| 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 common "yomlw.h") |
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| 13 | c Stephen Lewis 6/2000 FF |
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| 14 | c |
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| 15 | implicit none |
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| 16 | #include "dimensions.h" |
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| 17 | #include "dimphys.h" |
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| 18 | #include "dimradmars.h" |
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| 19 | #include "nlteparams.h" |
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| 20 | #include "yomlw.h" |
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| 21 | |
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| 22 | c Input: |
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| 23 | integer ngrid, nlayer |
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| 24 | real pplay(ngrid, nlayer) |
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| 25 | real zdtlw(ngrid, nlayer) |
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| 26 | real zdtsw(ngrid, nlayer) |
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| 27 | real zdtnirco2(ngrid, nlayer) |
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| 28 | real zdtnlte(ngrid, nlayer) |
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| 29 | c |
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| 30 | c Output: |
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| 31 | real dtrad(ngrid, nlayer) |
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| 32 | c |
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| 33 | c Local: |
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| 34 | integer l, ig |
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| 35 | real alpha |
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| 36 | c |
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| 37 | c This is split into two loops to minimize number of calculations, |
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| 38 | c but for vector machines it may be faster to perform one big |
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| 39 | c loop from 1 to nlayer and remove the second loop. |
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| 40 | c |
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| 41 | c Loop over layers for which zdtsw/lw have been calculated. |
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| 42 | do l = 1,nlaylte |
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| 43 | do ig = 1, ngrid |
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| 44 | c alpha is actually 0.5*(1+tanh((z-ztrans)/zw)) |
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| 45 | c written here in a simpler form, with z=-ln(p) and zwi=2/zw |
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| 46 | alpha = 1./(1.+(pplay(ig,l)/ptrans)**zwi) |
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| 47 | dtrad(ig,l) = (1.-alpha)*(zdtsw(ig,l)+zdtlw(ig,l)) |
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| 48 | & + zdtnirco2(ig,l) + alpha*zdtnlte(ig,l) |
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| 49 | enddo |
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| 50 | enddo |
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| 51 | c |
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| 52 | c Faster loop over any remaining layers. |
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| 53 | do l = nlaylte+1, nlayer |
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| 54 | do ig = 1, ngrid |
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| 55 | dtrad(ig,l) = zdtnirco2(ig,l) + zdtnlte(ig,l) |
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| 56 | enddo |
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| 57 | enddo |
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| 58 | c |
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| 59 | return |
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| 60 | end |
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