Changeset 2096


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Timestamp:
Feb 8, 2019, 5:47:05 PM (6 years ago)
Author:
jvatant
Message:

Readme update of last commit
--JVO

File:
1 edited

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  • trunk/LMDZ.TITAN/README

    r2050 r2096  
    15241524  MUST have been set to 1 ( no self-broadening then, assume it's a trace sepecie )
    15251525  -> You can't neither have CIA of variable species included upstream in the corr-k
     1526
     1527== 08/02/19 == JVO (r2095)
     1528Update radiative transfer with some of the latest updates in the generic model
     1529Cf r2056 by AB  and r1987-1991 by JL :
     1530  + == 28/08/2018 == JL
     1531  Start a series of commits to change the upper boundary conditions in the radiative transfer to solve some issues with the last two layers.
     1532  It seems to be good to have aerosols in the first "radiative layer" of the gcm in the IR but visible does not handle very well diffusion in first layer.
     1533  Tauaero and tauray are set to 0 (a small value for rayleigh because the code crashes otherwise) in the 4 first semilayers in optcv, but not optci.
     1534  This solves random variations of the sw heating at the model top.
     1535  We now shift the radiative model top from p=0 to the middle of the last physical layer. This is done by changing pmid and plevrad in callcorrk and some corrections need to be done in gfluxv.
     1536  This seems to get rid of the aratic temperature behavior in the last two layers of the model (especially on the night side on synchronous planets).
     1537  Additional speedup corrections have been made in gfluxi that change nothing to the result.
     1538  This has been done for water ice in aeropacity, but same correction should probably be done for other aerosol types.
     1539  Finally, if aerosols are present in the last layer we must account for them. Provides better upper boundary condition in the IR. They must however be put to zero in the sw (see optcv and changes in last commit.)
     1540 +== 07/01/2019 == AB
     1541 - Planck step function is replaced by a piecewise linear function in gfluxi.F and sfluxi.F in the computation of B1, B0, PLTOP, PLANCKSUM and BSURF.
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