[3] | 1 | SUBROUTINE LW_venus_ve( |
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| 2 | S PPB, pt, psi, deltapsi, |
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| 3 | S PCOOL, |
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| 4 | S PTOPLW,PSOLLW,PSOLLWDN, |
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| 5 | S ZFLNET) |
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| 6 | |
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[101] | 7 | use dimphy |
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[1621] | 8 | use cpdet_phy_mod, only: cpdet |
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[3] | 9 | IMPLICIT none |
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| 10 | |
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| 11 | #include "YOMCST.h" |
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| 12 | C |
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| 13 | C ------------------------------------------------------------------ |
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| 14 | C |
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| 15 | C PURPOSE. |
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| 16 | C -------- |
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| 17 | C |
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| 18 | c This routine uses the NER matrix |
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[953] | 19 | c (computed for a given cell and temp profile in radlwsw) |
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[3] | 20 | c to compute cooling rates and radiative fluxes. |
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| 21 | c |
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| 22 | C AUTHOR. |
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| 23 | C ------- |
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| 24 | C Sebastien Lebonnois |
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| 25 | C |
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| 26 | C MODIFICATIONS. |
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| 27 | C -------------- |
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| 28 | C ORIGINAL : 27/07/2005 |
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| 29 | C version multimatrice (topographie, sommet nuages): 20/12/2006 |
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| 30 | C ------------------------------------------------------------------ |
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| 31 | C |
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| 32 | C* ARGUMENTS: |
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| 33 | C |
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| 34 | c inputs |
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| 35 | |
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[892] | 36 | REAL PPB(klev+1) ! inter-couches PRESSURE (bar) |
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| 37 | REAL pt(klev) ! mid-layer temperature |
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| 38 | real psi(0:klev+1,0:klev+1) ! NER in W/m**2 |
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| 39 | real deltapsi(0:klev+1,0:klev+1) ! D NER / DT in W/m**2/K |
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[3] | 40 | C |
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| 41 | c output |
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| 42 | |
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[1301] | 43 | REAL PCOOL(klev) ! LONGWAVE COOLING (K/s) within each layer |
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[3] | 44 | REAL PTOPLW ! LONGWAVE FLUX AT T.O.A. (net, + vers le haut) |
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| 45 | REAL PSOLLW ! LONGWAVE FLUX AT SURFACE (net, + vers le haut) |
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| 46 | REAL PSOLLWDN ! LONGWAVE FLUX AT SURFACE (down, + vers le bas) |
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[892] | 47 | REAL ZFLNET(klev+1) ! net thermal flux at ppb levels (+ vers le haut) |
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[3] | 48 | |
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| 49 | C |
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| 50 | C* LOCAL VARIABLES: |
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| 51 | C |
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| 52 | integer i,j,p |
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[892] | 53 | real zlnet(klev+1) ! net thermal flux (W/m**2) |
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| 54 | real dzlnet(0:klev) ! Radiative budget (W/m**2) |
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| 55 | real pdp(klev) ! epaisseur de la couche en pression (Pa) |
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[3] | 56 | |
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| 57 | c -------------------------- |
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| 58 | c Calculation of the fluxes |
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| 59 | c -------------------------- |
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| 60 | |
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| 61 | c flux aux intercouches: |
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| 62 | c zlnet(i+1) est le flux net traversant le plafond de la couche i (+ vers le haut) |
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[892] | 63 | do p=0,klev ! numero de la couche |
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[3] | 64 | zlnet(p+1) = 0.0 |
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[892] | 65 | do j=p+1,klev+1 |
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[3] | 66 | do i=0,p |
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| 67 | zlnet(p+1) = zlnet(p+1)+ psi(i,j) |
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| 68 | enddo |
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| 69 | enddo |
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| 70 | enddo |
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| 71 | |
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| 72 | c flux net au sol, + vers le haut: |
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| 73 | PSOLLW = zlnet(1) |
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| 74 | c flux vers le bas au sol, + vers le bas: |
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| 75 | PSOLLWDN = 0.0 |
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[892] | 76 | do i=1,klev+1 |
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[3] | 77 | PSOLLWDN = PSOLLWDN+max(psi(i,0),0.0) |
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| 78 | enddo |
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| 79 | |
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| 80 | c dfluxnet = radiative budget (W m-2) |
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[892] | 81 | do p=0,klev ! numero de la couche |
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[3] | 82 | dzlnet(p) = 0.0 |
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[892] | 83 | do j=0,klev+1 |
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[3] | 84 | dzlnet(p) = dzlnet(p)+psi(p,j) |
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| 85 | enddo |
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| 86 | enddo |
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| 87 | |
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| 88 | c -------------------------------------- |
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| 89 | c Interpolation in the GCM vertical grid |
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| 90 | c -------------------------------------- |
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| 91 | |
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| 92 | c Flux net |
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| 93 | c -------- |
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| 94 | |
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[892] | 95 | do j=1,klev+1 |
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[3] | 96 | ZFLNET(j) = zlnet(j) |
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| 97 | enddo |
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[892] | 98 | PTOPLW = ZFLNET(klev+1) |
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[3] | 99 | |
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| 100 | c Heating rates |
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| 101 | c ------------- |
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| 102 | |
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| 103 | c cool (K/s) = dfluxnet (W/m2) ! positif quand nrj sort de la couche |
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| 104 | c *g (m/s2) |
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| 105 | c /(-dp) (epaisseur couche, en Pa=kg/m/s2) |
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| 106 | c /cp (J/kg/K) |
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| 107 | |
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[892] | 108 | do j=1,klev |
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[3] | 109 | pdp(j)=(PPB(j)-PPB(j+1))*1.e5 |
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| 110 | enddo |
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| 111 | |
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| 112 | c calcul direct OU calcul par schema implicit |
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[808] | 113 | if (1.eq.1) then |
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[892] | 114 | do j=1,klev |
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[3] | 115 | ! ADAPTATION GCM POUR CP(T) |
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| 116 | PCOOL(j) = dzlnet(j) *RG/cpdet(pt(j)) / pdp(j) |
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| 117 | enddo |
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| 118 | else |
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[892] | 119 | call lwi(klev,dzlnet,deltapsi,pdp,pt,PCOOL) |
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[3] | 120 | endif |
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| 121 | c print*,dzlnet |
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| 122 | c print*,pdp |
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| 123 | c print*,PCOOL |
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| 124 | |
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| 125 | return |
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| 126 | end |
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| 127 | |
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