1 | subroutine blendrad(ngrid, nlayer, pplay, |
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2 | & zdtsw, zdtlw, zdtnirco2, zdtnlte, dtrad) |
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3 | c |
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4 | c Combine radiative tendencies. LTE contributions (zdtsw and zdtlw) |
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5 | c have been calculated for the first NLAYLTE layers, zdtnirco2 and |
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6 | c zdtnlte have been calculated for all nlayer layers (but zdtnlte may |
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7 | c be zero low down). zdtlw is phased out in favour of zdtnlte with |
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8 | c height; zdtsw is also phased out to remove possible spurious heating |
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9 | c at low pressures. The pressure at which the transition occurs and |
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10 | c the scale over which this happens are set in the nlteparams.h file. |
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11 | c Above layer NLAYLTE the tendency is purely the sum of NLTE contributions. |
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12 | c (Note : nlaylte is calculated by "nlthermeq" and stored in module "yomlw_h") |
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13 | c Stephen Lewis 6/2000 FF |
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14 | c |
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15 | use yomlw_h, only: nlaylte |
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16 | implicit none |
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17 | #include "nlteparams.h" |
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18 | |
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19 | c Input: |
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20 | integer ngrid, nlayer |
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21 | real pplay(ngrid, nlayer) |
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22 | real zdtlw(ngrid, nlayer) |
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23 | real zdtsw(ngrid, nlayer) |
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24 | real zdtnirco2(ngrid, nlayer) |
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25 | real zdtnlte(ngrid, nlayer) |
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26 | c |
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27 | c Output: |
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28 | real dtrad(ngrid, nlayer) |
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29 | c |
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30 | c Local: |
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31 | integer l, ig |
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32 | real alpha |
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33 | c |
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34 | c This is split into two loops to minimize number of calculations, |
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35 | c but for vector machines it may be faster to perform one big |
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36 | c loop from 1 to nlayer and remove the second loop. |
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37 | c |
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38 | c Loop over layers for which zdtsw/lw have been calculated. |
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39 | do l = 1,nlaylte |
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40 | do ig = 1, ngrid |
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41 | c alpha is actually 0.5*(1+tanh((z-ztrans)/zw)) |
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42 | c written here in a simpler form, with z=-ln(p) and zwi=2/zw |
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43 | alpha = 1./(1.+(pplay(ig,l)/ptrans)**zwi) |
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44 | dtrad(ig,l) = (1.-alpha)*(zdtsw(ig,l)+zdtlw(ig,l)) |
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45 | & + zdtnirco2(ig,l) + alpha*zdtnlte(ig,l) |
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46 | enddo |
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47 | enddo |
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48 | c |
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49 | c Faster loop over any remaining layers. |
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50 | do l = nlaylte+1, nlayer |
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51 | do ig = 1, ngrid |
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52 | dtrad(ig,l) = zdtnirco2(ig,l) + zdtnlte(ig,l) |
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53 | enddo |
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54 | enddo |
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55 | c |
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56 | return |
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57 | end |
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