| 1 | !! Fortran version of different diagnostics |
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| 2 | ! L. Fita. LMD May 2016 |
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| 3 | ! gfortran module_generic.o -c module_ForDiagnostics.F90 |
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| 4 | ! |
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| 5 | ! f2py -m module_ForDiagnostics --f90exec=/usr/bin/gfortran-4.7 -c module_generic.F90 module_ForDiagnostics.F90 |
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| 6 | |
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| 7 | MODULE module_ForDiagnosticsVars |
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| 8 | |
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| 9 | USE module_definitions |
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| 10 | USE module_generic |
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| 11 | |
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| 12 | IMPLICIT NONE |
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| 13 | |
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| 14 | CONTAINS |
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| 15 | |
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| 16 | !!!!!!! Variables |
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| 17 | ! Cdrag_0: Fuction to compute a first order generic approximation of the drag coefficient |
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| 18 | ! compute_psl_ptarget4d2: Compute sea level pressure using a target pressure. Similar to the Benjamin |
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| 19 | ! and Miller (1990). Method found in p_interp.F90 |
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| 20 | ! compute_tv4d: 4D calculation of virtual temperaure |
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| 21 | ! SaturationMixingRatio: WRF's AFWA method to compute the saturation mixing ratio |
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| 22 | ! The2T: WRF's AFWA method to compute the temperature at any pressure level along a saturation adiabat |
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| 23 | ! by iteratively solving for it from the parcel thetae. |
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| 24 | ! Theta: WRF's AFWA method to compute potential temperature |
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| 25 | ! Thetae: WRF's AFWA method to compute equivalent potential temperature |
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| 26 | ! TLCL: WRF's AFWA method to compute the temperature of a parcel of air would have if lifed dry |
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| 27 | ! adiabatically to it's lifting condensation level (lcl) |
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| 28 | ! var_cape_afwa1D: WRF's AFWA method to compute cape, cin, fclp, fclz and li |
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| 29 | ! var_cllmh: low, medium, high-cloud [0,1] |
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| 30 | ! var_clt: total cloudiness [0,1] |
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| 31 | ! var_potevap_orPM: potential evapotranspiration following Penman-Monteith formulation implemented in ORCHIDEE |
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| 32 | ! var_psl_ecmwf: sea level pressure using ECMWF method following Mats Hamrud and Philippe Courtier [Pa] |
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| 33 | ! var_zmla_generic: Subroutine to compute pbl-height following a generic method |
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| 34 | ! var_zwind: Subroutine to extrapolate the wind at a given height following the 'power law' methodology |
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| 35 | ! var_zwind_log: Subroutine to extrapolate the wind at a given height following the 'logarithmic law' methodology |
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| 36 | ! var_zwind_MOtheor: Subroutine of wind extrapolation following Moin-Obukhov theory |
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| 37 | ! VirtualTemp1D: Function for 1D calculation of virtual temperaure |
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| 38 | ! VirtualTemperature: WRF's AFWA method to compute virtual temperature |
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| 39 | ! stabfunc_businger: Fucntion of the stability function after Businger et al. (1971) |
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| 40 | |
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| 41 | !!!!!!! Calculations |
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| 42 | ! compute_clt: Computation of total cloudiness |
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| 43 | |
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| 44 | !!! |
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| 45 | ! Variables |
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| 46 | !!! |
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| 47 | |
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| 48 | FUNCTION var_cllmh(clfra, p, dz) |
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| 49 | ! Function to compute cllmh on a 1D column 1: low-cloud; 2: medium-cloud; 3: high-cloud [1] |
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| 50 | |
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| 51 | IMPLICIT NONE |
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| 52 | |
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| 53 | INTEGER, INTENT(in) :: dz |
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| 54 | REAL(r_k), DIMENSION(dz), INTENT(in) :: clfra, p |
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| 55 | REAL(r_k), DIMENSION(3) :: var_cllmh |
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| 56 | |
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| 57 | ! Local |
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| 58 | INTEGER :: iz |
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| 59 | REAL(r_k) :: zclearl, zcloudl, zclearm, zcloudm, & |
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| 60 | zclearh, zcloudh |
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| 61 | |
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| 62 | !!!!!!! Variables |
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| 63 | ! clfra: cloudfraction as 1D verical-column [1] |
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| 64 | ! p: pressure values of the column |
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| 65 | fname = 'var_cllmh' |
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| 66 | |
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| 67 | zclearl = oneRK |
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| 68 | zcloudl = zeroRK |
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| 69 | zclearm = oneRK |
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| 70 | zcloudm = zeroRK |
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| 71 | zclearh = oneRK |
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| 72 | zcloudh = zeroRK |
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| 73 | |
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| 74 | var_cllmh = oneRK |
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| 75 | |
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| 76 | DO iz=1, dz |
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| 77 | IF (p(iz) < prmhc) THEN |
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| 78 | var_cllmh(3) = var_cllmh(3)*(oneRK-MAX(clfra(iz),zcloudh))/(oneRK-MIN(zcloudh,oneRK-ZEPSEC)) |
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| 79 | zcloudh = clfra(iz) |
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| 80 | ELSE IF ( (p(iz) >= prmhc) .AND. (p(iz) < prmlc) ) THEN |
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| 81 | var_cllmh(2) = var_cllmh(2)*(oneRK-MAX(clfra(iz),zcloudm))/(oneRK-MIN(zcloudm,oneRK-ZEPSEC)) |
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| 82 | zcloudm = clfra(iz) |
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| 83 | ELSE IF (p(iz) >= prmlc) THEN |
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| 84 | var_cllmh(1) = var_cllmh(1)*(oneRK-MAX(clfra(iz),zcloudl))/(oneRK-MIN(zcloudl,oneRK-ZEPSEC)) |
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| 85 | zcloudl = clfra(iz) |
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| 86 | ELSE |
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| 87 | PRINT *,' ' // TRIM(fname) // ': This is weird, pressure:', p(iz), ' Pa fails out!!' |
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| 88 | PRINT *,' from high, low cloud pressures:', prmhc, ' ,', prmlc,' Pa at z-level:', iz |
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| 89 | PRINT *,' p_high > p:', prmhc,'> ',p(iz),' Pa' |
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| 90 | PRINT *,' p_low > p >= p_high:', prmlc,'> ',p(iz),' >=', prmhc,' Pa' |
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| 91 | PRINT *,' p_low >= p:', prmlc,'>= ',p(iz),' Pa' |
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| 92 | STOP |
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| 93 | END IF |
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| 94 | END DO |
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| 95 | |
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| 96 | var_cllmh = oneRK - var_cllmh |
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| 97 | |
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| 98 | RETURN |
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| 99 | |
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| 100 | END FUNCTION var_cllmh |
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| 101 | |
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| 102 | REAL(r_k) FUNCTION var_clt(clfra, dz) |
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| 103 | ! Function to compute the total cloud following 'newmicro.F90' from LMDZ using 1D vertical |
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| 104 | ! column values |
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| 105 | |
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| 106 | IMPLICIT NONE |
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| 107 | |
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| 108 | INTEGER, INTENT(in) :: dz |
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| 109 | REAL(r_k), DIMENSION(dz), INTENT(in) :: clfra |
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| 110 | ! Local |
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| 111 | INTEGER :: iz |
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| 112 | REAL(r_k) :: zclear, zcloud |
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| 113 | |
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| 114 | !!!!!!! Variables |
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| 115 | ! cfra: 1-column cloud fraction values |
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| 116 | |
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| 117 | fname = 'var_clt' |
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| 118 | |
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| 119 | zclear = oneRK |
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| 120 | zcloud = zeroRK |
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| 121 | |
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| 122 | DO iz=1,dz |
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| 123 | zclear = zclear*(oneRK-MAX(clfra(iz),zcloud))/(oneRK-MIN(zcloud,1.-ZEPSEC)) |
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| 124 | var_clt = oneRK - zclear |
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| 125 | zcloud = clfra(iz) |
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| 126 | END DO |
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| 127 | |
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| 128 | RETURN |
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| 129 | |
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| 130 | END FUNCTION var_clt |
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| 131 | |
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| 132 | SUBROUTINE var_psl_ecmwf(PRPRESS, hgt, PTB, PRESBH, PRESBF, psl) |
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| 133 | ! Subroutine to compute sea level pressure using ECMWF method following Mats Hamrud and Philippe Courtier |
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| 134 | ! method found in LMDZ in phylmd/pppmer.F90 in combination with phylmd/ctsar.F90 |
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| 135 | |
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| 136 | ! IMPLICIT ARGUMENTS : CONSTANTS FROM YOMCST,YOMGEM,YOMSTA. |
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| 137 | ! -------------------- |
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| 138 | |
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| 139 | IMPLICIT NONE |
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| 140 | |
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| 141 | REAL, INTENT(in) :: PRPRESS, hgt, PTB, PRESBH, PRESBF |
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| 142 | REAL, INTENT(out) :: psl |
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| 143 | |
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| 144 | ! Local |
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| 145 | REAL :: ghgt, PTSTAR, PT0, ZTSTAR |
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| 146 | REAL :: ZALPHA, POROG |
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| 147 | REAL :: ZDTDZSG, ZOROG, ZT0, ZTX, ZTY, ZX, ZY, ZY2 |
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| 148 | REAL, PARAMETER :: RDTDZ1 = -gammav |
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| 149 | |
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| 150 | !!!!!!! Variables |
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| 151 | ! PRPRESS: Surface pressure [Pa] |
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| 152 | ! hgt: Terrain height [m] |
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| 153 | ! PTB: Temperature first half-level [K] |
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| 154 | ! PRESBH: Pressure first half-level [Pa] |
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| 155 | ! PRESBF: Pressure second full-level [Pa] |
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| 156 | ! psl: sea-level pressure |
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| 157 | |
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| 158 | fname = 'var_psl_ecmwf' |
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| 159 | |
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| 160 | ! Height by gravity |
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| 161 | POROG = hgt*g |
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| 162 | |
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| 163 | !* 1. COMPUTES SURFACE TEMPERATURE |
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| 164 | !* THEN STANDARD SURFACE TEMPERATURE. |
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| 165 | |
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| 166 | ZDTDZSG=-RDTDZ1/g |
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| 167 | ZALPHA=ZDTDZSG*r_d |
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| 168 | |
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| 169 | PTSTAR=PTB*(1.0+ZALPHA*(PRESBH/PRESBF-1.0)) |
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| 170 | PT0=PTSTAR+ZDTDZSG*POROG |
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| 171 | |
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| 172 | !* 2. POST-PROCESS MSL PRESSURE. |
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| 173 | ! -------------------------- |
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| 174 | |
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| 175 | !* 2.1 COMPUTATION OF MODIFIED ALPHA AND TSTAR. |
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| 176 | |
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| 177 | ZTX=290.5 |
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| 178 | ZTY=255.0 |
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| 179 | |
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| 180 | IF (PTSTAR < ZTY) THEN |
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| 181 | ZTSTAR=0.5*(ZTY+PTSTAR) |
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| 182 | ELSEIF (PTSTAR < ZTX) THEN |
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| 183 | ZTSTAR=PTSTAR |
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| 184 | ELSE |
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| 185 | ZTSTAR=0.5*(ZTX+PTSTAR) |
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| 186 | ENDIF |
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| 187 | |
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| 188 | ZT0=ZTSTAR+ZDTDZSG*POROG |
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| 189 | IF (ZTX > ZTSTAR .AND. ZT0 > ZTX) THEN |
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| 190 | ZT0=ZTX |
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| 191 | ELSEIF (ZTX <= ZTSTAR .AND. ZT0 > ZTSTAR) THEN |
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| 192 | ZT0=ZTSTAR |
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| 193 | ELSE |
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| 194 | ZT0=PT0 |
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| 195 | ENDIF |
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| 196 | |
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| 197 | ZOROG=SIGN(MAX(1.0,ABS(POROG)),POROG) |
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| 198 | ZALPHA=r_d*(ZT0-ZTSTAR)/ZOROG |
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| 199 | |
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| 200 | !* 2.2 COMPUTATION OF MSL PRESSURE. |
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| 201 | |
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| 202 | IF (ABS(POROG) >= 0.001) THEN |
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| 203 | ZX=POROG/(r_d*ZTSTAR) |
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| 204 | ZY=ZALPHA*ZX |
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| 205 | ZY2=ZY*ZY |
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| 206 | |
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| 207 | psl=PRPRESS*EXP(ZX*(1.0-0.5*ZY+1.0/3.*ZY2)) |
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| 208 | ELSE |
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| 209 | psl=PRPRESS |
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| 210 | ENDIF |
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| 211 | |
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| 212 | RETURN |
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| 213 | |
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| 214 | END SUBROUTINE var_psl_ecmwf |
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| 215 | |
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| 216 | SUBROUTINE compute_psl_ptarget4d2(press, ps, hgt, ta, qv, ptarget, psl, d1, d2, d3, d4) |
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| 217 | ! Subroutine to compute sea level pressure using a target pressure. Similar to the Benjamin |
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| 218 | ! and Miller (1990). Method found in p_interp.F90 |
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| 219 | |
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| 220 | IMPLICIT NONE |
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| 221 | |
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| 222 | INTEGER, INTENT(in) :: d1, d2, d3, d4 |
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| 223 | REAL(r_k), DIMENSION(d1,d2,d3,d4), INTENT(in) :: press, ta, qv |
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| 224 | REAL(r_k), DIMENSION(d1,d2,d4), INTENT(in) :: ps |
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| 225 | REAL(r_k), DIMENSION(d1,d2), INTENT(in) :: hgt |
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| 226 | REAL(r_k), INTENT(in) :: ptarget |
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| 227 | REAL(r_k), DIMENSION(d1,d2,d4), INTENT(out) :: psl |
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| 228 | |
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| 229 | ! Local |
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| 230 | INTEGER :: i, j, it |
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| 231 | INTEGER :: kin |
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| 232 | INTEGER :: kupper |
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| 233 | REAL(r_k) :: dpmin, dp, tbotextrap, & |
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| 234 | tvbotextrap, virtual |
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| 235 | ! Exponential related to standard atmosphere lapse rate r_d*gammav/g |
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| 236 | REAL(r_k), PARAMETER :: expon=r_d*gammav/grav |
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| 237 | |
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| 238 | !!!!!!! Variables |
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| 239 | ! press: Atmospheric pressure [Pa] |
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| 240 | ! ps: surface pressure [Pa] |
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| 241 | ! hgt: surface height |
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| 242 | ! ta: temperature [K] |
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| 243 | ! qv: water vapor mixing ratio |
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| 244 | ! dz: number of vertical levels |
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| 245 | ! psl: sea-level pressure |
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| 246 | |
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| 247 | fname = 'compute_psl_ptarget4d2' |
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| 248 | |
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| 249 | ! Minimal distance between pressures [Pa] |
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| 250 | dpmin=1.e4 |
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| 251 | psl=0. |
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| 252 | |
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| 253 | DO i=1,d1 |
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| 254 | DO j=1,d2 |
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| 255 | IF (hgt(i,j) /= 0.) THEN |
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| 256 | DO it=1,d4 |
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| 257 | |
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| 258 | ! target pressure to be used for the extrapolation [Pa] (defined in namelist.input) |
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| 259 | ! ptarget = 70000. default value |
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| 260 | |
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| 261 | ! We are below both the ground and the lowest data level. |
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| 262 | |
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| 263 | ! First, find the model level that is closest to a "target" pressure |
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| 264 | ! level, where the "target" pressure is delta-p less that the local |
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| 265 | ! value of a horizontally smoothed surface pressure field. We use |
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| 266 | ! delta-p = 150 hPa here. A standard lapse rate temperature profile |
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| 267 | ! passing through the temperature at this model level will be used |
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| 268 | ! to define the temperature profile below ground. This is similar |
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| 269 | ! to the Benjamin and Miller (1990) method, using |
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| 270 | ! 700 hPa everywhere for the "target" pressure. |
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| 271 | |
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| 272 | kupper = 0 |
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| 273 | loop_kIN: DO kin=d3,1,-1 |
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| 274 | kupper = kin |
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| 275 | dp=abs( press(i,j,kin,it) - ptarget ) |
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| 276 | IF (dp .GT. dpmin) EXIT loop_kIN |
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| 277 | dpmin=min(dpmin,dp) |
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| 278 | ENDDO loop_kIN |
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| 279 | |
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| 280 | tbotextrap=ta(i,j,kupper,it)*(ps(i,j,it)/ptarget)**expon |
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| 281 | tvbotextrap=virtualTemp1D(tbotextrap,qv(i,j,kupper,it)) |
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| 282 | |
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| 283 | psl(i,j,it) = ps(i,j,it)*((tvbotextrap+gammav*hgt(i,j))/tvbotextrap)**(1/expon) |
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| 284 | END DO |
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| 285 | ELSE |
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| 286 | psl(i,j,:) = ps(i,j,:) |
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| 287 | END IF |
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| 288 | END DO |
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| 289 | END DO |
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| 290 | |
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| 291 | RETURN |
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| 292 | |
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| 293 | END SUBROUTINE compute_psl_ptarget4d2 |
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| 294 | |
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| 295 | SUBROUTINE compute_tv4d(ta,qv,tv,d1,d2,d3,d4) |
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| 296 | ! 4D calculation of virtual temperaure |
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| 297 | |
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| 298 | IMPLICIT NONE |
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| 299 | |
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| 300 | INTEGER, INTENT(in) :: d1, d2, d3, d4 |
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| 301 | REAL(r_k), DIMENSION(d1,d2,d3,d4), INTENT(in) :: ta, qv |
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| 302 | REAL(r_k), DIMENSION(d1,d2,d3,d4), INTENT(out) :: tv |
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| 303 | |
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| 304 | ! Variables |
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| 305 | ! ta: temperature [K] |
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| 306 | ! qv: mixing ratio [kgkg-1] |
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| 307 | ! tv: virtual temperature |
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| 308 | |
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| 309 | tv = ta*(oneRK+(qv/epsilonv))/(oneRK+qv) |
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| 310 | |
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| 311 | END SUBROUTINE compute_tv4d |
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| 312 | |
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| 313 | FUNCTION VirtualTemp1D (ta,qv) result (tv) |
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| 314 | ! 1D calculation of virtual temperaure |
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| 315 | |
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| 316 | IMPLICIT NONE |
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| 317 | |
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| 318 | REAL(r_k), INTENT(in) :: ta, qv |
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| 319 | REAL(r_k) :: tv |
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| 320 | |
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| 321 | ! Variables |
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| 322 | ! ta: temperature [K] |
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| 323 | ! qv: mixing ratio [kgkg-1] |
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| 324 | |
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| 325 | tv = ta*(oneRK+(qv/epsilonv))/(oneRK+qv) |
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| 326 | |
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| 327 | END FUNCTION VirtualTemp1D |
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| 328 | |
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| 329 | ! ---- BEGIN modified from module_diag_afwa.F ---- ! |
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| 330 | |
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| 331 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 332 | !~ |
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| 333 | !~ Name: |
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| 334 | !~ Theta |
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| 335 | !~ |
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| 336 | !~ Description: |
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| 337 | !~ This function calculates potential temperature as defined by |
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| 338 | !~ Poisson's equation, given temperature and pressure ( hPa ). |
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| 339 | !~ |
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| 340 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 341 | FUNCTION Theta ( t, p ) |
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| 342 | |
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| 343 | IMPLICIT NONE |
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| 344 | |
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| 345 | !~ Variable declaration |
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| 346 | ! -------------------- |
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| 347 | REAL(r_k), INTENT ( IN ) :: t |
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| 348 | REAL(r_k), INTENT ( IN ) :: p |
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| 349 | REAL(r_k) :: theta |
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| 350 | |
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| 351 | ! Using WRF values |
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| 352 | !REAL :: Rd ! Dry gas constant |
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| 353 | !REAL :: Cp ! Specific heat of dry air at constant pressure |
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| 354 | !REAL :: p00 ! Standard pressure ( 1000 hPa ) |
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| 355 | REAL(r_k) :: Rd, p00 |
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| 356 | |
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| 357 | !Rd = 287.04 |
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| 358 | !Cp = 1004.67 |
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| 359 | !p00 = 1000.00 |
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| 360 | |
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| 361 | Rd = r_d |
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| 362 | p00 = p1000mb/100. |
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| 363 | |
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| 364 | !~ Poisson's equation |
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| 365 | ! ------------------ |
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| 366 | theta = t * ( (p00/p)**(Rd/Cp) ) |
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| 367 | |
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| 368 | END FUNCTION Theta |
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| 369 | |
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| 370 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 371 | !~ |
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| 372 | !~ Name: |
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| 373 | !~ Thetae |
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| 374 | !~ |
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| 375 | !~ Description: |
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| 376 | !~ This function returns equivalent potential temperature using the |
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| 377 | !~ method described in Bolton 1980, Monthly Weather Review, equation 43. |
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| 378 | !~ |
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| 379 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 380 | FUNCTION Thetae ( tK, p, rh, mixr ) |
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| 381 | |
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| 382 | IMPLICIT NONE |
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| 383 | |
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| 384 | !~ Variable Declarations |
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| 385 | ! --------------------- |
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| 386 | REAL(r_k) :: tK ! Temperature ( K ) |
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| 387 | REAL(r_k) :: p ! Pressure ( hPa ) |
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| 388 | REAL(r_k) :: rh ! Relative humidity |
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| 389 | REAL(r_k) :: mixr ! Mixing Ratio ( kg kg^-1) |
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| 390 | REAL(r_k) :: te ! Equivalent temperature ( K ) |
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| 391 | REAL(r_k) :: thetae ! Equivalent potential temperature |
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| 392 | |
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| 393 | ! Using WRF values |
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| 394 | !REAL, PARAMETER :: R = 287.04 ! Universal gas constant (J/deg kg) |
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| 395 | !REAL, PARAMETER :: P0 = 1000.0 ! Standard pressure at surface (hPa) |
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| 396 | REAL(r_k) :: R, p00, Lv |
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| 397 | !REAL, PARAMETER :: lv = 2.54*(10**6) ! Latent heat of vaporization |
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| 398 | ! (J kg^-1) |
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| 399 | !REAL, PARAMETER :: cp = 1004.67 ! Specific heat of dry air constant |
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| 400 | ! at pressure (J/deg kg) |
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| 401 | REAL(r_k) :: tlc ! LCL temperature |
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| 402 | |
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| 403 | R = r_d |
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| 404 | p00 = p1000mb/100. |
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| 405 | lv = XLV |
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| 406 | |
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| 407 | !~ Calculate the temperature of the LCL |
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| 408 | ! ------------------------------------ |
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| 409 | tlc = TLCL ( tK, rh ) |
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| 410 | |
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| 411 | !~ Calculate theta-e |
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| 412 | ! ----------------- |
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| 413 | thetae = (tK * (p00/p)**( (R/Cp)*(1.- ( (.28E-3)*mixr*1000.) ) ) )* & |
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| 414 | exp( (((3.376/tlc)-.00254))*& |
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| 415 | (mixr*1000.*(1.+(.81E-3)*mixr*1000.)) ) |
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| 416 | |
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| 417 | END FUNCTION Thetae |
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| 418 | |
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| 419 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 420 | !~ |
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| 421 | !~ Name: |
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| 422 | !~ The2T.f90 |
|---|
| 423 | !~ |
|---|
| 424 | !~ Description: |
|---|
| 425 | !~ This function returns the temperature at any pressure level along a |
|---|
| 426 | !~ saturation adiabat by iteratively solving for it from the parcel |
|---|
| 427 | !~ thetae. |
|---|
| 428 | !~ |
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| 429 | !~ Dependencies: |
|---|
| 430 | !~ function thetae.f90 |
|---|
| 431 | !~ |
|---|
| 432 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
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| 433 | FUNCTION The2T ( thetaeK, pres, flag ) result ( tparcel ) |
|---|
| 434 | |
|---|
| 435 | IMPLICIT NONE |
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| 436 | |
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| 437 | !~ Variable Declaration |
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| 438 | ! -------------------- |
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| 439 | REAL(r_k), INTENT ( IN ) :: thetaeK |
|---|
| 440 | REAL(r_k), INTENT ( IN ) :: pres |
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| 441 | LOGICAL, INTENT ( INOUT ) :: flag |
|---|
| 442 | REAL(r_k) :: tparcel |
|---|
| 443 | |
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| 444 | REAL(r_k) :: thetaK |
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| 445 | REAL(r_k) :: tovtheta |
|---|
| 446 | REAL(r_k) :: tcheck |
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| 447 | REAL(r_k) :: svpr, svpr2 |
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| 448 | REAL(r_k) :: smixr, smixr2 |
|---|
| 449 | REAL(r_k) :: thetae_check, thetae_check2 |
|---|
| 450 | REAL(r_k) :: tguess_2, correction |
|---|
| 451 | |
|---|
| 452 | LOGICAL :: found |
|---|
| 453 | INTEGER :: iter |
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| 454 | |
|---|
| 455 | ! Using WRF values |
|---|
| 456 | !REAL :: R ! Dry gas constant |
|---|
| 457 | !REAL :: Cp ! Specific heat for dry air |
|---|
| 458 | !REAL :: kappa ! Rd / Cp |
|---|
| 459 | !REAL :: Lv ! Latent heat of vaporization at 0 deg. C |
|---|
| 460 | REAL(r_k) :: R, kappa, Lv |
|---|
| 461 | |
|---|
| 462 | R = r_d |
|---|
| 463 | Lv = XLV |
|---|
| 464 | !R = 287.04 |
|---|
| 465 | !Cp = 1004.67 |
|---|
| 466 | Kappa = R/Cp |
|---|
| 467 | !Lv = 2.500E+6 |
|---|
| 468 | |
|---|
| 469 | !~ Make initial guess for temperature of the parcel |
|---|
| 470 | ! ------------------------------------------------ |
|---|
| 471 | tovtheta = (pres/100000.0)**(r/cp) |
|---|
| 472 | tparcel = thetaeK/exp(lv*.012/(cp*295.))*tovtheta |
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| 473 | |
|---|
| 474 | iter = 1 |
|---|
| 475 | found = .false. |
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| 476 | flag = .false. |
|---|
| 477 | |
|---|
| 478 | DO |
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| 479 | IF ( iter > 105 ) EXIT |
|---|
| 480 | |
|---|
| 481 | tguess_2 = tparcel + REAL ( 1 ) |
|---|
| 482 | |
|---|
| 483 | svpr = 6.122 * exp ( (17.67*(tparcel-273.15)) / (tparcel-29.66) ) |
|---|
| 484 | smixr = ( 0.622*svpr ) / ( (pres/100.0)-svpr ) |
|---|
| 485 | svpr2 = 6.122 * exp ( (17.67*(tguess_2-273.15)) / (tguess_2-29.66) ) |
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| 486 | smixr2 = ( 0.622*svpr2 ) / ( (pres/100.0)-svpr2 ) |
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| 487 | |
|---|
| 488 | ! ------------------------------------------------------------------ ~! |
|---|
| 489 | !~ When this function was orinially written, the final parcel ~! |
|---|
| 490 | !~ temperature check was based off of the parcel temperature and ~! |
|---|
| 491 | !~ not the theta-e it produced. As there are multiple temperature- ~! |
|---|
| 492 | !~ mixing ratio combinations that can produce a single theta-e value, ~! |
|---|
| 493 | !~ we change the check to be based off of the resultant theta-e ~! |
|---|
| 494 | !~ value. This seems to be the most accurate way of backing out ~! |
|---|
| 495 | !~ temperature from theta-e. ~! |
|---|
| 496 | !~ ~! |
|---|
| 497 | !~ Rentschler, April 2010 ~! |
|---|
| 498 | ! ------------------------------------------------------------------ ! |
|---|
| 499 | |
|---|
| 500 | !~ Old way... |
|---|
| 501 | !thetaK = thetaeK / EXP (lv * smixr /(cp*tparcel) ) |
|---|
| 502 | !tcheck = thetaK * tovtheta |
|---|
| 503 | |
|---|
| 504 | !~ New way |
|---|
| 505 | thetae_check = Thetae ( tparcel, pres/100., 100., smixr ) |
|---|
| 506 | thetae_check2 = Thetae ( tguess_2, pres/100., 100., smixr2 ) |
|---|
| 507 | |
|---|
| 508 | !~ Whew doggies - that there is some accuracy... |
|---|
| 509 | !IF ( ABS (tparcel-tcheck) < .05) THEN |
|---|
| 510 | IF ( ABS (thetaeK-thetae_check) < .001) THEN |
|---|
| 511 | found = .true. |
|---|
| 512 | flag = .true. |
|---|
| 513 | EXIT |
|---|
| 514 | END IF |
|---|
| 515 | |
|---|
| 516 | !~ Old |
|---|
| 517 | !tparcel = tparcel + (tcheck - tparcel)*.3 |
|---|
| 518 | |
|---|
| 519 | !~ New |
|---|
| 520 | correction = ( thetaeK-thetae_check ) / ( thetae_check2-thetae_check ) |
|---|
| 521 | tparcel = tparcel + correction |
|---|
| 522 | |
|---|
| 523 | iter = iter + 1 |
|---|
| 524 | END DO |
|---|
| 525 | |
|---|
| 526 | !IF ( .not. found ) THEN |
|---|
| 527 | ! print*, "Warning! Thetae to temperature calculation did not converge!" |
|---|
| 528 | ! print*, "Thetae ", thetaeK, "Pressure ", pres |
|---|
| 529 | !END IF |
|---|
| 530 | |
|---|
| 531 | END FUNCTION The2T |
|---|
| 532 | |
|---|
| 533 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 534 | !~ |
|---|
| 535 | !~ Name: |
|---|
| 536 | !~ VirtualTemperature |
|---|
| 537 | !~ |
|---|
| 538 | !~ Description: |
|---|
| 539 | !~ This function returns virtual temperature given temperature ( K ) |
|---|
| 540 | !~ and mixing ratio. |
|---|
| 541 | !~ |
|---|
| 542 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 543 | FUNCTION VirtualTemperature ( tK, w ) result ( Tv ) |
|---|
| 544 | |
|---|
| 545 | IMPLICIT NONE |
|---|
| 546 | |
|---|
| 547 | !~ Variable declaration |
|---|
| 548 | real(r_k), intent ( in ) :: tK !~ Temperature |
|---|
| 549 | real(r_k), intent ( in ) :: w !~ Mixing ratio ( kg kg^-1 ) |
|---|
| 550 | real(r_k) :: Tv !~ Virtual temperature |
|---|
| 551 | |
|---|
| 552 | Tv = tK * ( 1.0 + (w/0.622) ) / ( 1.0 + w ) |
|---|
| 553 | |
|---|
| 554 | END FUNCTION VirtualTemperature |
|---|
| 555 | |
|---|
| 556 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 557 | !~ |
|---|
| 558 | !~ Name: |
|---|
| 559 | !~ SaturationMixingRatio |
|---|
| 560 | !~ |
|---|
| 561 | !~ Description: |
|---|
| 562 | !~ This function calculates saturation mixing ratio given the |
|---|
| 563 | !~ temperature ( K ) and the ambient pressure ( Pa ). Uses |
|---|
| 564 | !~ approximation of saturation vapor pressure. |
|---|
| 565 | !~ |
|---|
| 566 | !~ References: |
|---|
| 567 | !~ Bolton (1980), Monthly Weather Review, pg. 1047, Eq. 10 |
|---|
| 568 | !~ |
|---|
| 569 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 570 | FUNCTION SaturationMixingRatio ( tK, p ) result ( ws ) |
|---|
| 571 | |
|---|
| 572 | IMPLICIT NONE |
|---|
| 573 | |
|---|
| 574 | REAL(r_k), INTENT ( IN ) :: tK |
|---|
| 575 | REAL(r_k), INTENT ( IN ) :: p |
|---|
| 576 | REAL(r_k) :: ws |
|---|
| 577 | |
|---|
| 578 | REAL(r_k) :: es |
|---|
| 579 | |
|---|
| 580 | es = 6.122 * exp ( (17.67*(tK-273.15))/ (tK-29.66) ) |
|---|
| 581 | ws = ( 0.622*es ) / ( (p/100.0)-es ) |
|---|
| 582 | |
|---|
| 583 | END FUNCTION SaturationMixingRatio |
|---|
| 584 | |
|---|
| 585 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 586 | !~ |
|---|
| 587 | !~ Name: |
|---|
| 588 | !~ tlcl |
|---|
| 589 | !~ |
|---|
| 590 | !~ Description: |
|---|
| 591 | !~ This function calculates the temperature of a parcel of air would have |
|---|
| 592 | !~ if lifed dry adiabatically to it's lifting condensation level (lcl). |
|---|
| 593 | !~ |
|---|
| 594 | !~ References: |
|---|
| 595 | !~ Bolton (1980), Monthly Weather Review, pg. 1048, Eq. 22 |
|---|
| 596 | !~ |
|---|
| 597 | !!!~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~!!! |
|---|
| 598 | FUNCTION TLCL ( tk, rh ) |
|---|
| 599 | |
|---|
| 600 | IMPLICIT NONE |
|---|
| 601 | |
|---|
| 602 | REAL(r_k), INTENT ( IN ) :: tK !~ Temperature ( K ) |
|---|
| 603 | REAL(r_k), INTENT ( IN ) :: rh !~ Relative Humidity ( % ) |
|---|
| 604 | REAL(r_k) :: tlcl |
|---|
| 605 | |
|---|
| 606 | REAL(r_k) :: denom, term1, term2 |
|---|
| 607 | |
|---|
| 608 | term1 = 1.0 / ( tK - 55.0 ) |
|---|
| 609 | !! Lluis |
|---|
| 610 | ! IF ( rh > REAL (0) ) THEN |
|---|
| 611 | IF ( rh > zeroRK ) THEN |
|---|
| 612 | term2 = ( LOG (rh/100.0) / 2840.0 ) |
|---|
| 613 | ELSE |
|---|
| 614 | term2 = ( LOG (0.001/oneRK) / 2840.0 ) |
|---|
| 615 | END IF |
|---|
| 616 | denom = term1 - term2 |
|---|
| 617 | !! Lluis |
|---|
| 618 | ! tlcl = ( 1.0 / denom ) + REAL ( 55 ) |
|---|
| 619 | tlcl = ( oneRK / denom ) + 55*oneRK |
|---|
| 620 | |
|---|
| 621 | END FUNCTION TLCL |
|---|
| 622 | |
|---|
| 623 | FUNCTION var_cape_afwa1D(nz, tk, rhv, p, hgt, sfc, cape, cin, zlfc, plfc, lidx, parcel) RESULT (ostat) |
|---|
| 624 | ! Function to compute cape on a 1D column following implementation in phys/module_diag_afwa.F |
|---|
| 625 | |
|---|
| 626 | IMPLICIT NONE |
|---|
| 627 | |
|---|
| 628 | INTEGER, INTENT(in) :: nz, sfc |
|---|
| 629 | REAL(r_k), DIMENSION(nz), INTENT(in) :: tk, rhv, p, hgt |
|---|
| 630 | REAL(r_k), INTENT(out) :: cape, cin, zlfc, plfc, lidx |
|---|
| 631 | INTEGER :: ostat |
|---|
| 632 | INTEGER, INTENT(in) :: parcel |
|---|
| 633 | |
|---|
| 634 | ! Local |
|---|
| 635 | !~ Derived profile variables |
|---|
| 636 | ! ------------------------- |
|---|
| 637 | REAL(r_k), DIMENSION(nz) :: rh, ws, w, dTvK, buoy |
|---|
| 638 | REAL(r_k) :: tlclK, plcl, nbuoy, pbuoy |
|---|
| 639 | |
|---|
| 640 | !~ Source parcel information |
|---|
| 641 | ! ------------------------- |
|---|
| 642 | REAL(r_k) :: srctK, srcrh, srcws, srcw, srcp, & |
|---|
| 643 | srctheta, srcthetaeK |
|---|
| 644 | INTEGER :: srclev |
|---|
| 645 | REAL(r_k) :: spdiff |
|---|
| 646 | |
|---|
| 647 | !~ Parcel variables |
|---|
| 648 | ! ---------------- |
|---|
| 649 | REAL(r_k) :: ptK, ptvK, tvK, pw |
|---|
| 650 | |
|---|
| 651 | !~ Other utility variables |
|---|
| 652 | ! ----------------------- |
|---|
| 653 | INTEGER :: i, j, k |
|---|
| 654 | INTEGER :: lfclev |
|---|
| 655 | INTEGER :: prcl |
|---|
| 656 | INTEGER :: mlev |
|---|
| 657 | INTEGER :: lyrcnt |
|---|
| 658 | LOGICAL :: flag |
|---|
| 659 | LOGICAL :: wflag |
|---|
| 660 | REAL(r_k) :: freeze |
|---|
| 661 | REAL(r_k) :: pdiff |
|---|
| 662 | REAL(r_k) :: pm, pu, pd |
|---|
| 663 | REAL(r_k) :: lidxu |
|---|
| 664 | REAL(r_k) :: lidxd |
|---|
| 665 | |
|---|
| 666 | REAL(r_k), PARAMETER :: Rd = r_d |
|---|
| 667 | REAL(r_k), PARAMETER :: RUNDEF = -9.999E30 |
|---|
| 668 | |
|---|
| 669 | !!!!!!! Variables |
|---|
| 670 | ! nz: Number of vertical levels |
|---|
| 671 | ! sfc: Surface level in the profile |
|---|
| 672 | ! tk: Temperature profile [K] |
|---|
| 673 | ! rhv: Relative Humidity profile [1] |
|---|
| 674 | ! rh: Relative Humidity profile [%] |
|---|
| 675 | ! p: Pressure profile [Pa] |
|---|
| 676 | ! hgt: Geopotential height profile [gpm] |
|---|
| 677 | ! cape: CAPE [Jkg-1] |
|---|
| 678 | ! cin: CIN [Jkg-1] |
|---|
| 679 | ! zlfc: LFC Height [gpm] |
|---|
| 680 | ! plfc: LFC Pressure [Pa] |
|---|
| 681 | ! lidx: Lifted index |
|---|
| 682 | ! FROM: https://en.wikipedia.org/wiki/Lifted_index |
|---|
| 683 | ! lidx >= 6: Very Stable Conditions |
|---|
| 684 | ! 6 > lidx > 1: Stable Conditions, Thunderstorms Not Likely |
|---|
| 685 | ! 0 > lidx > -2: Slightly Unstable, Thunderstorms Possible, With Lifting Mechanism (i.e., cold front, daytime heating, ...) |
|---|
| 686 | ! -2 > lidx > -6: Unstable, Thunderstorms Likely, Some Severe With Lifting Mechanism |
|---|
| 687 | ! -6 > lidx: Very Unstable, Severe Thunderstorms Likely With Lifting Mechanism |
|---|
| 688 | ! ostat: Function return status (Nonzero is bad) |
|---|
| 689 | ! parcel: |
|---|
| 690 | ! Most Unstable = 1 (default) |
|---|
| 691 | ! Mean layer = 2 |
|---|
| 692 | ! Surface based = 3 |
|---|
| 693 | !~ Derived profile variables |
|---|
| 694 | ! ------------------------- |
|---|
| 695 | ! ws: Saturation mixing ratio |
|---|
| 696 | ! w: Mixing ratio |
|---|
| 697 | ! dTvK: Parcel / ambient Tv difference |
|---|
| 698 | ! buoy: Buoyancy |
|---|
| 699 | ! tlclK: LCL temperature [K] |
|---|
| 700 | ! plcl: LCL pressure [Pa] |
|---|
| 701 | ! nbuoy: Negative buoyancy |
|---|
| 702 | ! pbuoy: Positive buoyancy |
|---|
| 703 | |
|---|
| 704 | !~ Source parcel information |
|---|
| 705 | ! ------------------------- |
|---|
| 706 | ! srctK: Source parcel temperature [K] |
|---|
| 707 | ! srcrh: Source parcel rh [%] |
|---|
| 708 | ! srcws: Source parcel sat. mixing ratio |
|---|
| 709 | ! srcw: Source parcel mixing ratio |
|---|
| 710 | ! srcp: Source parcel pressure [Pa] |
|---|
| 711 | ! srctheta: Source parcel theta [K] |
|---|
| 712 | ! srcthetaeK: Source parcel theta-e [K] |
|---|
| 713 | ! srclev: Level of the source parcel |
|---|
| 714 | ! spdiff: Pressure difference |
|---|
| 715 | |
|---|
| 716 | !~ Parcel variables |
|---|
| 717 | ! ---------------- |
|---|
| 718 | ! ptK: Parcel temperature [K] |
|---|
| 719 | ! ptvK: Parcel virtual temperature [K] |
|---|
| 720 | ! tvK: Ambient virtual temperature [K] |
|---|
| 721 | ! pw: Parcel mixing ratio |
|---|
| 722 | |
|---|
| 723 | !~ Other utility variables |
|---|
| 724 | ! ----------------------- |
|---|
| 725 | ! lfclev: Level of LFC |
|---|
| 726 | ! prcl: Internal parcel type indicator |
|---|
| 727 | ! mlev: Level for ML calculation |
|---|
| 728 | ! lyrcnt: Number of layers in mean layer |
|---|
| 729 | ! flag: Dummy flag |
|---|
| 730 | ! wflag: Saturation flag |
|---|
| 731 | ! freeze: Water loading multiplier |
|---|
| 732 | ! pdiff: Pressure difference between levs |
|---|
| 733 | ! pm, pu, pd: Middle, upper, lower pressures |
|---|
| 734 | ! lidxu: Lifted index at upper level |
|---|
| 735 | ! lidxd: Lifted index at lower level |
|---|
| 736 | |
|---|
| 737 | fname = 'var_cape_afwa' |
|---|
| 738 | |
|---|
| 739 | !~ Initialize variables |
|---|
| 740 | ! -------------------- |
|---|
| 741 | rh = rhv*100. |
|---|
| 742 | ostat = 0 |
|---|
| 743 | CAPE = zeroRK |
|---|
| 744 | CIN = zeroRK |
|---|
| 745 | ZLFC = RUNDEF |
|---|
| 746 | PLFC = RUNDEF |
|---|
| 747 | |
|---|
| 748 | !~ Look for submitted parcel definition |
|---|
| 749 | !~ 1 = Most unstable |
|---|
| 750 | !~ 2 = Mean layer |
|---|
| 751 | !~ 3 = Surface based |
|---|
| 752 | ! ------------------------------------- |
|---|
| 753 | IF ( parcel > 3 .or. parcel < 1 ) THEN |
|---|
| 754 | prcl = 1 |
|---|
| 755 | ELSE |
|---|
| 756 | prcl = parcel |
|---|
| 757 | END IF |
|---|
| 758 | |
|---|
| 759 | !~ Initalize our parcel to be (sort of) surface based. Because of |
|---|
| 760 | !~ issues we've been observing in the WRF model, specifically with |
|---|
| 761 | !~ excessive surface moisture values at the surface, using a true |
|---|
| 762 | !~ surface based parcel is resulting a more unstable environment |
|---|
| 763 | !~ than is actually occuring. To address this, our surface parcel |
|---|
| 764 | !~ is now going to be defined as the parcel between 25-50 hPa |
|---|
| 765 | !~ above the surface. UPDATE - now that this routine is in WRF, |
|---|
| 766 | !~ going to trust surface info. GAC 20140415 |
|---|
| 767 | ! ---------------------------------------------------------------- |
|---|
| 768 | |
|---|
| 769 | !~ Compute mixing ratio values for the layer |
|---|
| 770 | ! ----------------------------------------- |
|---|
| 771 | DO k = sfc, nz |
|---|
| 772 | ws ( k ) = SaturationMixingRatio ( tK(k), p(k) ) |
|---|
| 773 | w ( k ) = ( rh(k)/100.0 ) * ws ( k ) |
|---|
| 774 | END DO |
|---|
| 775 | |
|---|
| 776 | srclev = sfc |
|---|
| 777 | srctK = tK ( sfc ) |
|---|
| 778 | srcrh = rh ( sfc ) |
|---|
| 779 | srcp = p ( sfc ) |
|---|
| 780 | srcws = ws ( sfc ) |
|---|
| 781 | srcw = w ( sfc ) |
|---|
| 782 | srctheta = Theta ( tK(sfc), p(sfc)/100.0 ) |
|---|
| 783 | |
|---|
| 784 | !~ Compute the profile mixing ratio. If the parcel is the MU parcel, |
|---|
| 785 | !~ define our parcel to be the most unstable parcel within the lowest |
|---|
| 786 | !~ 180 mb. |
|---|
| 787 | ! ------------------------------------------------------------------- |
|---|
| 788 | mlev = sfc + 1 |
|---|
| 789 | DO k = sfc + 1, nz |
|---|
| 790 | |
|---|
| 791 | !~ Identify the last layer within 100 hPa of the surface |
|---|
| 792 | ! ----------------------------------------------------- |
|---|
| 793 | pdiff = ( p (sfc) - p (k) ) / REAL ( 100 ) |
|---|
| 794 | IF ( pdiff <= REAL (100) ) mlev = k |
|---|
| 795 | |
|---|
| 796 | !~ If we've made it past the lowest 180 hPa, exit the loop |
|---|
| 797 | ! ------------------------------------------------------- |
|---|
| 798 | IF ( pdiff >= REAL (180) ) EXIT |
|---|
| 799 | |
|---|
| 800 | IF ( prcl == 1 ) THEN |
|---|
| 801 | !IF ( (p(k) > 70000.0) .and. (w(k) > srcw) ) THEN |
|---|
| 802 | IF ( (w(k) > srcw) ) THEN |
|---|
| 803 | srctheta = Theta ( tK(k), p(k)/100.0 ) |
|---|
| 804 | srcw = w ( k ) |
|---|
| 805 | srclev = k |
|---|
| 806 | srctK = tK ( k ) |
|---|
| 807 | srcrh = rh ( k ) |
|---|
| 808 | srcp = p ( k ) |
|---|
| 809 | END IF |
|---|
| 810 | END IF |
|---|
| 811 | |
|---|
| 812 | END DO |
|---|
| 813 | |
|---|
| 814 | !~ If we want the mean layer parcel, compute the mean values in the |
|---|
| 815 | !~ lowest 100 hPa. |
|---|
| 816 | ! ---------------------------------------------------------------- |
|---|
| 817 | lyrcnt = mlev - sfc + 1 |
|---|
| 818 | IF ( prcl == 2 ) THEN |
|---|
| 819 | |
|---|
| 820 | srclev = sfc |
|---|
| 821 | srctK = SUM ( tK (sfc:mlev) ) / REAL ( lyrcnt ) |
|---|
| 822 | srcw = SUM ( w (sfc:mlev) ) / REAL ( lyrcnt ) |
|---|
| 823 | srcrh = SUM ( rh (sfc:mlev) ) / REAL ( lyrcnt ) |
|---|
| 824 | srcp = SUM ( p (sfc:mlev) ) / REAL ( lyrcnt ) |
|---|
| 825 | srctheta = Theta ( srctK, srcp/100. ) |
|---|
| 826 | |
|---|
| 827 | END IF |
|---|
| 828 | |
|---|
| 829 | srcthetaeK = Thetae ( srctK, srcp/100.0, srcrh, srcw ) |
|---|
| 830 | |
|---|
| 831 | !~ Calculate temperature and pressure of the LCL |
|---|
| 832 | ! --------------------------------------------- |
|---|
| 833 | tlclK = TLCL ( tK(srclev), rh(srclev) ) |
|---|
| 834 | plcl = p(srclev) * ( (tlclK/tK(srclev))**(Cp/Rd) ) |
|---|
| 835 | |
|---|
| 836 | !~ Now lift the parcel |
|---|
| 837 | ! ------------------- |
|---|
| 838 | |
|---|
| 839 | buoy = REAL ( 0 ) |
|---|
| 840 | pw = srcw |
|---|
| 841 | wflag = .false. |
|---|
| 842 | DO k = srclev, nz |
|---|
| 843 | IF ( p (k) <= plcl ) THEN |
|---|
| 844 | |
|---|
| 845 | !~ The first level after we pass the LCL, we're still going to |
|---|
| 846 | !~ lift the parcel dry adiabatically, as we haven't added the |
|---|
| 847 | !~ the required code to switch between the dry adiabatic and moist |
|---|
| 848 | !~ adiabatic cooling. Since the dry version results in a greater |
|---|
| 849 | !~ temperature loss, doing that for the first step so we don't over |
|---|
| 850 | !~ guesstimate the instability. |
|---|
| 851 | ! ---------------------------------------------------------------- |
|---|
| 852 | |
|---|
| 853 | IF ( wflag ) THEN |
|---|
| 854 | flag = .false. |
|---|
| 855 | |
|---|
| 856 | !~ Above the LCL, our parcel is now undergoing moist adiabatic |
|---|
| 857 | !~ cooling. Because of the latent heating being undergone as |
|---|
| 858 | !~ the parcel rises above the LFC, must iterative solve for the |
|---|
| 859 | !~ parcel temperature using equivalant potential temperature, |
|---|
| 860 | !~ which is conserved during both dry adiabatic and |
|---|
| 861 | !~ pseudoadiabatic displacements. |
|---|
| 862 | ! -------------------------------------------------------------- |
|---|
| 863 | ptK = The2T ( srcthetaeK, p(k), flag ) |
|---|
| 864 | |
|---|
| 865 | !~ Calculate the parcel mixing ratio, which is now changing |
|---|
| 866 | !~ as we condense moisture out of the parcel, and is equivalent |
|---|
| 867 | !~ to the saturation mixing ratio, since we are, in theory, at |
|---|
| 868 | !~ saturation. |
|---|
| 869 | ! ------------------------------------------------------------ |
|---|
| 870 | pw = SaturationMixingRatio ( ptK, p(k) ) |
|---|
| 871 | |
|---|
| 872 | !~ Now we can calculate the virtual temperature of the parcel |
|---|
| 873 | !~ and the surrounding environment to assess the buoyancy. |
|---|
| 874 | ! ---------------------------------------------------------- |
|---|
| 875 | ptvK = VirtualTemperature ( ptK, pw ) |
|---|
| 876 | tvK = VirtualTemperature ( tK (k), w (k) ) |
|---|
| 877 | |
|---|
| 878 | !~ Modification to account for water loading |
|---|
| 879 | ! ----------------------------------------- |
|---|
| 880 | freeze = 0.033 * ( 263.15 - pTvK ) |
|---|
| 881 | IF ( freeze > 1.0 ) freeze = 1.0 |
|---|
| 882 | IF ( freeze < 0.0 ) freeze = 0.0 |
|---|
| 883 | |
|---|
| 884 | !~ Approximate how much of the water vapor has condensed out |
|---|
| 885 | !~ of the parcel at this level |
|---|
| 886 | ! --------------------------------------------------------- |
|---|
| 887 | freeze = freeze * 333700.0 * ( srcw - pw ) / 1005.7 |
|---|
| 888 | |
|---|
| 889 | pTvK = pTvK - pTvK * ( srcw - pw ) + freeze |
|---|
| 890 | dTvK ( k ) = ptvK - tvK |
|---|
| 891 | buoy ( k ) = g * ( dTvK ( k ) / tvK ) |
|---|
| 892 | |
|---|
| 893 | ELSE |
|---|
| 894 | |
|---|
| 895 | !~ Since the theta remains constant whilst undergoing dry |
|---|
| 896 | !~ adiabatic processes, can back out the parcel temperature |
|---|
| 897 | !~ from potential temperature below the LCL |
|---|
| 898 | ! -------------------------------------------------------- |
|---|
| 899 | ptK = srctheta / ( 100000.0/p(k) )**(Rd/Cp) |
|---|
| 900 | |
|---|
| 901 | !~ Grab the parcel virtual temperture, can use the source |
|---|
| 902 | !~ mixing ratio since we are undergoing dry adiabatic cooling |
|---|
| 903 | ! ---------------------------------------------------------- |
|---|
| 904 | ptvK = VirtualTemperature ( ptK, srcw ) |
|---|
| 905 | |
|---|
| 906 | !~ Virtual temperature of the environment |
|---|
| 907 | ! -------------------------------------- |
|---|
| 908 | tvK = VirtualTemperature ( tK (k), w (k) ) |
|---|
| 909 | |
|---|
| 910 | !~ Buoyancy at this level |
|---|
| 911 | ! ---------------------- |
|---|
| 912 | dTvK ( k ) = ptvK - tvK |
|---|
| 913 | buoy ( k ) = g * ( dtvK ( k ) / tvK ) |
|---|
| 914 | |
|---|
| 915 | wflag = .true. |
|---|
| 916 | |
|---|
| 917 | END IF |
|---|
| 918 | |
|---|
| 919 | ELSE |
|---|
| 920 | |
|---|
| 921 | !~ Since the theta remains constant whilst undergoing dry |
|---|
| 922 | !~ adiabatic processes, can back out the parcel temperature |
|---|
| 923 | !~ from potential temperature below the LCL |
|---|
| 924 | ! -------------------------------------------------------- |
|---|
| 925 | ptK = srctheta / ( 100000.0/p(k) )**(Rd/Cp) |
|---|
| 926 | |
|---|
| 927 | !~ Grab the parcel virtual temperture, can use the source |
|---|
| 928 | !~ mixing ratio since we are undergoing dry adiabatic cooling |
|---|
| 929 | ! ---------------------------------------------------------- |
|---|
| 930 | ptvK = VirtualTemperature ( ptK, srcw ) |
|---|
| 931 | |
|---|
| 932 | !~ Virtual temperature of the environment |
|---|
| 933 | ! -------------------------------------- |
|---|
| 934 | tvK = VirtualTemperature ( tK (k), w (k) ) |
|---|
| 935 | |
|---|
| 936 | !~ Buoyancy at this level |
|---|
| 937 | ! --------------------- |
|---|
| 938 | dTvK ( k ) = ptvK - tvK |
|---|
| 939 | buoy ( k ) = g * ( dtvK ( k ) / tvK ) |
|---|
| 940 | |
|---|
| 941 | END IF |
|---|
| 942 | |
|---|
| 943 | !~ Chirp |
|---|
| 944 | ! ----- |
|---|
| 945 | ! WRITE ( *,'(I15,6F15.3)' )k,p(k)/100.,ptK,pw*1000.,ptvK,tvK,buoy(k) |
|---|
| 946 | |
|---|
| 947 | END DO |
|---|
| 948 | |
|---|
| 949 | !~ Add up the buoyancies, find the LFC |
|---|
| 950 | ! ----------------------------------- |
|---|
| 951 | flag = .false. |
|---|
| 952 | lfclev = -1 |
|---|
| 953 | nbuoy = REAL ( 0 ) |
|---|
| 954 | pbuoy = REAL ( 0 ) |
|---|
| 955 | DO k = sfc + 1, nz |
|---|
| 956 | IF ( tK (k) < 253.15 ) EXIT |
|---|
| 957 | CAPE = CAPE + MAX ( buoy (k), 0.0 ) * ( hgt (k) - hgt (k-1) ) |
|---|
| 958 | CIN = CIN + MIN ( buoy (k), 0.0 ) * ( hgt (k) - hgt (k-1) ) |
|---|
| 959 | |
|---|
| 960 | !~ If we've already passed the LFC |
|---|
| 961 | ! ------------------------------- |
|---|
| 962 | IF ( flag .and. buoy (k) > REAL (0) ) THEN |
|---|
| 963 | pbuoy = pbuoy + buoy (k) |
|---|
| 964 | END IF |
|---|
| 965 | |
|---|
| 966 | !~ We are buoyant now - passed the LFC |
|---|
| 967 | ! ----------------------------------- |
|---|
| 968 | IF ( .not. flag .and. buoy (k) > REAL (0) .and. p (k) < plcl ) THEN |
|---|
| 969 | flag = .true. |
|---|
| 970 | pbuoy = pbuoy + buoy (k) |
|---|
| 971 | lfclev = k |
|---|
| 972 | END IF |
|---|
| 973 | |
|---|
| 974 | !~ If we think we've passed the LFC, but encounter a negative layer |
|---|
| 975 | !~ start adding it up. |
|---|
| 976 | ! ---------------------------------------------------------------- |
|---|
| 977 | IF ( flag .and. buoy (k) < REAL (0) ) THEN |
|---|
| 978 | nbuoy = nbuoy + buoy (k) |
|---|
| 979 | |
|---|
| 980 | !~ If the accumulated negative buoyancy is greater than the |
|---|
| 981 | !~ positive buoyancy, then we are capped off. Got to go higher |
|---|
| 982 | !~ to find the LFC. Reset positive and negative buoyancy summations |
|---|
| 983 | ! ---------------------------------------------------------------- |
|---|
| 984 | IF ( ABS (nbuoy) > pbuoy ) THEN |
|---|
| 985 | flag = .false. |
|---|
| 986 | nbuoy = REAL ( 0 ) |
|---|
| 987 | pbuoy = REAL ( 0 ) |
|---|
| 988 | lfclev = -1 |
|---|
| 989 | END IF |
|---|
| 990 | END IF |
|---|
| 991 | |
|---|
| 992 | END DO |
|---|
| 993 | |
|---|
| 994 | !~ Calculate lifted index by interpolating difference between |
|---|
| 995 | !~ parcel and ambient Tv to 500mb. |
|---|
| 996 | ! ---------------------------------------------------------- |
|---|
| 997 | DO k = sfc + 1, nz |
|---|
| 998 | |
|---|
| 999 | pm = 50000. |
|---|
| 1000 | pu = p ( k ) |
|---|
| 1001 | pd = p ( k - 1 ) |
|---|
| 1002 | |
|---|
| 1003 | !~ If we're already above 500mb just set lifted index to 0. |
|---|
| 1004 | !~ -------------------------------------------------------- |
|---|
| 1005 | IF ( pd .le. pm ) THEN |
|---|
| 1006 | lidx = zeroRK |
|---|
| 1007 | EXIT |
|---|
| 1008 | |
|---|
| 1009 | ELSEIF ( pu .le. pm .and. pd .gt. pm) THEN |
|---|
| 1010 | |
|---|
| 1011 | !~ Found trapping pressure: up, middle, down. |
|---|
| 1012 | !~ We are doing first order interpolation. |
|---|
| 1013 | ! ------------------------------------------ |
|---|
| 1014 | lidxu = -dTvK ( k ) * ( pu / 100000. ) ** (Rd/Cp) |
|---|
| 1015 | lidxd = -dTvK ( k-1 ) * ( pd / 100000. ) ** (Rd/Cp) |
|---|
| 1016 | lidx = ( lidxu * (pm-pd) + lidxd * (pu-pm) ) / (pu-pd) |
|---|
| 1017 | EXIT |
|---|
| 1018 | |
|---|
| 1019 | ENDIF |
|---|
| 1020 | |
|---|
| 1021 | END DO |
|---|
| 1022 | |
|---|
| 1023 | !~ Assuming the the LFC is at a pressure level for now |
|---|
| 1024 | ! --------------------------------------------------- |
|---|
| 1025 | IF ( lfclev > zeroRK ) THEN |
|---|
| 1026 | PLFC = p ( lfclev ) |
|---|
| 1027 | ZLFC = hgt ( lfclev ) |
|---|
| 1028 | END IF |
|---|
| 1029 | |
|---|
| 1030 | IF ( PLFC /= PLFC .OR. PLFC < zeroRK ) THEN |
|---|
| 1031 | PLFC = -oneRK |
|---|
| 1032 | ZLFC = -oneRK |
|---|
| 1033 | END IF |
|---|
| 1034 | |
|---|
| 1035 | IF ( CAPE /= CAPE ) cape = zeroRK |
|---|
| 1036 | |
|---|
| 1037 | IF ( CIN /= CIN ) cin = zeroRK |
|---|
| 1038 | |
|---|
| 1039 | !~ Chirp |
|---|
| 1040 | ! ----- |
|---|
| 1041 | ! WRITE ( *,* ) ' CAPE: ', cape, ' CIN: ', cin |
|---|
| 1042 | ! WRITE ( *,* ) ' LFC: ', ZLFC, ' PLFC: ', PLFC |
|---|
| 1043 | ! WRITE ( *,* ) '' |
|---|
| 1044 | ! WRITE ( *,* ) ' Exiting buoyancy.' |
|---|
| 1045 | ! WRITE ( *,* ) ' ==================================== ' |
|---|
| 1046 | ! WRITE ( *,* ) '' |
|---|
| 1047 | |
|---|
| 1048 | RETURN |
|---|
| 1049 | |
|---|
| 1050 | END FUNCTION var_cape_afwa1D |
|---|
| 1051 | |
|---|
| 1052 | ! ---- END modified from module_diag_afwa.F ---- ! |
|---|
| 1053 | |
|---|
| 1054 | SUBROUTINE var_zmla_generic(dz, qv, tpot, z, topo, zmla) |
|---|
| 1055 | ! Subroutine to compute pbl-height following a generic method |
|---|
| 1056 | ! from Nielsen-Gammon et al., 2008 J. Appl. Meteor. Clim. |
|---|
| 1057 | ! applied also in Garcia-Diez et al., 2013, QJRMS |
|---|
| 1058 | ! where |
|---|
| 1059 | ! "The technique identifies the ML height as a threshold increase of potential temperature from |
|---|
| 1060 | ! its minimum value within the boundary layer." |
|---|
| 1061 | ! here applied similarly to Garcia-Diez et al. where |
|---|
| 1062 | ! zmla = "...first level where potential temperature exceeds the minimum potential temperature |
|---|
| 1063 | ! reached in the mixed layer by more than 1.5 K" |
|---|
| 1064 | |
|---|
| 1065 | IMPLICIT NONE |
|---|
| 1066 | |
|---|
| 1067 | INTEGER, INTENT(in) :: dz |
|---|
| 1068 | REAL(r_k), DIMENSION(dz), INTENT(in) :: qv, tpot, z |
|---|
| 1069 | REAL(r_k), INTENT(in) :: topo |
|---|
| 1070 | REAL(r_k), INTENT(out) :: zmla |
|---|
| 1071 | |
|---|
| 1072 | ! Local |
|---|
| 1073 | INTEGER :: i |
|---|
| 1074 | INTEGER :: mldlev, bllev |
|---|
| 1075 | REAL(r_k) :: dqvar, tpotmin, refdt |
|---|
| 1076 | |
|---|
| 1077 | !!!!!!! Variables |
|---|
| 1078 | ! qv: water vapour mixing ratio |
|---|
| 1079 | ! tpot: potential temperature [K] |
|---|
| 1080 | ! z: height above sea level [m] |
|---|
| 1081 | ! topo: topographic height [m] |
|---|
| 1082 | ! zmla: boundary layer height [m] |
|---|
| 1083 | |
|---|
| 1084 | fname = 'var_zmla_generic' |
|---|
| 1085 | |
|---|
| 1086 | ! Pecentage of difference of mixing ratio used to determine Mixed layer depth |
|---|
| 1087 | dqvar = 0.1 |
|---|
| 1088 | |
|---|
| 1089 | ! MLD = Mixed layer with no substantial variation of mixing ratio /\qv < 10% ? |
|---|
| 1090 | !PRINT *,' Mixed layer mixing ratios qv[1] lev qv[lev] dqvar% _______' |
|---|
| 1091 | DO mldlev = 2, dz |
|---|
| 1092 | IF (ABS(qv(mldlev)-qv(1))/qv(1) > dqvar ) EXIT |
|---|
| 1093 | ! PRINT *,qv(1), mldlev, qv(mldlev), ABS(qv(mldlev)-qv(1))/qv(1) |
|---|
| 1094 | END DO |
|---|
| 1095 | |
|---|
| 1096 | ! Looking for the minimum potential temperature within the MLD [tpotmin = min(tpot)_0^MLD] |
|---|
| 1097 | tpotmin = MINVAL(tpot(1:mldlev)) |
|---|
| 1098 | |
|---|
| 1099 | ! Change in temperature to determine boundary layer height |
|---|
| 1100 | refdt = 1.5 |
|---|
| 1101 | |
|---|
| 1102 | ! Determine the first level where tpot > tpotmin + 1.5 K |
|---|
| 1103 | !PRINT *,' Mixed layer tpotmin lev tpotmin[lev] dtpot _______' |
|---|
| 1104 | DO bllev = 1, dz |
|---|
| 1105 | IF (ABS(tpot(bllev)-tpotmin) > refdt ) EXIT |
|---|
| 1106 | ! PRINT *,tpotmin, bllev, tpot(bllev), ABS(tpot(bllev)-tpotmin) |
|---|
| 1107 | END DO |
|---|
| 1108 | |
|---|
| 1109 | !PRINT *,' height end MLD:', z(mldlev) |
|---|
| 1110 | !PRINT *,' pbl height:', z(bllev) |
|---|
| 1111 | |
|---|
| 1112 | zmla = z(bllev) - topo |
|---|
| 1113 | |
|---|
| 1114 | RETURN |
|---|
| 1115 | |
|---|
| 1116 | END SUBROUTINE var_zmla_generic |
|---|
| 1117 | |
|---|
| 1118 | SUBROUTINE var_zwind(d1, u, v, z, u10, v10, sa, ca, newz, unewz, vnewz) |
|---|
| 1119 | ! Subroutine to extrapolate the wind at a given height following the 'power law' methodology |
|---|
| 1120 | ! wss[newz] = wss[z1]*(newz/z1)**alpha |
|---|
| 1121 | ! alpha = (ln(wss[z2])-ln(wss[z1]))/(ln(z2)-ln(z1)) |
|---|
| 1122 | ! AFTER: Phd Thesis: |
|---|
| 1123 | ! Benedicte Jourdier. Ressource eolienne en France metropolitaine : methodes dâevaluation du |
|---|
| 1124 | ! potentiel, variabilite et tendances. Climatologie. Ecole Doctorale Polytechnique, 2015. French |
|---|
| 1125 | ! |
|---|
| 1126 | IMPLICIT NONE |
|---|
| 1127 | |
|---|
| 1128 | INTEGER, INTENT(in) :: d1 |
|---|
| 1129 | REAL(r_k), DIMENSION(d1), INTENT(in) :: u,v,z |
|---|
| 1130 | REAL(r_k), INTENT(in) :: u10, v10, sa, ca, newz |
|---|
| 1131 | REAL(r_k), INTENT(out) :: unewz, vnewz |
|---|
| 1132 | |
|---|
| 1133 | ! Local |
|---|
| 1134 | INTEGER :: inear |
|---|
| 1135 | REAL(r_k) :: zaground |
|---|
| 1136 | REAL(r_k), DIMENSION(2) :: v1, v2, zz, alpha, uvnewz |
|---|
| 1137 | |
|---|
| 1138 | !!!!!!! Variables |
|---|
| 1139 | ! u,v: vertical wind components [ms-1] |
|---|
| 1140 | ! z: height above surface on half-mass levels [m] |
|---|
| 1141 | ! u10,v10: 10-m wind components [ms-1] |
|---|
| 1142 | ! sa, ca: local sine and cosine of map rotation [1.] |
|---|
| 1143 | ! newz: desired height above grpund of extrapolation |
|---|
| 1144 | ! unewz,vnewz: Wind compoonents at the given height [ms-1] |
|---|
| 1145 | |
|---|
| 1146 | fname = 'var_zwind' |
|---|
| 1147 | |
|---|
| 1148 | !PRINT *,' ilev zaground newz z[ilev+1] z[ilev+2] _______' |
|---|
| 1149 | IF (z(1) < newz ) THEN |
|---|
| 1150 | DO inear = 1,d1-2 |
|---|
| 1151 | ! L. Fita, CIMA. Feb. 2018 |
|---|
| 1152 | !! Choose between extra/inter-polate. Maybe better interpolate? |
|---|
| 1153 | ! Here we extrapolate from two closest lower levels |
|---|
| 1154 | !zaground = z(inear+2) |
|---|
| 1155 | zaground = z(inear+1) |
|---|
| 1156 | !PRINT *, inear, z(inear), newz, z(inear+1), z(inear+2) |
|---|
| 1157 | IF ( zaground >= newz) EXIT |
|---|
| 1158 | END DO |
|---|
| 1159 | ELSE |
|---|
| 1160 | !PRINT *, 1, z(1), newz, z(2), z(3), ' z(1) > newz' |
|---|
| 1161 | inear = d1 - 2 |
|---|
| 1162 | END IF |
|---|
| 1163 | |
|---|
| 1164 | IF (inear == d1-2) THEN |
|---|
| 1165 | ! No vertical pair of levels is below newz, using 10m wind as first value and the first level as the second |
|---|
| 1166 | v1(1) = u10 |
|---|
| 1167 | v1(2) = v10 |
|---|
| 1168 | v2(1) = u(1) |
|---|
| 1169 | v2(2) = v(1) |
|---|
| 1170 | zz(1) = 10. |
|---|
| 1171 | zz(2) = z(1) |
|---|
| 1172 | ELSE |
|---|
| 1173 | v1(1) = u(inear) |
|---|
| 1174 | v1(2) = v(inear) |
|---|
| 1175 | v2(1) = u(inear+1) |
|---|
| 1176 | v2(2) = v(inear+1) |
|---|
| 1177 | zz(1) = z(inear) |
|---|
| 1178 | zz(2) = z(inear+1) |
|---|
| 1179 | END IF |
|---|
| 1180 | |
|---|
| 1181 | ! Computing for each component |
|---|
| 1182 | alpha = (LOG(ABS(v2))-LOG(ABS(v1)))/(LOG(zz(2))-LOG(zz(1))) |
|---|
| 1183 | !PRINT *,' Computing with v1:', v1, ' ms-1 v2:', v2, ' ms-1' |
|---|
| 1184 | !PRINT *,' z1:', zz(1), 'm z2:', zz(2), ' m' |
|---|
| 1185 | !PRINT *,' alhpa u:', alpha(1), ' alpha 2:', alpha(2) |
|---|
| 1186 | |
|---|
| 1187 | uvnewz = v1*(newz/zz(1))**alpha |
|---|
| 1188 | ! Earth-rotation |
|---|
| 1189 | unewz = uvnewz(1)*ca - uvnewz(2)*sa |
|---|
| 1190 | vnewz = uvnewz(1)*sa + uvnewz(2)*ca |
|---|
| 1191 | |
|---|
| 1192 | !PRINT *,' result vz:', uvnewz |
|---|
| 1193 | |
|---|
| 1194 | !STOP |
|---|
| 1195 | |
|---|
| 1196 | RETURN |
|---|
| 1197 | |
|---|
| 1198 | END SUBROUTINE var_zwind |
|---|
| 1199 | |
|---|
| 1200 | SUBROUTINE var_zwind_log(d1, u, v, z, u10, v10, sa, ca, newz, unewz, vnewz) |
|---|
| 1201 | ! Subroutine to extrapolate the wind at a given height following the 'logarithmic law' methodology |
|---|
| 1202 | ! wsz = wss[z2]*(ln(newz)-ln(z0))(ln(z2)-ln(z0)) |
|---|
| 1203 | ! ln(z0) = (ws(z2)*ln(z1)-ws(z1)*ln(z2))/(ws(z2)-ws(z1)) |
|---|
| 1204 | ! AFTER: Phd Thesis: |
|---|
| 1205 | ! Benedicte Jourdier. Ressource eolienne en France metropolitaine : methodes dâevaluation du |
|---|
| 1206 | ! potentiel, variabilite et tendances. Climatologie. Ecole Doctorale Polytechnique, 2015. French |
|---|
| 1207 | ! |
|---|
| 1208 | IMPLICIT NONE |
|---|
| 1209 | |
|---|
| 1210 | INTEGER, INTENT(in) :: d1 |
|---|
| 1211 | REAL(r_k), DIMENSION(d1), INTENT(in) :: u,v,z |
|---|
| 1212 | REAL(r_k), INTENT(in) :: u10, v10, sa, ca, newz |
|---|
| 1213 | REAL(r_k), INTENT(out) :: unewz, vnewz |
|---|
| 1214 | |
|---|
| 1215 | ! Local |
|---|
| 1216 | INTEGER :: inear |
|---|
| 1217 | REAL(r_k) :: zaground |
|---|
| 1218 | REAL(r_k), DIMENSION(2) :: v1, v2, zz, logz0, uvnewz |
|---|
| 1219 | |
|---|
| 1220 | !!!!!!! Variables |
|---|
| 1221 | ! u,v: vertical wind components [ms-1] |
|---|
| 1222 | ! z: height above surface on half-mass levels [m] |
|---|
| 1223 | ! u10,v10: 10-m wind components [ms-1] |
|---|
| 1224 | ! sa, ca: local sine and cosine of map rotation [1.] |
|---|
| 1225 | ! newz: desired height above grpund of extrapolation |
|---|
| 1226 | ! unewz,vnewz: Wind compoonents at the given height [ms-1] |
|---|
| 1227 | |
|---|
| 1228 | fname = 'var_zwind_log' |
|---|
| 1229 | |
|---|
| 1230 | !PRINT *,' ilev zaground newz z[ilev+1] z[ilev+2] _______' |
|---|
| 1231 | IF (z(1) < newz ) THEN |
|---|
| 1232 | DO inear = 1,d1-2 |
|---|
| 1233 | ! L. Fita, CIMA. Feb. 2018 |
|---|
| 1234 | !! Choose between extra/inter-polate. Maybe better interpolate? |
|---|
| 1235 | ! Here we extrapolate from two closest lower levels |
|---|
| 1236 | !zaground = z(inear+2) |
|---|
| 1237 | zaground = z(inear+1) |
|---|
| 1238 | !PRINT *, inear, z(inear), newz, z(inear+1), z(inear+2) |
|---|
| 1239 | IF ( zaground >= newz) EXIT |
|---|
| 1240 | END DO |
|---|
| 1241 | ELSE |
|---|
| 1242 | !PRINT *, 1, z(1), newz, z(2), z(3), ' z(1) > newz' |
|---|
| 1243 | inear = d1 - 2 |
|---|
| 1244 | END IF |
|---|
| 1245 | |
|---|
| 1246 | IF (inear == d1-2) THEN |
|---|
| 1247 | ! No vertical pair of levels is below newz, using 10m wind as first value and the first level as the second |
|---|
| 1248 | v1(1) = u10 |
|---|
| 1249 | v1(2) = v10 |
|---|
| 1250 | v2(1) = u(1) |
|---|
| 1251 | v2(2) = v(1) |
|---|
| 1252 | zz(1) = 10. |
|---|
| 1253 | zz(2) = z(1) |
|---|
| 1254 | ELSE |
|---|
| 1255 | v1(1) = u(inear) |
|---|
| 1256 | v1(2) = v(inear) |
|---|
| 1257 | v2(1) = u(inear+1) |
|---|
| 1258 | v2(2) = v(inear+1) |
|---|
| 1259 | zz(1) = z(inear) |
|---|
| 1260 | zz(2) = z(inear+1) |
|---|
| 1261 | END IF |
|---|
| 1262 | |
|---|
| 1263 | ! Computing for each component |
|---|
| 1264 | logz0 = (v2*LOG(zz(1))-v1*LOG(zz(2)))/(v2-v1) |
|---|
| 1265 | |
|---|
| 1266 | uvnewz = v2*(LOG(newz)-logz0)/(LOG(zz(2))-logz0) |
|---|
| 1267 | ! Earth-rotation |
|---|
| 1268 | unewz = uvnewz(1)*ca - uvnewz(2)*sa |
|---|
| 1269 | vnewz = uvnewz(1)*sa + uvnewz(2)*ca |
|---|
| 1270 | |
|---|
| 1271 | !PRINT *,' result vz:', uvnewz |
|---|
| 1272 | |
|---|
| 1273 | !STOP |
|---|
| 1274 | |
|---|
| 1275 | RETURN |
|---|
| 1276 | |
|---|
| 1277 | END SUBROUTINE var_zwind_log |
|---|
| 1278 | |
|---|
| 1279 | SUBROUTINE var_zwind_MOtheor(ust, znt, rmol, u10, v10, sa, ca, newz, uznew, vznew) |
|---|
| 1280 | ! Subroutine of wind extrapolation following Moin-Obukhov theory R. B. Stull, 1988, |
|---|
| 1281 | ! Springer (p376-383) |
|---|
| 1282 | ! Only usefull for newz < 80. m |
|---|
| 1283 | ! Ackonwledgement: M. A. Jimenez, UIB |
|---|
| 1284 | |
|---|
| 1285 | IMPLICIT NONE |
|---|
| 1286 | |
|---|
| 1287 | REAL, INTENT(in) :: ust, znt, rmol, u10, v10, sa, ca |
|---|
| 1288 | REAL, INTENT(in) :: newz |
|---|
| 1289 | REAL, INTENT(out) :: uznew, vznew |
|---|
| 1290 | |
|---|
| 1291 | ! Local |
|---|
| 1292 | REAL :: OL |
|---|
| 1293 | REAL :: stability |
|---|
| 1294 | REAL :: wsz, alpha |
|---|
| 1295 | REAL, DIMENSION(2) :: uvnewz |
|---|
| 1296 | |
|---|
| 1297 | !!!!!!! Variables |
|---|
| 1298 | ! ust: u* in similarity theory [ms-1] |
|---|
| 1299 | ! z0: roughness length [m] |
|---|
| 1300 | !!! L. Fita, CIMA. Feb. 2018 |
|---|
| 1301 | !! NOT SURE if it should be z0 instead? |
|---|
| 1302 | ! znt: thermal time-varying roughness length [m] |
|---|
| 1303 | ! rmol: inverse of Obukhov length [m-1] |
|---|
| 1304 | ! u10: x-component 10-m wind speed [ms-1] |
|---|
| 1305 | ! v10: y-component 10-m wind speed [ms-1] |
|---|
| 1306 | ! sa, ca: local sine and cosine of map rotation [1.] |
|---|
| 1307 | ! |
|---|
| 1308 | fname = 'var_zwind_MOtheor' |
|---|
| 1309 | |
|---|
| 1310 | ! Obukhov Length (using the Boussinesq approximation giving Tv from t2) |
|---|
| 1311 | OL = 1/rmol |
|---|
| 1312 | |
|---|
| 1313 | ! Wind speed at desired height |
|---|
| 1314 | PRINT *,'ust:', ust, 'znt:', znt, 'OL:', OL |
|---|
| 1315 | |
|---|
| 1316 | CALL stabfunc_businger(newz,OL,stability) |
|---|
| 1317 | PRINT *,' z/L:', newz/OL,' stabfunc:', stability, 'log:', LOG(newz/znt), 'log+stability:', LOG(newz/znt) + stability |
|---|
| 1318 | PRINT *,' ust/karman:', ust/karman |
|---|
| 1319 | |
|---|
| 1320 | wsz = ust/karman*( LOG(newz/znt) + stability) |
|---|
| 1321 | PRINT *,' wsz:', wsz |
|---|
| 1322 | |
|---|
| 1323 | ! Without taking into account Ekcman pumping, etc... redistributed by components unsing 10-m wind |
|---|
| 1324 | ! as reference... |
|---|
| 1325 | alpha = ATAN2(v10,u10) |
|---|
| 1326 | uvnewz(1) = wsz*COS(alpha) |
|---|
| 1327 | uvnewz(2) = wsz*SIN(alpha) |
|---|
| 1328 | PRINT *,' uvnewz:', uvnewz |
|---|
| 1329 | |
|---|
| 1330 | ! Earth-rotation |
|---|
| 1331 | uznew = uvnewz(1)*ca - uvnewz(2)*sa |
|---|
| 1332 | vznew = uvnewz(1)*sa + uvnewz(2)*ca |
|---|
| 1333 | PRINT *,' uznew:', uznew, ' vznew:', vznew |
|---|
| 1334 | |
|---|
| 1335 | RETURN |
|---|
| 1336 | |
|---|
| 1337 | END SUBROUTINE var_zwind_MOtheor |
|---|
| 1338 | |
|---|
| 1339 | ! L. Fita, CIMA. Feb. 2018 |
|---|
| 1340 | ! WRF seems to have problems with my functions, let'suse subroutine instead |
|---|
| 1341 | !REAL FUNCTION stabfunc_businger(z,L) |
|---|
| 1342 | SUBROUTINE stabfunc_businger(z,L,stabfunc_busingerv) |
|---|
| 1343 | ! Fucntion of the stability function after Businger et al. (1971), JAS, 28(2), 181â189 |
|---|
| 1344 | |
|---|
| 1345 | IMPLICIT NONE |
|---|
| 1346 | |
|---|
| 1347 | REAL, INTENT(in) :: z,L |
|---|
| 1348 | REAL, INTENT(out) :: stabfunc_busingerv |
|---|
| 1349 | |
|---|
| 1350 | ! Local |
|---|
| 1351 | REAL :: zL, X |
|---|
| 1352 | |
|---|
| 1353 | !!!!!!! Variables |
|---|
| 1354 | ! z: height [m] |
|---|
| 1355 | ! L: Obukhov length [-] |
|---|
| 1356 | |
|---|
| 1357 | fname = 'stabfunc_businger' |
|---|
| 1358 | |
|---|
| 1359 | IF (L /= 0.) THEN |
|---|
| 1360 | zL = z/L |
|---|
| 1361 | ELSE |
|---|
| 1362 | ! Neutral |
|---|
| 1363 | zL = 0. |
|---|
| 1364 | END IF |
|---|
| 1365 | |
|---|
| 1366 | IF (zL > 0.) THEN |
|---|
| 1367 | ! Stable case |
|---|
| 1368 | stabfunc_busingerv = 4.7*z/L |
|---|
| 1369 | ELSE IF (zL < 0.) THEN |
|---|
| 1370 | ! unstable |
|---|
| 1371 | X = (1. - 15.*z/L)**(0.25) |
|---|
| 1372 | !stabfunc_busingerv = -2.*LOG((1.+X)/2.)-LOG((1.+X**2)/2.)+2.*ATAN(X)-piconst/2. |
|---|
| 1373 | stabfunc_busingerv = LOG( ((1.+X**2)/2.)*((1.+X)/2.)**2)-2.*ATAN(X)+piconst/2. |
|---|
| 1374 | ELSE |
|---|
| 1375 | stabfunc_busingerv = 0. |
|---|
| 1376 | END IF |
|---|
| 1377 | |
|---|
| 1378 | RETURN |
|---|
| 1379 | |
|---|
| 1380 | ! END FUNCTION stabfunc_businger |
|---|
| 1381 | END SUBROUTINE stabfunc_businger |
|---|
| 1382 | |
|---|
| 1383 | REAL(r_k) FUNCTION Cdrag_0(ust,uas,vas) |
|---|
| 1384 | ! Fuction to compute a first order generic approximation of the drag coefficient as |
|---|
| 1385 | ! CD = (ust/wss)**2 |
|---|
| 1386 | ! after, Garratt, J.R., 1992.: The Atmospheric Boundary Layer. Cambridge Univ. Press, |
|---|
| 1387 | ! Cambridge, U.K., 316 pp |
|---|
| 1388 | ! Ackonwledgement: M. A. Jimenez, UIB |
|---|
| 1389 | ! |
|---|
| 1390 | IMPLICIT NONE |
|---|
| 1391 | |
|---|
| 1392 | REAL(r_k), INTENT(in) :: ust, uas, vas |
|---|
| 1393 | |
|---|
| 1394 | !!!!!!! Variables |
|---|
| 1395 | ! ust: u* in similarity theory [ms-1] |
|---|
| 1396 | ! uas, vas: x/y-components of wind at 10 m |
|---|
| 1397 | |
|---|
| 1398 | fname = 'Cdrag_0' |
|---|
| 1399 | |
|---|
| 1400 | Cdrag_0 = ust**2/(uas**2+vas**2) |
|---|
| 1401 | |
|---|
| 1402 | END FUNCTION Cdrag_0 |
|---|
| 1403 | |
|---|
| 1404 | SUBROUTINE var_potevap_orPM(rho1, ust, uas, vas, tas, ps, qv1, potevap) |
|---|
| 1405 | ! Subroutine to compute the potential evapotranspiration following Penman-Monteith formulation |
|---|
| 1406 | ! implemented in ORCHIDEE |
|---|
| 1407 | ! potevap = dt*rho1*qc*(q2sat-qv1) |
|---|
| 1408 | |
|---|
| 1409 | IMPLICIT NONE |
|---|
| 1410 | |
|---|
| 1411 | REAL(r_k), INTENT(in) :: rho1, ust, uas, vas, tas, ps, qv1 |
|---|
| 1412 | REAL(r_k), INTENT(out) :: potevap |
|---|
| 1413 | |
|---|
| 1414 | ! Local |
|---|
| 1415 | REAL(r_k) :: q2sat, Cd, qc |
|---|
| 1416 | |
|---|
| 1417 | !!!!!!! Variables |
|---|
| 1418 | ! rho1: atsmophere density at the first layer [kgm-3] |
|---|
| 1419 | ! ust: u* in similarity theory [ms-1] |
|---|
| 1420 | ! uas, vas: x/y-components of 10-m wind [ms-1] |
|---|
| 1421 | ! tas: 2-m atmosphere temperature [K] |
|---|
| 1422 | ! ps: surface pressure [Pa] |
|---|
| 1423 | ! qv1: 1st layer atmospheric mixing ratio [kgkg-1] |
|---|
| 1424 | ! potevap: potential evapo transpiration [kgm-2s-1] |
|---|
| 1425 | fname = 'var_potevap_orPM' |
|---|
| 1426 | |
|---|
| 1427 | ! q2sat: Saturated air at 2m (can be assumed to be q2 == qsfc?) |
|---|
| 1428 | q2sat = SaturationMixingRatio(tas, ps) |
|---|
| 1429 | |
|---|
| 1430 | ! Cd: drag coeffiecient |
|---|
| 1431 | Cd = Cdrag_0(ust, uas, vas) |
|---|
| 1432 | |
|---|
| 1433 | ! qc: surface drag coefficient |
|---|
| 1434 | qc = SQRT(uas**2 + vas**2)*Cd |
|---|
| 1435 | |
|---|
| 1436 | potevap = MAX(zeroRK, rho1*qc*(q2sat - qv1)) |
|---|
| 1437 | |
|---|
| 1438 | END SUBROUTINE var_potevap_orPM |
|---|
| 1439 | |
|---|
| 1440 | END MODULE module_ForDiagnosticsVars |
|---|