| 1 | SUBROUTINE COOLING(NG,NL,PRESS,TEMP,Z,Q0,lwnet,pfluxi,icld) |
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| 2 | |
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| 3 | c======================================================================= |
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| 4 | c |
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| 5 | c Author : C. P. Mc Kay 01/02/91 |
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| 6 | c ------ |
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| 7 | c |
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| 8 | c Object : |
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| 9 | c -------- |
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| 10 | c |
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| 11 | C THIS SUBROUTINE RETURNS THE COOLING RATE IN TITAN'S ATMOSPHERE |
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| 12 | C INPUTS ARE PRESS(BARS), TEMP(K), Z(KM) |
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| 13 | C OUTPUT IS: Q(K/SEC)C |
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| 14 | C |
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| 15 | C COOLING RATE COMPUTED NEGLECTING SCATTERING. |
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| 16 | C THE TRICK OF THIS ROUTINE IS THAT IT READS IN THE OPACITIES |
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| 17 | C FOR EACH LAYER AT EACH WAVENUMBER IN THE SPECTRAL DOMAIN |
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| 18 | C THESE OPACITIES ARE HELD CONSTANT WITH TEMPERATURE AND TIME. |
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| 19 | c |
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| 20 | c Interface: |
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| 21 | c ---------- |
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| 22 | c |
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| 23 | c Arguments: |
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| 24 | c ---------- |
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| 25 | c |
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| 26 | c input: |
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| 27 | c ------ |
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| 28 | c |
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| 29 | c nl number of levels |
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| 30 | c press(nl) pressure levels (layers) |
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| 31 | c temp(nl) temperature (layers) |
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| 32 | c z(nl) altitude (m, levels) |
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| 33 | c |
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| 34 | c output: |
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| 35 | c ------- |
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| 36 | c |
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| 37 | c q0(nl-1) radiative cooling in K/sec |
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| 38 | c lwnet(nl) net fluxes, (+) upward |
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| 39 | c pfluxi IR descendant a la surface (+ vers le bas) |
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| 40 | c |
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| 41 | c Commons: |
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| 42 | c -------- |
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| 43 | c |
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| 44 | c COMMON/IRTAUS/dtaui(nlayer,nspeci) |
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| 45 | c infrared opacities of the differents layers for differents |
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| 46 | c spectral ranges. This common is initialized by radtitan. |
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| 47 | c |
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| 48 | c COMMON /PLANT/ CSUBP,F0PI |
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| 49 | c This common is initialized by tgmdat. |
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| 50 | c |
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| 51 | c======================================================================= |
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| 52 | c----------------------------------------------------------------------- |
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| 53 | c Declarations: |
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| 54 | c ------------ |
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| 55 | |
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| 56 | use dimphy |
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| 57 | IMPLICIT NONE |
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| 58 | #include "dimensions.h" |
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| 59 | #include "YOMCST.h" |
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| 60 | #include "clesphys.h" |
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| 61 | INTEGER NLAYER,NSPECI,NSPC1I |
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| 62 | PARAMETER(NLAYER=llm) |
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| 63 | PARAMETER (NSPECI=46,NSPC1I=47) |
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| 64 | |
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| 65 | c ASTUCE POUR EVITER klon... EN ATTENDANT MIEUX |
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| 66 | INTEGER ngrid |
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| 67 | PARAMETER (ngrid=(jjm-1)*iim+2) ! = klon |
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| 68 | c |
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| 69 | c Arguments: |
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| 70 | c ---------- |
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| 71 | |
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| 72 | INTEGER NG,NL,icld |
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| 73 | REAL PRESS(NG,NL),TEMP(NG,NL) |
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| 74 | REAL Z(NG,NL),Q0(NG,NL-1) |
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| 75 | REAL lwnet(NG,NL),UBARI2 |
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| 76 | real pfluxi(NG) |
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| 77 | |
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| 78 | |
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| 79 | c Common: |
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| 80 | c ------- |
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| 81 | |
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| 82 | C DTAU IS PASSED EN-MASS, SO ITS DEMENSIONS ARE CRITICAL |
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| 83 | REAL dtaui(ngrid,NLAYER,NSPECI) |
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| 84 | REAL dtauip(ngrid,NLAYER,NSPECI) |
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| 85 | COMMON /IRTAUS/ dtaui,dtauip |
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| 86 | |
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| 87 | COMMON /PLANT/ CSUBP,F0PI |
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| 88 | REAL CSUBP,F0PI |
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| 89 | |
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| 90 | c Local: |
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| 91 | c ------ |
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| 92 | |
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| 93 | REAL WNOI(NSPECI),DWNI(NSPECI) ! SPECTAL INTERVALS |
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| 94 | REAL B0(ngrid,llm+1) |
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| 95 | REAL EM(ngrid,llm+1) |
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| 96 | REAL DW,WAVEN,TJ,BSURF,QOUT,QIN,eff_g,COLDEN |
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| 97 | |
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| 98 | INTEGER ig,K,J,I,L |
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| 99 | |
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| 100 | c EXTERNAL PLNCK |
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| 101 | REAL PLNCK,zz1,zz2,zz3,zz4,WAVNUM,Xtest |
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| 102 | |
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| 103 | REAL FNETIS(ngrid,llm+1),FNETI(ngrid,llm+1) |
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| 104 | REAL FDIS(ngrid,llm+1,nspeci),FUPIS(ngrid,llm+1,nspeci) |
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| 105 | REAL FDI(ngrid,llm+1), FUPI(ngrid,llm+1) |
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| 106 | |
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| 107 | c Data: |
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| 108 | c ----- |
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| 109 | |
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| 110 | REAL RHOP,UBARI |
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| 111 | DATA RHOP/1.E4/ ! CONVERSION FROM PRESSURE TO MASS |
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| 112 | DATA UBARI/0.5/ ! MEAN COSINE FOR 2-STREAM |
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| 113 | DATA WNOI/ |
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| 114 | & 11.500, 20.000, 31.250, 50.000, 75.000, |
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| 115 | & 100.000, 125.000, 150.000, 175.000, 200.000, |
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| 116 | & 225.000, 250.000, 275.000, 300.000, 325.000, |
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| 117 | & 350.000, 375.000, 400.000, 425.000, 450.000, |
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| 118 | & 475.000, 500.000, 525.000, 550.000, 575.000, |
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| 119 | & 600.000, 628.750, 662.838, 681.757, 683.919, |
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| 120 | & 686.541, 689.623, 692.704, 695.786, 715.141, |
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| 121 | & 733.836, 735.597, 737.358, 739.119, 742.720, |
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| 122 | & 748.160, 753.600, 834.560, 917.333, 926.400, |
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| 123 | & 935.466/ |
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| 124 | DATA DWNI/ |
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| 125 | & 7.000, 10.000, 12.500, 25.000, 25.000, |
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| 126 | & 25.000, 25.000, 25.000, 25.000, 25.000, |
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| 127 | & 25.000, 25.000, 25.000, 25.000, 25.000, |
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| 128 | & 25.000, 25.000, 25.000, 25.000, 25.000, |
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| 129 | & 25.000, 25.000, 25.000, 25.000, 25.000, |
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| 130 | & 25.000, 32.500, 35.676, 2.162, 2.162, |
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| 131 | & 3.082, 3.082, 3.082, 3.082, 35.629, |
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| 132 | & 1.761, 1.761, 1.761, 1.761, 5.440, |
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| 133 | & 5.440, 5.440, 156.480, 9.067, 9.067, |
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| 134 | & 9.067/ |
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| 135 | |
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| 136 | |
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| 137 | save RHOP,UBARI,WNOI,DWNI |
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| 138 | |
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| 139 | REAL effg ! effg est une fonction(z en m) |
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| 140 | |
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| 141 | c----------------------------------------------------------------------- |
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| 142 | |
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| 143 | c Initialisations: |
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| 144 | c ---------------- |
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| 145 | |
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| 146 | UBARI2=1./1.66 |
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| 147 | UBARI2=UBARI |
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| 148 | |
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| 149 | C ZERO THE NET FLUXES |
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| 150 | Q0 = 0.0 |
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| 151 | lwnet = 0.0 |
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| 152 | |
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| 153 | c----------------------------------------------------------------------- |
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| 154 | C WE NOW ENTER A MAJOR LOOP OVER SPECRAL INTERVALS IN THE INFRARED |
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| 155 | C TO CALCULATE THE NET FLUX IN EACH SPECTRAL INTERVAL |
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| 156 | c----------------------------------------------------------------------- |
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| 157 | |
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| 158 | DO 2000 K=1,NSPECI ! *** START OF SPECTRAL LOOP |
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| 159 | |
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| 160 | c----------------------------------------------------------------------- |
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| 161 | C SET UP ALTITIDUE PARAMETERS |
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| 162 | |
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| 163 | WAVEN=WNOI(K) |
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| 164 | DW=DWNI(K) |
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| 165 | zz1=DW/(2.*2) |
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| 166 | EM = 0. |
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| 167 | B0 = 0. |
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| 168 | |
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| 169 | DO J=1,NL-1 |
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| 170 | DO ig=1,NG |
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| 171 | TJ=TEMP(ig,J) |
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| 172 | |
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| 173 | |
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| 174 | C Modif: in-lining de la fonction planck pour vectorisation |
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| 175 | C B0(ig,J)=PLNCK(WAVEN,TJ,DW) |
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| 176 | C FUNCTION PLNCK(WAV,T,DW) |
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| 177 | C* PLNCK FUNCTION RETURNS B IN CGS UNITS, ERGS CM-2 WAVENUMBER-1 |
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| 178 | C* WAVNUM IS WAVENUMBER IN CM-1 |
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| 179 | C* T IS IN KELVIN |
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| 180 | PLNCK=0. |
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| 181 | DO I=-2,2,1 |
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| 182 | WAVNUM=WAVEN + I*zz1 |
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| 183 | zz2=EXP(-1.4388 * WAVNUM/TEMP(ig,J)) |
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| 184 | zz3=WAVNUM*WAVNUM*WAVNUM |
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| 185 | PLNCK=PLNCK+1.191E-5* zz3*zz2/(1.-zz2) |
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| 186 | ENDDO |
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| 187 | B0(ig,J)=.2*PLNCK |
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| 188 | ENDDO |
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| 189 | |
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| 190 | IF (ICLD.EQ.1) THEN |
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| 191 | DO ig=1,NG |
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| 192 | zz4=EXP(-DTAUI(ig,J,K)/UBARI2) |
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| 193 | EM(ig,J)=zz4 |
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| 194 | ENDDO |
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| 195 | ELSE |
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| 196 | DO ig=1,NG |
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| 197 | zz4=EXP(-DTAUIP(ig,J,K)/UBARI2) |
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| 198 | EM(ig,J)=zz4 |
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| 199 | ENDDO |
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| 200 | ENDIF |
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| 201 | ENDDO |
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| 202 | |
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| 203 | c----------------------------------------------------------------------- |
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| 204 | C CALCULATE THE DOWNWELLING RADIATION AT THE TOP OF THE MODEL |
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| 205 | C OR THE TOP LAYER WILL COOL TO SPACE UNPHYSICALLY |
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| 206 | |
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| 207 | FDI =0. |
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| 208 | FDIS =0. |
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| 209 | FUPI =0. |
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| 210 | FUPIS=0. |
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| 211 | |
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| 212 | DO 2220 J=1,NL-1 |
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| 213 | DO 2230 ig=1,NG |
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| 214 | FDI(ig,J+1) = FDI(ig,J)*EM(ig,J) + 2.*RPI*UBARI* |
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| 215 | & B0(ig,J)*(1.-EM(ig,J)) |
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| 216 | FDIS(ig,J+1,K) = FDIS(ig,J,K)*EM(ig,J) + 2.*RPI*UBARI* |
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| 217 | & B0(ig,J)*(1.-EM(ig,J)) |
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| 218 | 2230 CONTINUE |
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| 219 | 2220 CONTINUE |
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| 220 | c write(*,*) |
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| 221 | c write(*,*) 'cooling : EM =' , |
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| 222 | c & ((EM(i,l),l=1,nl),i=1,ngrid) |
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| 223 | c write(*,*) |
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| 224 | c write(*,*) 'cooling : B0 =' , |
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| 225 | c & ((B0(i,l),l=1,nl),i=1,ngrid) |
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| 226 | c write(*,*) |
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| 227 | c write(*,*) 'cooling : FDI =' , |
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| 228 | c & ((FDI(i,l),l=1,nl),i=1,ngrid) |
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| 229 | |
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| 230 | c----------------------------------------------------------------------- |
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| 231 | C UPWARD FLUXES: SURFACE EMISSIONS |
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| 232 | |
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| 233 | DO 2310 ig=1,NG |
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| 234 | PLNCK=0. |
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| 235 | DO I=-2,2,1 |
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| 236 | WAVNUM=WAVEN + I*zz1 |
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| 237 | zz2=EXP(-1.4388 * WAVNUM/TEMP(ig,NL)) |
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| 238 | zz3=WAVNUM*WAVNUM*WAVNUM |
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| 239 | PLNCK=PLNCK+1.191E-5* zz3*zz2/(1.-zz2) |
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| 240 | ENDDO |
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| 241 | c BSURF=PLNCK( WAVEN, TEMP(ig,NL), DW) |
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| 242 | BSURF=.2*PLNCK*emis |
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| 243 | FUPI(ig,NL) =BSURF*2.*RPI*UBARI+(1-emis)*FDI(ig,NL) |
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| 244 | FUPIS(ig,NL,K)=BSURF*2.*RPI*UBARI+(1-emis)*FDIS(ig,NL,K) |
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| 245 | 2310 CONTINUE |
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| 246 | c write(*,*) |
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| 247 | c write(*,*) 'cooling : FUPI/NL =' , |
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| 248 | c & ((FUPI(i,l),l=nl,nl),i=1,NG) |
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| 249 | c write(*,*) |
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| 250 | c write(*,*) 'cooling : FDI/NL =' , |
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| 251 | c & ((FDI(i,l),l=nl,nl),i=1,NG) |
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| 252 | |
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| 253 | DO 2320 J=NL-1,1,-1 |
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| 254 | DO 2330 ig=1,NG |
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| 255 | FUPI(ig,J) = FUPI(ig,J+1)*EM(ig,J) + 2.*RPI*UBARI* |
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| 256 | & B0(ig,J)*(1.-EM(ig,J)) |
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| 257 | FUPIS(ig,J,K) = FUPIS(ig,J+1,K)*EM(ig,J)+2.*RPI*UBARI* |
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| 258 | & B0(ig,J)*(1.-EM(ig,J)) |
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| 259 | 2330 CONTINUE |
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| 260 | 2320 CONTINUE |
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| 261 | c write(*,*) |
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| 262 | c write(*,*) 'cooling : EM =' , |
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| 263 | c & ((EM(i,l),l=1,nl),i=1,ngrid) |
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| 264 | c write(*,*) |
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| 265 | c write(*,*) 'cooling : B0 =' , |
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| 266 | c & ((B0(i,l),l=1,nl),i=1,ngrid) |
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| 267 | c write(*,*) |
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| 268 | c write(*,*) 'cooling : FUPI =' , |
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| 269 | c & ((FUPI(i,l),l=1,nl),i=1,ngrid) |
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| 270 | |
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| 271 | c compute the downward IR flux at the surface: |
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| 272 | c |
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| 273 | DO 3520 ig=1,NG |
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| 274 | pfluxi(ig)=pfluxi(ig)+ DWNI(K)*FDI(ig,NL) |
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| 275 | 3520 CONTINUE |
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| 276 | |
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| 277 | c compute the net IR flux, (+) upward: |
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| 278 | c |
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| 279 | DO J=1,NL |
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| 280 | DO ig=1,NG |
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| 281 | lwnet(ig,J)= lwnet(ig,J)+ DWNI(K)*(FUPI(ig,J)-FDI(ig,J)) |
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| 282 | ENDDO |
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| 283 | ENDDO |
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| 284 | |
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| 285 | DO 3210 J=1,NL-1 |
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| 286 | DO 3220 ig=1,NG |
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| 287 | QOUT=FUPI(ig,J) + FDI(ig,J+1) ! OUT OF LAYER |
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| 288 | QIN =FDI(ig,J) + FUPI(ig,J+1) ! INTO LAYER |
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| 289 | Q0(ig,J)=Q0(ig,J)+(QOUT-QIN)*DWNI(K) |
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| 290 | 3220 CONTINUE |
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| 291 | 3210 CONTINUE |
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| 292 | |
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| 293 | c write(*,*) |
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| 294 | c write(*,*) 'cooling/loop : FUPI =' , |
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| 295 | c & ((FUPI(i,l),l=1,nl),i=1,ngrid) |
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| 296 | c write(*,*) |
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| 297 | c write(*,*) 'cooling : FDI =' , |
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| 298 | c & ((FDI(i,l),l=1,nl),i=1,ngrid) |
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| 299 | c write(*,*) |
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| 300 | c write(*,*) 'cooling : Q0 =' , |
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| 301 | c & ((Q0(i,l),l=1,nl-1),i=1,ngrid) |
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| 302 | |
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| 303 | |
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| 304 | c----------------------------------------------------------------------- |
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| 305 | |
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| 306 | 2000 CONTINUE ! *** END SPECTRAL INTERVAL COMPUTATIONS |
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| 307 | |
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| 308 | |
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| 309 | c----------------------------------------------------------------------- |
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| 310 | |
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| 311 | c convertion erg/cm2 -> J/m2 |
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| 312 | DO 3550 ig=1,NG |
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| 313 | pfluxi(ig) = 1.e-3*pfluxi(ig) |
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| 314 | lwnet(ig,:) = 1.e-3*lwnet(ig,:) |
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| 315 | 3550 CONTINUE |
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| 316 | |
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| 317 | c PRINT*,'flux IR' |
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| 318 | c WRITE(*,'(8e10.2)') pfluxi |
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| 319 | |
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| 320 | C COMPUTE THE BASELINE COOLING RATE |
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| 321 | |
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| 322 | DO 3000 J=1,NL-1 |
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| 323 | C TURN THE Q'S INTO TIMESCALES..... |
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| 324 | DO 3300 ig=1,NG |
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| 325 | COLDEN = RHOP*(PRESS(ig,J+1)-PRESS(ig,J))/effg(Z(ig,J)) |
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| 326 | c Q0(J) = (COLDEN * CSUBP )/Q0(J) |
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| 327 | Q0(ig,J) = Q0(ig,J) / (COLDEN*CSUBP) |
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| 328 | 3300 CONTINUE |
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| 329 | 3000 CONTINUE |
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| 330 | |
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| 331 | c write(*,*) |
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| 332 | c write(*,*) 'cooling/end : Q0 =' |
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| 333 | c write(*,*) ((Q0(k,l)*1e7,l=1,nl-1),k=1,ngrid) |
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| 334 | c----------------------------------------------------------------------- |
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| 335 | |
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| 336 | RETURN |
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| 337 | END |
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