[524] | 1 | ! |
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| 2 | ! $Header$ |
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| 3 | ! |
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| 4 | SUBROUTINE advy(limit,dty,pbarv,sm,s0,sx,sy,sz) |
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| 5 | IMPLICIT NONE |
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| 6 | |
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| 7 | CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC |
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| 8 | C C |
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| 9 | C first-order moments (SOM) advection of tracer in Y direction C |
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| 10 | C C |
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[2600] | 11 | C Source : Pascal Simon ( Meteo, CNRM ) C |
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| 12 | C Adaptation : A.A. (LGGE) C |
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[524] | 13 | C Derniere Modif : 15/12/94 LAST |
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[2600] | 14 | C C |
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| 15 | C sont les arguments d'entree pour le s-pg C |
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| 16 | C C |
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| 17 | C argument de sortie du s-pg C |
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| 18 | C C |
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[524] | 19 | CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC |
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| 20 | CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC |
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| 21 | C |
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| 22 | C Rem : Probleme aux poles il faut reecrire ce cas specifique |
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| 23 | C Attention au sens de l'indexation |
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| 24 | C |
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| 25 | C parametres principaux du modele |
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| 26 | C |
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| 27 | C |
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[2600] | 28 | include "dimensions.h" |
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| 29 | include "paramet.h" |
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| 30 | include "comgeom2.h" |
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[524] | 31 | |
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| 32 | C Arguments : |
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| 33 | C ---------- |
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| 34 | C dty : frequence fictive d'appel du transport |
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| 35 | C parbu,pbarv : flux de masse en x et y en Pa.m2.s-1 |
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| 36 | |
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| 37 | INTEGER lon,lat,niv |
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| 38 | INTEGER i,j,jv,k,kp,l |
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| 39 | INTEGER ntra |
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| 40 | PARAMETER (ntra = 1) |
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| 41 | |
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| 42 | REAL dty |
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| 43 | REAL pbarv ( iip1,jjm, llm ) |
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| 44 | |
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| 45 | C moments: SM total mass in each grid box |
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| 46 | C S0 mass of tracer in each grid box |
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| 47 | C Si 1rst order moment in i direction |
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| 48 | C |
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| 49 | REAL SM(iip1,jjp1,llm) |
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| 50 | + ,S0(iip1,jjp1,llm,ntra) |
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| 51 | REAL sx(iip1,jjp1,llm,ntra) |
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| 52 | + ,sy(iip1,jjp1,llm,ntra) |
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| 53 | + ,sz(iip1,jjp1,llm,ntra) |
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| 54 | |
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| 55 | |
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| 56 | C Local : |
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| 57 | C ------- |
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| 58 | |
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| 59 | C mass fluxes across the boundaries (UGRI,VGRI,WGRI) |
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| 60 | C mass fluxes in kg |
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| 61 | C declaration : |
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| 62 | |
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| 63 | REAL VGRI(iip1,0:jjp1,llm) |
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| 64 | |
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| 65 | C Rem : UGRI et WGRI ne sont pas utilises dans |
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| 66 | C cette subroutine ( advection en y uniquement ) |
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| 67 | C Rem 2 :le dimensionnement de VGRI depend de celui de pbarv |
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| 68 | C |
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| 69 | C the moments F are similarly defined and used as temporary |
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| 70 | C storage for portions of the grid boxes in transit |
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| 71 | C |
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| 72 | REAL F0(iim,0:jjp1,ntra),FM(iim,0:jjp1) |
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| 73 | REAL FX(iim,jjm,ntra),FY(iim,jjm,ntra) |
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| 74 | REAL FZ(iim,jjm,ntra) |
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| 75 | REAL S00(ntra) |
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| 76 | REAL SM0 ! Just temporal variable |
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| 77 | C |
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| 78 | C work arrays |
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| 79 | C |
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| 80 | REAL ALF(iim,0:jjp1),ALF1(iim,0:jjp1) |
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| 81 | REAL ALFQ(iim,0:jjp1),ALF1Q(iim,0:jjp1) |
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| 82 | REAL TEMPTM ! Just temporal variable |
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| 83 | c |
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| 84 | C Special pour poles |
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| 85 | c |
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| 86 | REAL sbms,sfms,sfzs,sbmn,sfmn,sfzn |
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| 87 | REAL sns0(ntra),snsz(ntra),snsm |
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| 88 | REAL s1v(llm),slatv(llm) |
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| 89 | REAL qy1(iim,llm,ntra),qylat(iim,llm,ntra) |
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| 90 | REAL cx1(llm,ntra), cxLAT(llm,ntra) |
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| 91 | REAL cy1(llm,ntra), cyLAT(llm,ntra) |
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| 92 | REAL z1(iim), zcos(iim), zsin(iim) |
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| 93 | real smpn,smps,s0pn,s0ps |
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| 94 | REAL SSUM |
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| 95 | EXTERNAL SSUM |
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| 96 | C |
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| 97 | REAL sqi,sqf |
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| 98 | LOGICAL LIMIT |
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| 99 | |
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| 100 | lon = iim ! rem : Il est possible qu'un pbl. arrive ici |
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| 101 | lat = jjp1 ! a cause des dim. differentes entre les |
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| 102 | niv=llm |
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| 103 | |
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| 104 | C |
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| 105 | C the moments Fi are used as temporary storage for |
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| 106 | C portions of the grid boxes in transit at the current level |
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| 107 | C |
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| 108 | C work arrays |
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| 109 | C |
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| 110 | |
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| 111 | DO l = 1,llm |
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| 112 | DO j = 1,jjm |
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| 113 | DO i = 1,iip1 |
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| 114 | vgri (i,j,llm+1-l)=-1.*pbarv(i,j,l) |
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| 115 | enddo |
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| 116 | enddo |
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| 117 | do i=1,iip1 |
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| 118 | vgri(i,0,l) = 0. |
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| 119 | vgri(i,jjp1,l) = 0. |
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| 120 | enddo |
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| 121 | enddo |
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| 122 | |
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| 123 | DO 1 L=1,NIV |
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| 124 | C |
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| 125 | C place limits on appropriate moments before transport |
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| 126 | C (if flux-limiting is to be applied) |
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| 127 | C |
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| 128 | IF(.NOT.LIMIT) GO TO 11 |
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| 129 | C |
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| 130 | DO 10 JV=1,NTRA |
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| 131 | DO 10 K=1,LAT |
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| 132 | DO 100 I=1,LON |
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| 133 | sy(I,K,L,JV)=SIGN(AMIN1(AMAX1(S0(I,K,L,JV),0.), |
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| 134 | + ABS(sy(I,K,L,JV))),sy(I,K,L,JV)) |
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| 135 | 100 CONTINUE |
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| 136 | 10 CONTINUE |
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| 137 | C |
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| 138 | 11 CONTINUE |
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| 139 | C |
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| 140 | C le flux a travers le pole Nord est traite separement |
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| 141 | C |
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| 142 | SM0=0. |
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| 143 | DO 20 JV=1,NTRA |
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| 144 | S00(JV)=0. |
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| 145 | 20 CONTINUE |
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| 146 | C |
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| 147 | DO 21 I=1,LON |
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| 148 | C |
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| 149 | IF(VGRI(I,0,L).LE.0.) THEN |
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| 150 | FM(I,0)=-VGRI(I,0,L)*DTY |
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| 151 | ALF(I,0)=FM(I,0)/SM(I,1,L) |
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| 152 | SM(I,1,L)=SM(I,1,L)-FM(I,0) |
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| 153 | SM0=SM0+FM(I,0) |
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| 154 | ENDIF |
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| 155 | C |
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| 156 | ALFQ(I,0)=ALF(I,0)*ALF(I,0) |
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| 157 | ALF1(I,0)=1.-ALF(I,0) |
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| 158 | ALF1Q(I,0)=ALF1(I,0)*ALF1(I,0) |
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| 159 | C |
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| 160 | 21 CONTINUE |
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| 161 | C |
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| 162 | DO 22 JV=1,NTRA |
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| 163 | DO 220 I=1,LON |
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| 164 | C |
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| 165 | IF(VGRI(I,0,L).LE.0.) THEN |
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| 166 | C |
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| 167 | F0(I,0,JV)=ALF(I,0)* |
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| 168 | + ( S0(I,1,L,JV)-ALF1(I,0)*sy(I,1,L,JV) ) |
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| 169 | C |
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| 170 | S00(JV)=S00(JV)+F0(I,0,JV) |
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| 171 | S0(I,1,L,JV)=S0(I,1,L,JV)-F0(I,0,JV) |
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| 172 | sy(I,1,L,JV)=ALF1Q(I,0)*sy(I,1,L,JV) |
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| 173 | sx(I,1,L,JV)=ALF1 (I,0)*sx(I,1,L,JV) |
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| 174 | sz(I,1,L,JV)=ALF1 (I,0)*sz(I,1,L,JV) |
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| 175 | C |
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| 176 | ENDIF |
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| 177 | C |
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| 178 | 220 CONTINUE |
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| 179 | 22 CONTINUE |
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| 180 | C |
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| 181 | DO 23 I=1,LON |
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| 182 | IF(VGRI(I,0,L).GT.0.) THEN |
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| 183 | FM(I,0)=VGRI(I,0,L)*DTY |
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| 184 | ALF(I,0)=FM(I,0)/SM0 |
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| 185 | ENDIF |
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| 186 | 23 CONTINUE |
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| 187 | C |
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| 188 | DO 24 JV=1,NTRA |
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| 189 | DO 240 I=1,LON |
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| 190 | IF(VGRI(I,0,L).GT.0.) THEN |
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| 191 | F0(I,0,JV)=ALF(I,0)*S00(JV) |
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| 192 | ENDIF |
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| 193 | 240 CONTINUE |
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| 194 | 24 CONTINUE |
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| 195 | C |
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| 196 | C puts the temporary moments Fi into appropriate neighboring boxes |
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| 197 | C |
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| 198 | DO 25 I=1,LON |
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| 199 | C |
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| 200 | IF(VGRI(I,0,L).GT.0.) THEN |
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| 201 | SM(I,1,L)=SM(I,1,L)+FM(I,0) |
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| 202 | ALF(I,0)=FM(I,0)/SM(I,1,L) |
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| 203 | ENDIF |
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| 204 | C |
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| 205 | ALF1(I,0)=1.-ALF(I,0) |
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| 206 | C |
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| 207 | 25 CONTINUE |
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| 208 | C |
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| 209 | DO 26 JV=1,NTRA |
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| 210 | DO 260 I=1,LON |
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| 211 | C |
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| 212 | IF(VGRI(I,0,L).GT.0.) THEN |
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| 213 | C |
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| 214 | TEMPTM=ALF(I,0)*S0(I,1,L,JV)-ALF1(I,0)*F0(I,0,JV) |
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| 215 | S0(I,1,L,JV)=S0(I,1,L,JV)+F0(I,0,JV) |
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| 216 | sy(I,1,L,JV)=ALF1(I,0)*sy(I,1,L,JV)+3.*TEMPTM |
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| 217 | C |
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| 218 | ENDIF |
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| 219 | C |
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| 220 | 260 CONTINUE |
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| 221 | 26 CONTINUE |
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| 222 | C |
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| 223 | C calculate flux and moments between adjacent boxes |
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| 224 | C 1- create temporary moments/masses for partial boxes in transit |
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| 225 | C 2- reajusts moments remaining in the box |
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| 226 | C |
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| 227 | C flux from KP to K if V(K).lt.0 and from K to KP if V(K).gt.0 |
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| 228 | C |
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| 229 | DO 30 K=1,LAT-1 |
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| 230 | KP=K+1 |
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| 231 | DO 300 I=1,LON |
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| 232 | C |
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| 233 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 234 | FM(I,K)=-VGRI(I,K,L)*DTY |
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| 235 | ALF(I,K)=FM(I,K)/SM(I,KP,L) |
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| 236 | SM(I,KP,L)=SM(I,KP,L)-FM(I,K) |
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| 237 | ELSE |
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| 238 | FM(I,K)=VGRI(I,K,L)*DTY |
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| 239 | ALF(I,K)=FM(I,K)/SM(I,K,L) |
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| 240 | SM(I,K,L)=SM(I,K,L)-FM(I,K) |
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| 241 | ENDIF |
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| 242 | C |
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| 243 | ALFQ(I,K)=ALF(I,K)*ALF(I,K) |
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| 244 | ALF1(I,K)=1.-ALF(I,K) |
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| 245 | ALF1Q(I,K)=ALF1(I,K)*ALF1(I,K) |
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| 246 | C |
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| 247 | 300 CONTINUE |
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| 248 | 30 CONTINUE |
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| 249 | C |
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| 250 | DO 31 JV=1,NTRA |
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| 251 | DO 31 K=1,LAT-1 |
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| 252 | KP=K+1 |
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| 253 | DO 310 I=1,LON |
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| 254 | C |
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| 255 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 256 | C |
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| 257 | F0(I,K,JV)=ALF (I,K)* |
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| 258 | + ( S0(I,KP,L,JV)-ALF1(I,K)*sy(I,KP,L,JV) ) |
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| 259 | FY(I,K,JV)=ALFQ(I,K)*sy(I,KP,L,JV) |
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| 260 | FX(I,K,JV)=ALF (I,K)*sx(I,KP,L,JV) |
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| 261 | FZ(I,K,JV)=ALF (I,K)*sz(I,KP,L,JV) |
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| 262 | C |
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| 263 | S0(I,KP,L,JV)=S0(I,KP,L,JV)-F0(I,K,JV) |
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| 264 | sy(I,KP,L,JV)=ALF1Q(I,K)*sy(I,KP,L,JV) |
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| 265 | sx(I,KP,L,JV)=sx(I,KP,L,JV)-FX(I,K,JV) |
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| 266 | sz(I,KP,L,JV)=sz(I,KP,L,JV)-FZ(I,K,JV) |
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| 267 | C |
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| 268 | ELSE |
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| 269 | C |
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| 270 | F0(I,K,JV)=ALF (I,K)* |
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| 271 | + ( S0(I,K,L,JV)+ALF1(I,K)*sy(I,K,L,JV) ) |
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| 272 | FY(I,K,JV)=ALFQ(I,K)*sy(I,K,L,JV) |
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| 273 | FX(I,K,JV)=ALF(I,K)*sx(I,K,L,JV) |
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| 274 | FZ(I,K,JV)=ALF(I,K)*sz(I,K,L,JV) |
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| 275 | C |
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| 276 | S0(I,K,L,JV)=S0(I,K,L,JV)-F0(I,K,JV) |
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| 277 | sy(I,K,L,JV)=ALF1Q(I,K)*sy(I,K,L,JV) |
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| 278 | sx(I,K,L,JV)=sx(I,K,L,JV)-FX(I,K,JV) |
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| 279 | sz(I,K,L,JV)=sz(I,K,L,JV)-FZ(I,K,JV) |
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| 280 | C |
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| 281 | ENDIF |
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| 282 | C |
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| 283 | 310 CONTINUE |
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| 284 | 31 CONTINUE |
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| 285 | C |
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| 286 | C puts the temporary moments Fi into appropriate neighboring boxes |
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| 287 | C |
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| 288 | DO 32 K=1,LAT-1 |
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| 289 | KP=K+1 |
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| 290 | DO 320 I=1,LON |
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| 291 | C |
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| 292 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 293 | SM(I,K,L)=SM(I,K,L)+FM(I,K) |
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| 294 | ALF(I,K)=FM(I,K)/SM(I,K,L) |
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| 295 | ELSE |
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| 296 | SM(I,KP,L)=SM(I,KP,L)+FM(I,K) |
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| 297 | ALF(I,K)=FM(I,K)/SM(I,KP,L) |
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| 298 | ENDIF |
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| 299 | C |
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| 300 | ALF1(I,K)=1.-ALF(I,K) |
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| 301 | C |
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| 302 | 320 CONTINUE |
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| 303 | 32 CONTINUE |
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| 304 | C |
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| 305 | DO 33 JV=1,NTRA |
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| 306 | DO 33 K=1,LAT-1 |
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| 307 | KP=K+1 |
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| 308 | DO 330 I=1,LON |
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| 309 | C |
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| 310 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 311 | C |
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| 312 | TEMPTM=-ALF(I,K)*S0(I,K,L,JV)+ALF1(I,K)*F0(I,K,JV) |
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| 313 | S0(I,K,L,JV)=S0(I,K,L,JV)+F0(I,K,JV) |
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| 314 | sy(I,K,L,JV)=ALF(I,K)*FY(I,K,JV)+ALF1(I,K)*sy(I,K,L,JV) |
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| 315 | + +3.*TEMPTM |
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| 316 | sx(I,K,L,JV)=sx(I,K,L,JV)+FX(I,K,JV) |
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| 317 | sz(I,K,L,JV)=sz(I,K,L,JV)+FZ(I,K,JV) |
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| 318 | C |
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| 319 | ELSE |
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| 320 | C |
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| 321 | TEMPTM=ALF(I,K)*S0(I,KP,L,JV)-ALF1(I,K)*F0(I,K,JV) |
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| 322 | S0(I,KP,L,JV)=S0(I,KP,L,JV)+F0(I,K,JV) |
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| 323 | sy(I,KP,L,JV)=ALF(I,K)*FY(I,K,JV)+ALF1(I,K)*sy(I,KP,L,JV) |
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| 324 | + +3.*TEMPTM |
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| 325 | sx(I,KP,L,JV)=sx(I,KP,L,JV)+FX(I,K,JV) |
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| 326 | sz(I,KP,L,JV)=sz(I,KP,L,JV)+FZ(I,K,JV) |
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| 327 | C |
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| 328 | ENDIF |
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| 329 | C |
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| 330 | 330 CONTINUE |
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| 331 | 33 CONTINUE |
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| 332 | C |
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| 333 | C traitement special pour le pole Sud (idem pole Nord) |
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| 334 | C |
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| 335 | K=LAT |
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| 336 | C |
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| 337 | SM0=0. |
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| 338 | DO 40 JV=1,NTRA |
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| 339 | S00(JV)=0. |
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| 340 | 40 CONTINUE |
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| 341 | C |
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| 342 | DO 41 I=1,LON |
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| 343 | C |
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| 344 | IF(VGRI(I,K,L).GE.0.) THEN |
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| 345 | FM(I,K)=VGRI(I,K,L)*DTY |
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| 346 | ALF(I,K)=FM(I,K)/SM(I,K,L) |
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| 347 | SM(I,K,L)=SM(I,K,L)-FM(I,K) |
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| 348 | SM0=SM0+FM(I,K) |
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| 349 | ENDIF |
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| 350 | C |
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| 351 | ALFQ(I,K)=ALF(I,K)*ALF(I,K) |
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| 352 | ALF1(I,K)=1.-ALF(I,K) |
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| 353 | ALF1Q(I,K)=ALF1(I,K)*ALF1(I,K) |
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| 354 | C |
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| 355 | 41 CONTINUE |
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| 356 | C |
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| 357 | DO 42 JV=1,NTRA |
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| 358 | DO 420 I=1,LON |
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| 359 | C |
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| 360 | IF(VGRI(I,K,L).GE.0.) THEN |
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| 361 | F0 (I,K,JV)=ALF(I,K)* |
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| 362 | + ( S0(I,K,L,JV)+ALF1(I,K)*sy(I,K,L,JV) ) |
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| 363 | S00(JV)=S00(JV)+F0(I,K,JV) |
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| 364 | C |
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| 365 | S0(I,K,L,JV)=S0 (I,K,L,JV)-F0 (I,K,JV) |
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| 366 | sy(I,K,L,JV)=ALF1Q(I,K)*sy(I,K,L,JV) |
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| 367 | sx(I,K,L,JV)=ALF1(I,K)*sx(I,K,L,JV) |
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| 368 | sz(I,K,L,JV)=ALF1(I,K)*sz(I,K,L,JV) |
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| 369 | ENDIF |
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| 370 | C |
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| 371 | 420 CONTINUE |
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| 372 | 42 CONTINUE |
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| 373 | C |
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| 374 | DO 43 I=1,LON |
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| 375 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 376 | FM(I,K)=-VGRI(I,K,L)*DTY |
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| 377 | ALF(I,K)=FM(I,K)/SM0 |
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| 378 | ENDIF |
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| 379 | 43 CONTINUE |
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| 380 | C |
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| 381 | DO 44 JV=1,NTRA |
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| 382 | DO 440 I=1,LON |
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| 383 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 384 | F0(I,K,JV)=ALF(I,K)*S00(JV) |
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| 385 | ENDIF |
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| 386 | 440 CONTINUE |
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| 387 | 44 CONTINUE |
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| 388 | C |
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| 389 | C puts the temporary moments Fi into appropriate neighboring boxes |
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| 390 | C |
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| 391 | DO 45 I=1,LON |
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| 392 | C |
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| 393 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 394 | SM(I,K,L)=SM(I,K,L)+FM(I,K) |
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| 395 | ALF(I,K)=FM(I,K)/SM(I,K,L) |
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| 396 | ENDIF |
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| 397 | C |
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| 398 | ALF1(I,K)=1.-ALF(I,K) |
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| 399 | C |
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| 400 | 45 CONTINUE |
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| 401 | C |
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| 402 | DO 46 JV=1,NTRA |
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| 403 | DO 460 I=1,LON |
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| 404 | C |
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| 405 | IF(VGRI(I,K,L).LT.0.) THEN |
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| 406 | C |
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| 407 | TEMPTM=-ALF(I,K)*S0(I,K,L,JV)+ALF1(I,K)*F0(I,K,JV) |
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| 408 | S0(I,K,L,JV)=S0(I,K,L,JV)+F0(I,K,JV) |
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| 409 | sy(I,K,L,JV)=ALF1(I,K)*sy(I,K,L,JV)+3.*TEMPTM |
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| 410 | C |
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| 411 | ENDIF |
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| 412 | C |
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| 413 | 460 CONTINUE |
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| 414 | 46 CONTINUE |
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| 415 | C |
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| 416 | 1 CONTINUE |
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| 417 | C |
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| 418 | RETURN |
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| 419 | END |
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| 420 | |
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