| [1585] | 1 | ! path: $Source$ |
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| 2 | ! author: $Author: miacono $ |
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| 3 | ! revision: $Revision: 23308 $ |
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| 4 | ! created: $Date: 2013-12-27 17:23:51 -0500 (Fri, 27 Dec 2013) $ |
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| 5 | |
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| 6 | module rrtmg_sw_cldprmc |
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| 7 | |
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| 8 | ! -------------------------------------------------------------------------- |
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| 9 | ! | | |
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| 10 | ! | Copyright 2002-2009, Atmospheric & Environmental Research, Inc. (AER). | |
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| 11 | ! | This software may be used, copied, or redistributed as long as it is | |
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| 12 | ! | not sold and this copyright notice is reproduced on each copy made. | |
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| 13 | ! | This model is provided as is without any express or implied warranties. | |
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| 14 | ! | (http://www.rtweb.aer.com/) | |
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| 15 | ! | | |
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| 16 | ! -------------------------------------------------------------------------- |
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| 17 | |
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| 18 | ! ------- Modules ------- |
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| 19 | |
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| 20 | use parkind, only : im => kind_im, rb => kind_rb |
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| 21 | use parrrsw, only : ngptsw, jpband, jpb1, jpb2 |
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| 22 | use rrsw_cld, only : extliq1, ssaliq1, asyliq1, & |
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| 23 | extice2, ssaice2, asyice2, & |
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| 24 | extice3, ssaice3, asyice3, fdlice3, & |
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| 25 | abari, bbari, cbari, dbari, ebari, fbari |
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| 26 | use rrsw_wvn, only : wavenum1, wavenum2, ngb |
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| 27 | use rrsw_vsn, only : hvrclc, hnamclc |
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| 28 | |
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| 29 | implicit none |
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| 30 | |
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| 31 | contains |
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| 32 | |
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| 33 | ! ---------------------------------------------------------------------------- |
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| 34 | subroutine cldprmc_sw(nlayers, inflag, iceflag, liqflag, cldfmc, & |
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| 35 | ciwpmc, clwpmc, reicmc, relqmc, & |
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| 36 | taormc, taucmc, ssacmc, asmcmc, fsfcmc) |
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| 37 | ! ---------------------------------------------------------------------------- |
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| 38 | |
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| 39 | ! Purpose: Compute the cloud optical properties for each cloudy layer |
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| 40 | ! and g-point interval for use by the McICA method. |
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| 41 | ! Note: Only inflag = 0 and inflag=2/liqflag=1/iceflag=1,2,3 are available; |
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| 42 | ! (Hu & Stamnes, Ebert and Curry, Key, and Fu) are implemented. |
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| 43 | |
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| 44 | ! ------- Input ------- |
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| 45 | |
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| 46 | integer(kind=im), intent(in) :: nlayers ! total number of layers |
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| 47 | integer(kind=im), intent(in) :: inflag ! see definitions |
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| 48 | integer(kind=im), intent(in) :: iceflag ! see definitions |
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| 49 | integer(kind=im), intent(in) :: liqflag ! see definitions |
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| 50 | |
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| 51 | real(kind=rb), intent(in) :: cldfmc(:,:) ! cloud fraction [mcica] |
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| 52 | ! Dimensions: (ngptsw,nlayers) |
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| 53 | real(kind=rb), intent(in) :: ciwpmc(:,:) ! cloud ice water path [mcica] |
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| 54 | ! Dimensions: (ngptsw,nlayers) |
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| 55 | real(kind=rb), intent(in) :: clwpmc(:,:) ! cloud liquid water path [mcica] |
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| 56 | ! Dimensions: (ngptsw,nlayers) |
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| 57 | real(kind=rb), intent(in) :: relqmc(:) ! cloud liquid particle effective radius (microns) |
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| 58 | ! Dimensions: (nlayers) |
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| 59 | real(kind=rb), intent(in) :: reicmc(:) ! cloud ice particle effective radius (microns) |
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| 60 | ! Dimensions: (nlayers) |
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| 61 | ! specific definition of reicmc depends on setting of iceflag: |
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| 62 | ! iceflag = 0: (inactive) |
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| 63 | ! |
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| 64 | ! iceflag = 1: ice effective radius, r_ec, (Ebert and Curry, 1992), |
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| 65 | ! r_ec range is limited to 13.0 to 130.0 microns |
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| 66 | ! iceflag = 2: ice effective radius, r_k, (Key, Streamer Ref. Manual, 1996) |
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| 67 | ! r_k range is limited to 5.0 to 131.0 microns |
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| 68 | ! iceflag = 3: generalized effective size, dge, (Fu, 1996), |
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| 69 | ! dge range is limited to 5.0 to 140.0 microns |
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| 70 | ! [dge = 1.0315 * r_ec] |
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| 71 | real(kind=rb), intent(in) :: fsfcmc(:,:) ! cloud forward scattering fraction |
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| 72 | ! Dimensions: (ngptsw,nlayers) |
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| 73 | |
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| 74 | ! ------- Output ------- |
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| 75 | |
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| 76 | real(kind=rb), intent(inout) :: taucmc(:,:) ! cloud optical depth (delta scaled) |
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| 77 | ! Dimensions: (ngptsw,nlayers) |
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| 78 | real(kind=rb), intent(inout) :: ssacmc(:,:) ! single scattering albedo (delta scaled) |
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| 79 | ! Dimensions: (ngptsw,nlayers) |
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| 80 | real(kind=rb), intent(inout) :: asmcmc(:,:) ! asymmetry parameter (delta scaled) |
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| 81 | ! Dimensions: (ngptsw,nlayers) |
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| 82 | real(kind=rb), intent(out) :: taormc(:,:) ! cloud optical depth (non-delta scaled) |
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| 83 | ! Dimensions: (ngptsw,nlayers) |
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| 84 | |
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| 85 | ! ------- Local ------- |
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| 86 | |
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| 87 | ! integer(kind=im) :: ncbands |
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| 88 | integer(kind=im) :: ib, lay, istr, index, icx, ig |
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| 89 | |
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| 90 | real(kind=rb), parameter :: eps = 1.e-06_rb ! epsilon |
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| 91 | real(kind=rb), parameter :: cldmin = 1.e-20_rb ! minimum value for cloud quantities |
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| 92 | real(kind=rb) :: cwp ! total cloud water path |
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| 93 | real(kind=rb) :: radliq ! cloud liquid droplet radius (microns) |
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| 94 | real(kind=rb) :: radice ! cloud ice effective size (microns) |
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| 95 | real(kind=rb) :: factor |
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| 96 | real(kind=rb) :: fint |
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| 97 | |
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| 98 | real(kind=rb) :: taucldorig_a, taucloud_a, ssacloud_a, ffp, ffp1, ffpssa |
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| 99 | real(kind=rb) :: tauiceorig, scatice, ssaice, tauice, tauliqorig, scatliq, ssaliq, tauliq |
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| 100 | |
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| 101 | real(kind=rb) :: fdelta(ngptsw) |
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| 102 | real(kind=rb) :: extcoice(ngptsw), gice(ngptsw) |
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| 103 | real(kind=rb) :: ssacoice(ngptsw), forwice(ngptsw) |
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| 104 | real(kind=rb) :: extcoliq(ngptsw), gliq(ngptsw) |
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| 105 | real(kind=rb) :: ssacoliq(ngptsw), forwliq(ngptsw) |
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| 106 | |
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| 107 | ! Initialize |
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| 108 | |
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| 109 | hvrclc = '$Revision: 23308 $' |
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| 110 | |
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| 111 | ! Some of these initializations are done elsewhere |
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| 112 | do lay = 1, nlayers |
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| 113 | do ig = 1, ngptsw |
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| 114 | taormc(ig,lay) = taucmc(ig,lay) |
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| 115 | ! taucmc(ig,lay) = 0.0_rb |
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| 116 | ! ssacmc(ig,lay) = 1.0_rb |
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| 117 | ! asmcmc(ig,lay) = 0.0_rb |
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| 118 | enddo |
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| 119 | enddo |
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| 120 | |
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| 121 | ! Main layer loop |
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| 122 | do lay = 1, nlayers |
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| 123 | |
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| 124 | ! Main g-point interval loop |
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| 125 | do ig = 1, ngptsw |
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| 126 | cwp = ciwpmc(ig,lay) + clwpmc(ig,lay) |
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| 127 | if (cldfmc(ig,lay) .ge. cldmin .and. & |
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| 128 | (cwp .ge. cldmin .or. taucmc(ig,lay) .ge. cldmin)) then |
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| 129 | |
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| 130 | ! (inflag=0): Cloud optical properties input directly |
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| 131 | if (inflag .eq. 0) then |
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| 132 | ! Cloud optical properties already defined in taucmc, ssacmc, asmcmc are unscaled; |
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| 133 | ! Apply delta-M scaling here (using Henyey-Greenstein approximation) |
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| 134 | taucldorig_a = taucmc(ig,lay) |
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| 135 | ffp = fsfcmc(ig,lay) |
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| 136 | ffp1 = 1.0_rb - ffp |
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| 137 | ffpssa = 1.0_rb - ffp * ssacmc(ig,lay) |
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| 138 | ssacloud_a = ffp1 * ssacmc(ig,lay) / ffpssa |
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| 139 | taucloud_a = ffpssa * taucldorig_a |
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| 140 | |
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| 141 | taormc(ig,lay) = taucldorig_a |
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| 142 | ssacmc(ig,lay) = ssacloud_a |
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| 143 | taucmc(ig,lay) = taucloud_a |
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| 144 | asmcmc(ig,lay) = (asmcmc(ig,lay) - ffp) / (ffp1) |
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| 145 | |
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| 146 | elseif (inflag .eq. 1) then |
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| 147 | stop 'INFLAG = 1 OPTION NOT AVAILABLE WITH MCICA' |
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| 148 | |
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| 149 | ! (inflag=2): Separate treatement of ice clouds and water clouds. |
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| 150 | elseif (inflag .eq. 2) then |
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| 151 | radice = reicmc(lay) |
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| 152 | |
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| 153 | ! Calculation of absorption coefficients due to ice clouds. |
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| 154 | if (ciwpmc(ig,lay) .eq. 0.0_rb) then |
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| 155 | extcoice(ig) = 0.0_rb |
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| 156 | ssacoice(ig) = 0.0_rb |
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| 157 | gice(ig) = 0.0_rb |
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| 158 | forwice(ig) = 0.0_rb |
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| 159 | |
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| 160 | ! (iceflag = 1): |
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| 161 | ! Note: This option uses Ebert and Curry approach for all particle sizes similar to |
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| 162 | ! CAM3 implementation, though this is somewhat unjustified for large ice particles |
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| 163 | elseif (iceflag .eq. 1) then |
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| 164 | if (radice .lt. 13.0_rb .or. radice .gt. 130._rb) stop & |
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| 165 | 'ICE RADIUS OUT OF BOUNDS' |
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| 166 | ib = ngb(ig) |
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| 167 | if (wavenum2(ib) .gt. 1.43e04_rb) then |
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| 168 | icx = 1 |
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| 169 | elseif (wavenum2(ib) .gt. 7.7e03_rb) then |
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| 170 | icx = 2 |
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| 171 | elseif (wavenum2(ib) .gt. 5.3e03_rb) then |
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| 172 | icx = 3 |
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| 173 | elseif (wavenum2(ib) .gt. 4.0e03_rb) then |
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| 174 | icx = 4 |
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| 175 | elseif (wavenum2(ib) .ge. 2.5e03_rb) then |
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| 176 | icx = 5 |
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| 177 | endif |
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| 178 | extcoice(ig) = (abari(icx) + bbari(icx)/radice) |
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| 179 | ssacoice(ig) = 1._rb - cbari(icx) - dbari(icx) * radice |
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| 180 | gice(ig) = ebari(icx) + fbari(icx) * radice |
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| 181 | ! Check to ensure upper limit of gice is within physical limits for large particles |
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| 182 | if (gice(ig).ge.1._rb) gice(ig) = 1._rb - eps |
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| 183 | forwice(ig) = gice(ig)*gice(ig) |
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| 184 | ! Check to ensure all calculated quantities are within physical limits. |
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| 185 | if (extcoice(ig) .lt. 0.0_rb) stop 'ICE EXTINCTION LESS THAN 0.0' |
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| 186 | if (ssacoice(ig) .gt. 1.0_rb) stop 'ICE SSA GRTR THAN 1.0' |
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| 187 | if (ssacoice(ig) .lt. 0.0_rb) stop 'ICE SSA LESS THAN 0.0' |
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| 188 | if (gice(ig) .gt. 1.0_rb) stop 'ICE ASYM GRTR THAN 1.0' |
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| 189 | if (gice(ig) .lt. 0.0_rb) stop 'ICE ASYM LESS THAN 0.0' |
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| 190 | |
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| 191 | ! For iceflag=2 option, ice particle effective radius is limited to 5.0 to 131.0 microns |
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| 192 | |
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| 193 | elseif (iceflag .eq. 2) then |
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| 194 | if (radice .lt. 5.0_rb .or. radice .gt. 131.0_rb) stop 'ICE RADIUS OUT OF BOUNDS' |
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| 195 | factor = (radice - 2._rb)/3._rb |
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| 196 | index = int(factor) |
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| 197 | if (index .eq. 43) index = 42 |
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| 198 | fint = factor - real(index,kind=rb) |
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| 199 | ib = ngb(ig) |
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| 200 | extcoice(ig) = extice2(index,ib) + fint * & |
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| 201 | (extice2(index+1,ib) - extice2(index,ib)) |
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| 202 | ssacoice(ig) = ssaice2(index,ib) + fint * & |
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| 203 | (ssaice2(index+1,ib) - ssaice2(index,ib)) |
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| 204 | gice(ig) = asyice2(index,ib) + fint * & |
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| 205 | (asyice2(index+1,ib) - asyice2(index,ib)) |
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| 206 | forwice(ig) = gice(ig)*gice(ig) |
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| 207 | ! Check to ensure all calculated quantities are within physical limits. |
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| 208 | if (extcoice(ig) .lt. 0.0_rb) stop 'ICE EXTINCTION LESS THAN 0.0' |
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| 209 | if (ssacoice(ig) .gt. 1.0_rb) stop 'ICE SSA GRTR THAN 1.0' |
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| 210 | if (ssacoice(ig) .lt. 0.0_rb) stop 'ICE SSA LESS THAN 0.0' |
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| 211 | if (gice(ig) .gt. 1.0_rb) stop 'ICE ASYM GRTR THAN 1.0' |
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| 212 | if (gice(ig) .lt. 0.0_rb) stop 'ICE ASYM LESS THAN 0.0' |
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| 213 | |
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| 214 | ! For iceflag=3 option, ice particle generalized effective size is limited to 5.0 to 140.0 microns |
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| 215 | |
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| 216 | elseif (iceflag .eq. 3) then |
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| 217 | if (radice .lt. 5.0_rb .or. radice .gt. 140.0_rb) stop 'ICE GENERALIZED EFFECTIVE SIZE OUT OF BOUNDS' |
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| 218 | factor = (radice - 2._rb)/3._rb |
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| 219 | index = int(factor) |
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| 220 | if (index .eq. 46) index = 45 |
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| 221 | fint = factor - real(index,kind=rb) |
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| 222 | ib = ngb(ig) |
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| 223 | extcoice(ig) = extice3(index,ib) + fint * & |
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| 224 | (extice3(index+1,ib) - extice3(index,ib)) |
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| 225 | ssacoice(ig) = ssaice3(index,ib) + fint * & |
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| 226 | (ssaice3(index+1,ib) - ssaice3(index,ib)) |
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| 227 | gice(ig) = asyice3(index,ib) + fint * & |
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| 228 | (asyice3(index+1,ib) - asyice3(index,ib)) |
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| 229 | fdelta(ig) = fdlice3(index,ib) + fint * & |
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| 230 | (fdlice3(index+1,ib) - fdlice3(index,ib)) |
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| 231 | if (fdelta(ig) .lt. 0.0_rb) stop 'FDELTA LESS THAN 0.0' |
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| 232 | if (fdelta(ig) .gt. 1.0_rb) stop 'FDELTA GT THAN 1.0' |
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| 233 | forwice(ig) = fdelta(ig) + 0.5_rb / ssacoice(ig) |
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| 234 | ! See Fu 1996 p. 2067 |
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| 235 | if (forwice(ig) .gt. gice(ig)) forwice(ig) = gice(ig) |
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| 236 | ! Check to ensure all calculated quantities are within physical limits. |
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| 237 | if (extcoice(ig) .lt. 0.0_rb) stop 'ICE EXTINCTION LESS THAN 0.0' |
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| 238 | if (ssacoice(ig) .gt. 1.0_rb) stop 'ICE SSA GRTR THAN 1.0' |
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| 239 | if (ssacoice(ig) .lt. 0.0_rb) stop 'ICE SSA LESS THAN 0.0' |
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| 240 | if (gice(ig) .gt. 1.0_rb) stop 'ICE ASYM GRTR THAN 1.0' |
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| 241 | if (gice(ig) .lt. 0.0_rb) stop 'ICE ASYM LESS THAN 0.0' |
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| 242 | |
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| 243 | endif |
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| 244 | |
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| 245 | ! Calculation of absorption coefficients due to water clouds. |
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| 246 | if (clwpmc(ig,lay) .eq. 0.0_rb) then |
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| 247 | extcoliq(ig) = 0.0_rb |
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| 248 | ssacoliq(ig) = 0.0_rb |
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| 249 | gliq(ig) = 0.0_rb |
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| 250 | forwliq(ig) = 0.0_rb |
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| 251 | |
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| 252 | elseif (liqflag .eq. 1) then |
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| 253 | radliq = relqmc(lay) |
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| 254 | if (radliq .lt. 2.5_rb .or. radliq .gt. 60._rb) stop & |
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| 255 | 'LIQUID EFFECTIVE RADIUS OUT OF BOUNDS' |
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| 256 | index = int(radliq - 1.5_rb) |
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| 257 | if (index .eq. 0) index = 1 |
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| 258 | if (index .eq. 58) index = 57 |
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| 259 | fint = radliq - 1.5_rb - real(index,kind=rb) |
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| 260 | ib = ngb(ig) |
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| 261 | extcoliq(ig) = extliq1(index,ib) + fint * & |
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| 262 | (extliq1(index+1,ib) - extliq1(index,ib)) |
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| 263 | ssacoliq(ig) = ssaliq1(index,ib) + fint * & |
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| 264 | (ssaliq1(index+1,ib) - ssaliq1(index,ib)) |
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| 265 | if (fint .lt. 0._rb .and. ssacoliq(ig) .gt. 1._rb) & |
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| 266 | ssacoliq(ig) = ssaliq1(index,ib) |
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| 267 | gliq(ig) = asyliq1(index,ib) + fint * & |
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| 268 | (asyliq1(index+1,ib) - asyliq1(index,ib)) |
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| 269 | forwliq(ig) = gliq(ig)*gliq(ig) |
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| 270 | ! Check to ensure all calculated quantities are within physical limits. |
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| 271 | if (extcoliq(ig) .lt. 0.0_rb) stop 'LIQUID EXTINCTION LESS THAN 0.0' |
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| 272 | if (ssacoliq(ig) .gt. 1.0_rb) stop 'LIQUID SSA GRTR THAN 1.0' |
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| 273 | if (ssacoliq(ig) .lt. 0.0_rb) stop 'LIQUID SSA LESS THAN 0.0' |
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| 274 | if (gliq(ig) .gt. 1.0_rb) stop 'LIQUID ASYM GRTR THAN 1.0' |
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| 275 | if (gliq(ig) .lt. 0.0_rb) stop 'LIQUID ASYM LESS THAN 0.0' |
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| 276 | endif |
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| 277 | |
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| 278 | tauliqorig = clwpmc(ig,lay) * extcoliq(ig) |
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| 279 | tauiceorig = ciwpmc(ig,lay) * extcoice(ig) |
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| 280 | taormc(ig,lay) = tauliqorig + tauiceorig |
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| 281 | |
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| 282 | ssaliq = ssacoliq(ig) * (1._rb - forwliq(ig)) / & |
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| 283 | (1._rb - forwliq(ig) * ssacoliq(ig)) |
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| 284 | tauliq = (1._rb - forwliq(ig) * ssacoliq(ig)) * tauliqorig |
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| 285 | ssaice = ssacoice(ig) * (1._rb - forwice(ig)) / & |
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| 286 | (1._rb - forwice(ig) * ssacoice(ig)) |
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| 287 | tauice = (1._rb - forwice(ig) * ssacoice(ig)) * tauiceorig |
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| 288 | |
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| 289 | scatliq = ssaliq * tauliq |
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| 290 | scatice = ssaice * tauice |
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| 291 | taucmc(ig,lay) = tauliq + tauice |
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| 292 | |
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| 293 | ! Ensure non-zero taucmc and scatice |
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| 294 | if(taucmc(ig,lay).eq.0.) taucmc(ig,lay) = cldmin |
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| 295 | if(scatice.eq.0.) scatice = cldmin |
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| 296 | |
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| 297 | ssacmc(ig,lay) = (scatliq + scatice) / taucmc(ig,lay) |
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| 298 | |
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| 299 | if (iceflag .eq. 3) then |
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| 300 | ! In accordance with the 1996 Fu paper, equation A.3, |
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| 301 | ! the moments for ice were calculated depending on whether using spheres |
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| 302 | ! or hexagonal ice crystals. |
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| 303 | ! Set asymetry parameter to first moment (istr=1) |
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| 304 | istr = 1 |
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| 305 | asmcmc(ig,lay) = (1.0_rb/(scatliq+scatice))* & |
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| 306 | (scatliq*(gliq(ig)**istr - forwliq(ig)) / & |
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| 307 | (1.0_rb - forwliq(ig)) + scatice * ((gice(ig)-forwice(ig))/ & |
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| 308 | (1.0_rb - forwice(ig)))**istr) |
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| 309 | |
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| 310 | else |
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| 311 | ! This code is the standard method for delta-m scaling. |
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| 312 | ! Set asymetry parameter to first moment (istr=1) |
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| 313 | istr = 1 |
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| 314 | asmcmc(ig,lay) = (scatliq * & |
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| 315 | (gliq(ig)**istr - forwliq(ig)) / & |
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| 316 | (1.0_rb - forwliq(ig)) + scatice * (gice(ig)**istr - forwice(ig)) / & |
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| 317 | (1.0_rb - forwice(ig)))/(scatliq + scatice) |
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| 318 | endif |
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| 319 | |
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| 320 | endif |
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| 321 | |
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| 322 | endif |
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| 323 | |
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| 324 | ! End g-point interval loop |
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| 325 | enddo |
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| 326 | |
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| 327 | ! End layer loop |
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| 328 | enddo |
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| 329 | |
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| 330 | end subroutine cldprmc_sw |
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| 331 | |
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| 332 | end module rrtmg_sw_cldprmc |
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| 333 | |
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