| 1 | ! $Id$ |
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| 2 | module o3_chem_m |
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| 3 | |
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| 4 | IMPLICIT NONE |
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| 5 | |
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| 6 | PRIVATE o3_prod |
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| 7 | |
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| 8 | CONTAINS |
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| 9 | |
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| 10 | SUBROUTINE o3_chem(julien, gmtime, t_seri, zmasse, pdtphys, rlat, rlon, q) |
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| 11 | |
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| 12 | ! This procedure evolves the ozone mass fraction through a time |
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| 13 | ! step taking only chemistry into account. |
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| 14 | |
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| 15 | ! All the 2-dimensional arrays are on the partial "physics" grid. |
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| 16 | ! Their shape is "(/klon, nbp_lev/)". |
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| 17 | ! Index "(i, :)" is for longitude "rlon(i)", latitude "rlat(i)". |
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| 18 | |
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| 19 | USE lmdz_assert, ONLY: assert |
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| 20 | USE dimphy, ONLY: klon |
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| 21 | USE regr_pr_comb_coefoz_m, ONLY: c_Mob, a4_mass, a2, r_het_interm |
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| 22 | USE lmdz_grid_phy, ONLY: nbp_lev |
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| 23 | USE lmdz_physical_constants, ONLY: pi |
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| 24 | |
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| 25 | INTEGER, INTENT(IN):: julien ! jour julien, 1 <= julien <= 360 |
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| 26 | REAL, INTENT(IN):: gmtime ! heure de la journée en fraction de jour |
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| 27 | REAL, INTENT(IN):: t_seri(:, :) ! (klon, nbp_lev) temperature, in K |
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| 28 | |
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| 29 | REAL, INTENT(IN):: zmasse(:, :) ! (klon, nbp_lev) |
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| 30 | ! (column-density of mass of air in a cell, in kg m-2) |
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| 31 | ! "zmasse(:, k)" is for layer "k".) |
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| 32 | |
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| 33 | REAL, INTENT(IN):: pdtphys ! time step for physics, in s |
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| 34 | |
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| 35 | REAL, INTENT(IN):: rlat(:), rlon(:) |
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| 36 | ! (longitude and latitude of each horizontal position, in degrees) |
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| 37 | |
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| 38 | REAL, INTENT(INOUT):: q(:, :) ! (klon, nbp_lev) mass fraction of ozone |
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| 39 | ! "q(:, k)" is at middle of layer "k".) |
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| 40 | |
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| 41 | ! Variables local to the procedure: |
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| 42 | ! (for "pi") |
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| 43 | INTEGER k |
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| 44 | |
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| 45 | REAL c(klon, nbp_lev) |
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| 46 | ! (constant term during a time step in the net mass production |
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| 47 | ! rate of ozone by chemistry, per unit mass of air, in s-1) |
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| 48 | ! "c(:, k)" is at middle of layer "k".) |
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| 49 | |
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| 50 | REAL b(klon, nbp_lev) |
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| 51 | ! (coefficient of "q" in the net mass production |
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| 52 | ! rate of ozone by chemistry, per unit mass of air, in s-1) |
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| 53 | ! "b(:, k)" is at middle of layer "k".) |
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| 54 | |
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| 55 | REAL dq_o3_chem(klon, nbp_lev) |
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| 56 | ! (variation of ozone mass fraction due to chemistry during a time step) |
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| 57 | ! "dq_o3_chem(:, k)" is at middle of layer "k".) |
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| 58 | |
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| 59 | REAL earth_long |
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| 60 | ! (longitude vraie de la Terre dans son orbite solaire, par |
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| 61 | ! rapport au point vernal (21 mars), en degrés) |
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| 62 | |
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| 63 | REAL pmu0(klon) ! mean of cosine of solar zenith angle during "pdtphys" |
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| 64 | REAL trash1 |
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| 65 | REAL trash2(klon) |
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| 66 | |
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| 67 | !------------------------------------------------------------- |
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| 68 | |
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| 69 | CALL assert(klon == (/size(q, 1), size(t_seri, 1), size(zmasse, 1), & |
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| 70 | size(rlat), size(rlon)/), "o3_chem klon") |
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| 71 | CALL assert(nbp_lev == (/size(q, 2), size(t_seri, 2), size(zmasse, 2)/), & |
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| 72 | "o3_chem nbp_lev") |
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| 73 | |
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| 74 | c = c_Mob + a4_mass * t_seri |
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| 75 | |
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| 76 | ! Compute coefficient "b": |
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| 77 | |
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| 78 | ! Heterogeneous chemistry is only at low temperature: |
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| 79 | where (t_seri < 195.) |
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| 80 | b = r_het_interm |
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| 81 | elsewhere |
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| 82 | b = 0. |
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| 83 | end where |
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| 84 | |
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| 85 | ! Heterogeneous chemistry is only during daytime: |
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| 86 | CALL orbite(real(julien), earth_long, trash1) |
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| 87 | CALL zenang(earth_long, gmtime, 0., pdtphys, rlat, rlon, pmu0, trash2) |
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| 88 | forall (k = 1: nbp_lev) |
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| 89 | where (pmu0 <= cos(87. / 180. * pi)) b(:, k) = 0. |
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| 90 | end forall |
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| 91 | |
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| 92 | b = b + a2 |
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| 93 | |
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| 94 | ! Midpoint method: |
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| 95 | |
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| 96 | ! Trial step to the midpoint: |
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| 97 | dq_o3_chem = o3_prod(q, zmasse, c, b) * pdtphys / 2 |
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| 98 | ! "Real" step across the whole interval: |
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| 99 | dq_o3_chem = o3_prod(q + dq_o3_chem, zmasse, c, b) * pdtphys |
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| 100 | q = q + dq_o3_chem |
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| 101 | |
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| 102 | ! Confine the mass fraction: |
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| 103 | q = min(max(q, 0.), .01) |
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| 104 | |
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| 105 | END SUBROUTINE o3_chem |
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| 106 | |
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| 107 | !************************************************* |
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| 108 | |
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| 109 | function o3_prod(q, zmasse, c, b) |
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| 110 | |
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| 111 | ! This function computes the production rate of ozone by chemistry. |
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| 112 | |
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| 113 | ! All the 2-dimensional arrays are on the partial "physics" grid. |
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| 114 | ! Their shape is "(/klon, nbp_lev/)". |
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| 115 | ! Index "(i, :)" is for longitude "rlon(i)", latitude "rlat(i)". |
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| 116 | |
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| 117 | USE regr_pr_comb_coefoz_m, ONLY: a6_mass |
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| 118 | USE lmdz_assert, ONLY: assert |
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| 119 | USE dimphy, ONLY: klon |
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| 120 | USE lmdz_grid_phy, ONLY: nbp_lev |
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| 121 | |
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| 122 | REAL, INTENT(IN):: q(:, :) ! mass fraction of ozone |
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| 123 | ! "q(:, k)" is at middle of layer "k".) |
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| 124 | |
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| 125 | REAL, INTENT(IN):: zmasse(:, :) |
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| 126 | ! (column-density of mass of air in a layer, in kg m-2) |
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| 127 | ! ("zmasse(:, k)" is for layer "k".) |
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| 128 | |
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| 129 | REAL, INTENT(IN):: c(:, :) |
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| 130 | ! (constant term during a time step in the net mass production |
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| 131 | ! rate of ozone by chemistry, per unit mass of air, in s-1) |
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| 132 | ! "c(:, k)" is at middle of layer "k".) |
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| 133 | |
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| 134 | REAL, INTENT(IN):: b(:, :) |
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| 135 | ! (coefficient of "q" in the net mass production rate of ozone by |
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| 136 | ! chemistry, per unit mass of air, in s-1) |
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| 137 | ! ("b(:, k)" is at middle of layer "k".) |
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| 138 | |
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| 139 | REAL o3_prod(klon, nbp_lev) |
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| 140 | ! (net mass production rate of ozone by chemistry, per unit mass |
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| 141 | ! of air, in s-1) |
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| 142 | ! ("o3_prod(:, k)" is at middle of layer "k".) |
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| 143 | |
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| 144 | ! Variables local to the procedure: |
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| 145 | |
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| 146 | REAL sigma_mass(klon, nbp_lev) |
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| 147 | ! (mass column-density of ozone above point, in kg m-2) |
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| 148 | ! ("sigma_mass(:, k)" is at middle of layer "k".) |
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| 149 | |
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| 150 | INTEGER k |
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| 151 | |
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| 152 | !------------------------------------------------------------------- |
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| 153 | |
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| 154 | CALL assert(klon == (/size(q, 1), size(zmasse, 1), size(c, 1), & |
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| 155 | size(b, 1)/), "o3_prod 1") |
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| 156 | CALL assert(nbp_lev == (/size(q, 2), size(zmasse, 2), size(c, 2), & |
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| 157 | size(b, 2)/), "o3_prod 2") |
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| 158 | |
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| 159 | ! Compute the column-density above the base of layer |
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| 160 | ! "k", and, as a first approximation, take it as column-density |
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| 161 | ! above the middle of layer "k": |
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| 162 | sigma_mass(:, nbp_lev) = zmasse(:, nbp_lev) * q(:, nbp_lev) ! top layer |
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| 163 | do k = nbp_lev - 1, 1, -1 |
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| 164 | sigma_mass(:, k) = sigma_mass(:, k+1) + zmasse(:, k) * q(:, k) |
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| 165 | END DO |
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| 166 | |
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| 167 | o3_prod = c + b * q + a6_mass * sigma_mass |
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| 168 | |
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| 169 | END FUNCTION o3_prod |
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| 170 | |
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| 171 | END MODULE o3_chem_m |
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