[1992] | 1 | |
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[1403] | 2 | ! $Id: aaam_bud.F90 1992 2014-03-05 13:19:12Z fhourdin $ |
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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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| 8 | IMPLICIT NONE |
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| 9 | ! ====================================================================== |
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| 10 | ! Auteur(s): F.Lott (LMD/CNRS) date: 20031020 |
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| 11 | ! Object: Compute different terms of the axial AAAM Budget. |
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| 12 | ! No outputs, every AAM quantities are written on the IAM |
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| 13 | ! File. |
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[1403] | 14 | |
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[1992] | 15 | ! Modif : I.Musat (LMD/CNRS) date : 20041020 |
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| 16 | ! Outputs : axial components of wind AAM "aam" and total surface torque |
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| 17 | ! "torsfc", |
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| 18 | ! but no write in the iam file. |
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[1403] | 19 | |
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[1992] | 20 | ! WARNING: Only valid for regular rectangular grids. |
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| 21 | ! REMARK: CALL DANS PHYSIQ AFTER lift_noro: |
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| 22 | ! CALL aaam_bud (27,klon,klev,rjourvrai,gmtime, |
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| 23 | ! C ra,rg,romega, |
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| 24 | ! C rlat,rlon,pphis, |
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| 25 | ! C zustrdr,zustrli,zustrph, |
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| 26 | ! C zvstrdr,zvstrli,zvstrph, |
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| 27 | ! C paprs,u,v) |
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[1403] | 28 | |
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[1992] | 29 | ! ====================================================================== |
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| 30 | ! Explicit Arguments: |
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| 31 | ! ================== |
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| 32 | ! iam-----input-I-File number where AAMs and torques are written |
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| 33 | ! It is a formatted file that has been opened |
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| 34 | ! in physiq.F |
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| 35 | ! nlon----input-I-Total number of horizontal points that get into physics |
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| 36 | ! nlev----input-I-Number of vertical levels |
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| 37 | ! rjour -R-Jour compte depuis le debut de la simu (run.def) |
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| 38 | ! rsec -R-Seconde de la journee |
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| 39 | ! rea -R-Earth radius |
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| 40 | ! rg -R-gravity constant |
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| 41 | ! ome -R-Earth rotation rate |
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| 42 | ! plat ---input-R-Latitude en degres |
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| 43 | ! plon ---input-R-Longitude en degres |
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| 44 | ! phis ---input-R-Geopotential at the ground |
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| 45 | ! dragu---input-R-orodrag stress (zonal) |
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| 46 | ! liftu---input-R-orolift stress (zonal) |
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| 47 | ! phyu----input-R-Stress total de la physique (zonal) |
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| 48 | ! dragv---input-R-orodrag stress (Meridional) |
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| 49 | ! liftv---input-R-orolift stress (Meridional) |
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| 50 | ! phyv----input-R-Stress total de la physique (Meridional) |
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| 51 | ! p-------input-R-Pressure (Pa) at model half levels |
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| 52 | ! u-------input-R-Horizontal wind (m/s) |
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| 53 | ! v-------input-R-Meridional wind (m/s) |
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| 54 | ! aam-----output-R-Axial Wind AAM (=raam(3)) |
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| 55 | ! torsfc--output-R-Total surface torque (=tmou(3)+tsso(3)+tbls(3)) |
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[644] | 56 | |
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[1992] | 57 | ! Implicit Arguments: |
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| 58 | ! =================== |
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[644] | 59 | |
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[1992] | 60 | ! iim--common-I: Number of longitude intervals |
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| 61 | ! jjm--common-I: Number of latitude intervals |
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| 62 | ! klon-common-I: Number of points seen by the physics |
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| 63 | ! iim*(jjm-1)+2 for instance |
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| 64 | ! klev-common-I: Number of vertical layers |
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| 65 | ! ====================================================================== |
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| 66 | ! Local Variables: |
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| 67 | ! ================ |
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| 68 | ! dlat-----R: Latitude increment (Radians) |
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| 69 | ! dlon-----R: Longitude increment (Radians) |
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| 70 | ! raam ---R: Wind AAM (3 Components, 1 & 2 Equatoriales; 3 Axiale) |
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| 71 | ! oaam ---R: Mass AAM (3 Components, 1 & 2 Equatoriales; 3 Axiale) |
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| 72 | ! tmou-----R: Resolved Mountain torque (3 components) |
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| 73 | ! tsso-----R: Parameterised Moutain drag torque (3 components) |
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| 74 | ! tbls-----R: Parameterised Boundary layer torque (3 components) |
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[644] | 75 | |
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[1992] | 76 | ! LOCAL ARRAY: |
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| 77 | ! =========== |
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| 78 | ! zs ---R: Topographic height |
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| 79 | ! ps ---R: Surface Pressure |
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| 80 | ! ub ---R: Barotropic wind zonal |
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| 81 | ! vb ---R: Barotropic wind meridional |
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| 82 | ! zlat ---R: Latitude in radians |
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| 83 | ! zlon ---R: Longitude in radians |
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| 84 | ! ====================================================================== |
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[644] | 85 | |
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[1992] | 86 | include "dimensions.h" |
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| 87 | ! cc#include "dimphy.h" |
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[644] | 88 | |
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[1992] | 89 | ! ARGUMENTS |
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[644] | 90 | |
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[1992] | 91 | INTEGER iam, nlon, nlev |
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| 92 | REAL, INTENT (IN) :: rjour, rsec, rea, rg, ome |
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| 93 | REAL plat(nlon), plon(nlon), phis(nlon) |
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| 94 | REAL dragu(nlon), liftu(nlon), phyu(nlon) |
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| 95 | REAL dragv(nlon), liftv(nlon), phyv(nlon) |
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| 96 | REAL p(nlon, nlev+1), u(nlon, nlev), v(nlon, nlev) |
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[644] | 97 | |
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[1992] | 98 | ! Variables locales: |
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[644] | 99 | |
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[1992] | 100 | INTEGER i, j, k, l |
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| 101 | REAL xpi, hadley, hadday |
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| 102 | REAL dlat, dlon |
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| 103 | REAL raam(3), oaam(3), tmou(3), tsso(3), tbls(3) |
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| 104 | INTEGER iax |
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| 105 | ! IM ajout aam, torsfc |
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| 106 | ! aam = composante axiale du Wind AAM raam |
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| 107 | ! torsfc = composante axiale de (tmou+tsso+tbls) |
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| 108 | REAL aam, torsfc |
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[644] | 109 | |
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[1992] | 110 | REAL zs(801, 401), ps(801, 401) |
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| 111 | REAL ub(801, 401), vb(801, 401) |
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| 112 | REAL ssou(801, 401), ssov(801, 401) |
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| 113 | REAL blsu(801, 401), blsv(801, 401) |
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| 114 | REAL zlon(801), zlat(401) |
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[644] | 115 | |
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[1992] | 116 | CHARACTER (LEN=20) :: modname = 'aaam_bud' |
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| 117 | CHARACTER (LEN=80) :: abort_message |
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[644] | 118 | |
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| 119 | |
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| 120 | |
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[1992] | 121 | ! PUT AAM QUANTITIES AT ZERO: |
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[644] | 122 | |
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[1992] | 123 | IF (iim+1>801 .OR. jjm+1>401) THEN |
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| 124 | abort_message = 'Pb de dimension dans aaam_bud' |
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| 125 | CALL abort_gcm(modname, abort_message, 1) |
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| 126 | END IF |
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[644] | 127 | |
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[1992] | 128 | xpi = acos(-1.) |
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| 129 | hadley = 1.E18 |
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| 130 | hadday = 1.E18*24.*3600. |
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| 131 | dlat = xpi/real(jjm) |
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| 132 | dlon = 2.*xpi/real(iim) |
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[644] | 133 | |
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[1992] | 134 | DO iax = 1, 3 |
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| 135 | oaam(iax) = 0. |
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| 136 | raam(iax) = 0. |
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| 137 | tmou(iax) = 0. |
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| 138 | tsso(iax) = 0. |
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| 139 | tbls(iax) = 0. |
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| 140 | END DO |
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[644] | 141 | |
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[1992] | 142 | ! MOUNTAIN HEIGHT, PRESSURE AND BAROTROPIC WIND: |
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[644] | 143 | |
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[1992] | 144 | ! North pole values (j=1): |
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[644] | 145 | |
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[1992] | 146 | l = 1 |
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[644] | 147 | |
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[1992] | 148 | ub(1, 1) = 0. |
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| 149 | vb(1, 1) = 0. |
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| 150 | DO k = 1, nlev |
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| 151 | ub(1, 1) = ub(1, 1) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 152 | vb(1, 1) = vb(1, 1) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 153 | END DO |
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[644] | 154 | |
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[1992] | 155 | zlat(1) = plat(l)*xpi/180. |
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[644] | 156 | |
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[1992] | 157 | DO i = 1, iim + 1 |
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[644] | 158 | |
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[1992] | 159 | zs(i, 1) = phis(l)/rg |
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| 160 | ps(i, 1) = p(l, 1) |
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| 161 | ub(i, 1) = ub(1, 1) |
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| 162 | vb(i, 1) = vb(1, 1) |
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| 163 | ssou(i, 1) = dragu(l) + liftu(l) |
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| 164 | ssov(i, 1) = dragv(l) + liftv(l) |
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| 165 | blsu(i, 1) = phyu(l) - dragu(l) - liftu(l) |
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| 166 | blsv(i, 1) = phyv(l) - dragv(l) - liftv(l) |
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[644] | 167 | |
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[1992] | 168 | END DO |
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[644] | 169 | |
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| 170 | |
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[1992] | 171 | DO j = 2, jjm |
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[644] | 172 | |
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[1992] | 173 | ! Values at Greenwich (Periodicity) |
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[644] | 174 | |
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[1992] | 175 | zs(iim+1, j) = phis(l+1)/rg |
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| 176 | ps(iim+1, j) = p(l+1, 1) |
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| 177 | ssou(iim+1, j) = dragu(l+1) + liftu(l+1) |
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| 178 | ssov(iim+1, j) = dragv(l+1) + liftv(l+1) |
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| 179 | blsu(iim+1, j) = phyu(l+1) - dragu(l+1) - liftu(l+1) |
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| 180 | blsv(iim+1, j) = phyv(l+1) - dragv(l+1) - liftv(l+1) |
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| 181 | zlon(iim+1) = -plon(l+1)*xpi/180. |
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| 182 | zlat(j) = plat(l+1)*xpi/180. |
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[644] | 183 | |
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[1992] | 184 | ub(iim+1, j) = 0. |
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| 185 | vb(iim+1, j) = 0. |
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| 186 | DO k = 1, nlev |
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| 187 | ub(iim+1, j) = ub(iim+1, j) + u(l+1, k)*(p(l+1,k)-p(l+1,k+1))/rg |
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| 188 | vb(iim+1, j) = vb(iim+1, j) + v(l+1, k)*(p(l+1,k)-p(l+1,k+1))/rg |
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| 189 | END DO |
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[644] | 190 | |
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| 191 | |
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[1992] | 192 | DO i = 1, iim |
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[644] | 193 | |
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[1992] | 194 | l = l + 1 |
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| 195 | zs(i, j) = phis(l)/rg |
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| 196 | ps(i, j) = p(l, 1) |
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| 197 | ssou(i, j) = dragu(l) + liftu(l) |
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| 198 | ssov(i, j) = dragv(l) + liftv(l) |
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| 199 | blsu(i, j) = phyu(l) - dragu(l) - liftu(l) |
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| 200 | blsv(i, j) = phyv(l) - dragv(l) - liftv(l) |
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| 201 | zlon(i) = plon(l)*xpi/180. |
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[644] | 202 | |
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[1992] | 203 | ub(i, j) = 0. |
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| 204 | vb(i, j) = 0. |
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| 205 | DO k = 1, nlev |
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| 206 | ub(i, j) = ub(i, j) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 207 | vb(i, j) = vb(i, j) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 208 | END DO |
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[644] | 209 | |
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[1992] | 210 | END DO |
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[644] | 211 | |
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[1992] | 212 | END DO |
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[644] | 213 | |
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| 214 | |
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[1992] | 215 | ! South Pole |
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[644] | 216 | |
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[1992] | 217 | IF (jjm>1) THEN |
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| 218 | l = l + 1 |
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| 219 | ub(1, jjm+1) = 0. |
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| 220 | vb(1, jjm+1) = 0. |
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| 221 | DO k = 1, nlev |
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| 222 | ub(1, jjm+1) = ub(1, jjm+1) + u(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 223 | vb(1, jjm+1) = vb(1, jjm+1) + v(l, k)*(p(l,k)-p(l,k+1))/rg |
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| 224 | END DO |
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| 225 | zlat(jjm+1) = plat(l)*xpi/180. |
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[644] | 226 | |
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[1992] | 227 | DO i = 1, iim + 1 |
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| 228 | zs(i, jjm+1) = phis(l)/rg |
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| 229 | ps(i, jjm+1) = p(l, 1) |
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| 230 | ssou(i, jjm+1) = dragu(l) + liftu(l) |
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| 231 | ssov(i, jjm+1) = dragv(l) + liftv(l) |
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| 232 | blsu(i, jjm+1) = phyu(l) - dragu(l) - liftu(l) |
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| 233 | blsv(i, jjm+1) = phyv(l) - dragv(l) - liftv(l) |
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| 234 | ub(i, jjm+1) = ub(1, jjm+1) |
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| 235 | vb(i, jjm+1) = vb(1, jjm+1) |
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| 236 | END DO |
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| 237 | END IF |
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[644] | 238 | |
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| 239 | |
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[1992] | 240 | ! MOMENT ANGULAIRE |
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[644] | 241 | |
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[1992] | 242 | DO j = 1, jjm |
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| 243 | DO i = 1, iim |
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| 244 | |
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| 245 | raam(1) = raam(1) - rea**3*dlon*dlat*0.5*(cos(zlon(i))*sin(zlat(j))*cos & |
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| 246 | (zlat(j))*ub(i,j)+cos(zlon(i))*sin(zlat(j+1))*cos(zlat(j+ & |
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| 247 | 1))*ub(i,j+1)) + rea**3*dlon*dlat*0.5*(sin(zlon(i))*cos(zlat(j))*vb(i & |
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| 248 | ,j)+sin(zlon(i))*cos(zlat(j+1))*vb(i,j+1)) |
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| 249 | |
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| 250 | oaam(1) = oaam(1) - ome*rea**4*dlon*dlat/rg*0.5*(cos(zlon(i))*cos(zlat( & |
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| 251 | j))**2*sin(zlat(j))*ps(i,j)+cos(zlon(i))*cos(zlat(j+ & |
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| 252 | 1))**2*sin(zlat(j+1))*ps(i,j+1)) |
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| 253 | |
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| 254 | raam(2) = raam(2) - rea**3*dlon*dlat*0.5*(sin(zlon(i))*sin(zlat(j))*cos & |
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| 255 | (zlat(j))*ub(i,j)+sin(zlon(i))*sin(zlat(j+1))*cos(zlat(j+ & |
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| 256 | 1))*ub(i,j+1)) - rea**3*dlon*dlat*0.5*(cos(zlon(i))*cos(zlat(j))*vb(i & |
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| 257 | ,j)+cos(zlon(i))*cos(zlat(j+1))*vb(i,j+1)) |
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| 258 | |
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| 259 | oaam(2) = oaam(2) - ome*rea**4*dlon*dlat/rg*0.5*(sin(zlon(i))*cos(zlat( & |
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| 260 | j))**2*sin(zlat(j))*ps(i,j)+sin(zlon(i))*cos(zlat(j+ & |
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| 261 | 1))**2*sin(zlat(j+1))*ps(i,j+1)) |
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| 262 | |
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| 263 | raam(3) = raam(3) + rea**3*dlon*dlat*0.5*(cos(zlat(j))**2*ub(i,j)+cos( & |
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| 264 | zlat(j+1))**2*ub(i,j+1)) |
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| 265 | |
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| 266 | oaam(3) = oaam(3) + ome*rea**4*dlon*dlat/rg*0.5*(cos(zlat(j))**3*ps(i,j & |
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| 267 | )+cos(zlat(j+1))**3*ps(i,j+1)) |
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| 268 | |
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| 269 | END DO |
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| 270 | END DO |
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| 271 | |
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| 272 | |
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| 273 | ! COUPLE DES MONTAGNES: |
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| 274 | |
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| 275 | |
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| 276 | DO j = 1, jjm |
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| 277 | DO i = 1, iim |
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| 278 | tmou(1) = tmou(1) - rea**2*dlon*0.5*sin(zlon(i))*(zs(i,j)-zs(i,j+1))*( & |
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| 279 | cos(zlat(j+1))*ps(i,j+1)+cos(zlat(j))*ps(i,j)) |
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| 280 | tmou(2) = tmou(2) + rea**2*dlon*0.5*cos(zlon(i))*(zs(i,j)-zs(i,j+1))*( & |
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| 281 | cos(zlat(j+1))*ps(i,j+1)+cos(zlat(j))*ps(i,j)) |
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| 282 | END DO |
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| 283 | END DO |
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| 284 | |
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| 285 | DO j = 2, jjm |
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| 286 | DO i = 1, iim |
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| 287 | tmou(1) = tmou(1) + rea**2*dlat*0.5*sin(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 288 | cos(zlon(i+1))*ps(i+1,j)+cos(zlon(i))*ps(i,j)) |
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| 289 | tmou(2) = tmou(2) + rea**2*dlat*0.5*sin(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 290 | sin(zlon(i+1))*ps(i+1,j)+sin(zlon(i))*ps(i,j)) |
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| 291 | tmou(3) = tmou(3) - rea**2*dlat*0.5*cos(zlat(j))*(zs(i+1,j)-zs(i,j))*( & |
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| 292 | ps(i+1,j)+ps(i,j)) |
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| 293 | END DO |
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| 294 | END DO |
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| 295 | |
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| 296 | |
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| 297 | ! COUPLES DES DIFFERENTES FRICTION AU SOL: |
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| 298 | |
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| 299 | l = 1 |
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| 300 | DO j = 2, jjm |
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| 301 | DO i = 1, iim |
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| 302 | l = l + 1 |
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| 303 | tsso(1) = tsso(1) - rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*sin(zlat(j & |
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| 304 | ))*cos(zlon(i)) + rea**3*cos(zlat(j))*dlon*dlat*ssov(i, j)*sin(zlon(i & |
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| 305 | )) |
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| 306 | |
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| 307 | tsso(2) = tsso(2) - rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*sin(zlat(j & |
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| 308 | ))*sin(zlon(i)) - rea**3*cos(zlat(j))*dlon*dlat*ssov(i, j)*cos(zlon(i & |
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| 309 | )) |
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| 310 | |
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| 311 | tsso(3) = tsso(3) + rea**3*cos(zlat(j))*dlon*dlat*ssou(i, j)*cos(zlat(j & |
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| 312 | )) |
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| 313 | |
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| 314 | tbls(1) = tbls(1) - rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*sin(zlat(j & |
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| 315 | ))*cos(zlon(i)) + rea**3*cos(zlat(j))*dlon*dlat*blsv(i, j)*sin(zlon(i & |
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| 316 | )) |
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| 317 | |
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| 318 | tbls(2) = tbls(2) - rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*sin(zlat(j & |
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| 319 | ))*sin(zlon(i)) - rea**3*cos(zlat(j))*dlon*dlat*blsv(i, j)*cos(zlon(i & |
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| 320 | )) |
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| 321 | |
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| 322 | tbls(3) = tbls(3) + rea**3*cos(zlat(j))*dlon*dlat*blsu(i, j)*cos(zlat(j & |
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| 323 | )) |
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| 324 | |
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| 325 | END DO |
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| 326 | END DO |
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| 327 | |
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| 328 | |
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| 329 | ! write(*,*) 'AAM',rsec, |
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| 330 | ! write(*,*) 'AAM',rjour+rsec/86400., |
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| 331 | ! c raam(3)/hadday,oaam(3)/hadday, |
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| 332 | ! c tmou(3)/hadley,tsso(3)/hadley,tbls(3)/hadley |
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| 333 | |
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| 334 | ! write(iam,100)rjour+rsec/86400., |
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| 335 | ! c raam(1)/hadday,oaam(1)/hadday, |
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| 336 | ! c tmou(1)/hadley,tsso(1)/hadley,tbls(1)/hadley, |
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| 337 | ! c raam(2)/hadday,oaam(2)/hadday, |
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| 338 | ! c tmou(2)/hadley,tsso(2)/hadley,tbls(2)/hadley, |
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| 339 | ! c raam(3)/hadday,oaam(3)/hadday, |
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| 340 | ! c tmou(3)/hadley,tsso(3)/hadley,tbls(3)/hadley |
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| 341 | 100 FORMAT (F12.5, 15(1X,F12.5)) |
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| 342 | |
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| 343 | ! write(iam+1,*)((zs(i,j),i=1,iim),j=1,jjm+1) |
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| 344 | ! write(iam+1,*)((ps(i,j),i=1,iim),j=1,jjm+1) |
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| 345 | ! write(iam+1,*)((ub(i,j),i=1,iim),j=1,jjm+1) |
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| 346 | ! write(iam+1,*)((vb(i,j),i=1,iim),j=1,jjm+1) |
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| 347 | ! write(iam+1,*)((ssou(i,j),i=1,iim),j=1,jjm+1) |
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| 348 | ! write(iam+1,*)((ssov(i,j),i=1,iim),j=1,jjm+1) |
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| 349 | ! write(iam+1,*)((blsu(i,j),i=1,iim),j=1,jjm+1) |
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| 350 | ! write(iam+1,*)((blsv(i,j),i=1,iim),j=1,jjm+1) |
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| 351 | |
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| 352 | aam = raam(3) |
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| 353 | torsfc = tmou(3) + tsso(3) + tbls(3) |
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| 354 | |
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| 355 | RETURN |
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| 356 | END SUBROUTINE aaam_bud |
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