+sin(zlon(i))*cos(zlat(j+ & |
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| 264 | 1))**2*sin(zlat(j+1))*ps(i,j+1)) |
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| 265 | |
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| 266 | raam(3) = raam(3) + rea**3*dlon*dlat*0.5*(cos(zlat(j))**2*ub(i,j)+cos( & |
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| 267 | zlat(j+1))**2*ub(i,j+1)) |
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| 268 | |
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| 269 | oaam(3) = oaam(3) + ome*rea**4*dlon*dlat/rg*0.5*(cos(zlat(j))**3*ps(i,j & |
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| 270 | )+cos(zlat(j+1))**3*ps(i,j+1)) |
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| 271 | |
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| 272 | END DO |
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| 273 | END DO |
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| 274 | |
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| 275 | |
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| 276 | ! COUPLE DES MONTAGNES: |
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| 277 | |
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| 278 | |
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[2346] | 279 | DO j = 1, nbp_lat-1 |
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| 280 | DO i = 1, nbp_lon |
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[1992] | 281 | tmou(1) = tmou(1) - rea**2*dlon*0.5*sin(zlon(i))*(zs(i,j)-zs(i,j+1))*( & |
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| 282 | cos(zlat(j+1))*ps(i,j+1)+cos(zlat(j))*ps(i,j)) |
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| 283 | tmou(2) = tmou(2) + rea**2*dlon*0.5*cos(zlon(i))*(zs(i,j)-zs(i,j+1))*( & |
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| 284 | cos(zlat(j+1))*ps(i,j+1)+cos(zlat(j))*ps(i,j)) |
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| 285 | END DO |
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| 286 | END DO |
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| 287 | |
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[2346] | 288 | DO j = 2, nbp_lat-1 |
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| 289 | DO i = 1, nbp_lon |
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[1992] | 290 | tmou(1) = tmou(1) + rea**2*dlat*0.5*sin(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 291 | cos(zlon(i+1))*ps(i+1,j)+cos(zlon(i))*ps(i,j)) |
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| 292 | tmou(2) = tmou(2) + rea**2*dlat*0.5*sin(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 293 | sin(zlon(i+1))*ps(i+1,j)+sin(zlon(i))*ps(i,j)) |
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| 294 | tmou(3) = tmou(3) - rea**2*dlat*0.5*cos(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 295 | ps(i+1,j)+ps(i,j)) |
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| 296 | END DO |
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| 297 | END DO |
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| 298 | |
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| 299 | |
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| 300 | ! COUPLES DES DIFFERENTES FRICTION AU SOL: |
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| 301 | |
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| 302 | l = 1 |
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[2346] | 303 | DO j = 2, nbp_lat-1 |
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| 304 | DO i = 1, nbp_lon |
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[1992] | 305 | l = l + 1 |
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| 306 | tsso(1) = tsso(1) - rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*sin(zlat(j & |
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| 307 | ))*cos(zlon(i)) + rea**3*cos(zlat(j))*dlon*dlat*ssov(i, j)*sin(zlon(i & |
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| 308 | )) |
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| 309 | |
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| 310 | tsso(2) = tsso(2) - rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*sin(zlat(j & |
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| 311 | ))*sin(zlon(i)) - rea**3*cos(zlat(j))*dlon*dlat*ssov(i, j)*cos(zlon(i & |
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| 312 | )) |
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| 313 | |
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| 314 | tsso(3) = tsso(3) + rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*cos(zlat(j & |
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| 315 | )) |
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| 316 | |
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| 317 | tbls(1) = tbls(1) - rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*sin(zlat(j & |
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| 318 | ))*cos(zlon(i)) + rea**3*cos(zlat(j))*dlon*dlat*blsv(i, j)*sin(zlon(i & |
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| 319 | )) |
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| 320 | |
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| 321 | tbls(2) = tbls(2) - rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*sin(zlat(j & |
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| 322 | ))*sin(zlon(i)) - rea**3*cos(zlat(j))*dlon*dlat*blsv(i, j)*cos(zlon(i & |
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| 323 | )) |
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| 324 | |
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| 325 | tbls(3) = tbls(3) + rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*cos(zlat(j & |
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| 326 | )) |
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| 327 | |
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| 328 | END DO |
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| 329 | END DO |
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| 330 | |
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| 331 | |
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[5116] | 332 | ! WRITE(*,*) 'AAM',rsec, |
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| 333 | ! WRITE(*,*) 'AAM',rjour+rsec/86400., |
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[1992] | 334 | ! c raam(3)/hadday,oaam(3)/hadday, |
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| 335 | ! c tmou(3)/hadley,tsso(3)/hadley,tbls(3)/hadley |
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| 336 | |
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[5116] | 337 | ! WRITE(iam,100)rjour+rsec/86400., |
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[1992] | 338 | ! c raam(1)/hadday,oaam(1)/hadday, |
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| 339 | ! c tmou(1)/hadley,tsso(1)/hadley,tbls(1)/hadley, |
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| 340 | ! c raam(2)/hadday,oaam(2)/hadday, |
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| 341 | ! c tmou(2)/hadley,tsso(2)/hadley,tbls(2)/hadley, |
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| 342 | ! c raam(3)/hadday,oaam(3)/hadday, |
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| 343 | ! c tmou(3)/hadley,tsso(3)/hadley,tbls(3)/hadley |
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| 344 | 100 FORMAT (F12.5, 15(1X,F12.5)) |
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| 345 | |
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[5116] | 346 | ! WRITE(iam+1,*)((zs(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 347 | ! WRITE(iam+1,*)((ps(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 348 | ! WRITE(iam+1,*)((ub(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 349 | ! WRITE(iam+1,*)((vb(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 350 | ! WRITE(iam+1,*)((ssou(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 351 | ! WRITE(iam+1,*)((ssov(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 352 | ! WRITE(iam+1,*)((blsu(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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| 353 | ! WRITE(iam+1,*)((blsv(i,j),i=1,nbp_lon),j=1,nbp_lat) |
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[1992] | 354 | |
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| 355 | aam = raam(3) |
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| 356 | torsfc = tmou(3) + tsso(3) + tbls(3) |
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| 357 | |
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[5105] | 358 | |
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[1992] | 359 | END SUBROUTINE aaam_bud |
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