1 | subroutine growthrate(timestep,temp,pmid,ph2o,psat, |
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2 | & seq,rcrystal,growth) |
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3 | |
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4 | IMPLICIT NONE |
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5 | |
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6 | c======================================================================= |
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7 | c |
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8 | c Determination of the water ice crystal growth rate |
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9 | c |
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10 | c Authors: F. Montmessin |
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11 | c Adapted for the LMD/GCM by J.-B. Madeleine (October 2011) |
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12 | c |
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13 | c======================================================================= |
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14 | |
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15 | c----------------------------------------------------------------------- |
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16 | c declarations: |
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17 | c ------------- |
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18 | |
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19 | #include "dimensions.h" |
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20 | #include "dimphys.h" |
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21 | #include "comcstfi.h" |
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22 | #include "tracer.h" |
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23 | #include "microphys.h" |
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24 | |
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25 | c |
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26 | c arguments: |
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27 | c ---------- |
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28 | |
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29 | REAL timestep |
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30 | REAL temp ! temperature in the middle of the layer (K) |
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31 | REAL pmid ! pressure in the middle of the layer (K) |
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32 | REAL*8 ph2o ! water vapor partial pressure (Pa) |
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33 | REAL*8 psat ! water vapor saturation pressure (Pa) |
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34 | REAL rcrystal ! crystal radius before condensation (m) |
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35 | REAL*8 seq ! Equilibrium saturation ratio |
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36 | REAL*8 growth |
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37 | |
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38 | c local: |
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39 | c ------ |
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40 | |
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41 | REAL*8 k,Lv |
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42 | REAL*8 knudsen ! Knudsen number (gas mean free path/particle radius) |
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43 | REAL*8 afactor,Dv,lambda ! Intermediate computations for growth rate |
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44 | REAL*8 Rk,Rd |
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45 | |
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46 | c----------------------------------------------------------------------- |
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47 | c Ice particle growth rate by diffusion/impegement of water molecules |
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48 | c r.dr/dt = (S-Seq) / (Seq*Rk+Rd) |
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49 | c with r the crystal radius, Rk and Rd the resistances due to |
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50 | c latent heat release and to vapor diffusion respectively |
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51 | c----------------------------------------------------------------------- |
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52 | |
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53 | c - Equilibrium saturation accounting for KeLvin Effect |
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54 | c seq=exp(2*sigh2o*mh2o/(rho_ice*rgp*t*r)) |
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55 | c (already computed in improvedcloud.F) |
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56 | |
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57 | c - Thermal conductibility of CO2 |
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58 | k = (0.17913 * temp - 13.9789) * 4.184e-4 |
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59 | c - Latent heat of h2o (J.kg-1) |
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60 | Lv = (2834.3 |
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61 | & - 0.28 * (temp-To) |
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62 | & - 0.004 * (temp-To) * (temp-To) ) * 1.e+3 |
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63 | |
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64 | c - Constant to compute gas mean free path |
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65 | c l= (T/P)*a, with a = ( 0.707*8.31/(4*pi*molrad**2 * avogadro)) |
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66 | afactor = 0.707*rgp/(4 * pi * molco2 * molco2 * nav) |
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67 | |
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68 | c - Compute Dv, water vapor diffusion coefficient |
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69 | c accounting for both kinetic and continuum regime of diffusion, |
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70 | c the nature of which depending on the Knudsen number. |
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71 | |
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72 | Dv = 1./3. * sqrt( 8*kbz*temp/(pi*mh2o/nav) )* kbz * temp / |
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73 | & ( pi * pmid * (molco2+molh2o)*(molco2+molh2o) |
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74 | & * sqrt(1.+mh2o/mco2) ) |
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75 | |
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76 | knudsen = temp / pmid * afactor / rcrystal |
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77 | lambda = (1.333+0.71/knudsen) / (1.+1./knudsen) |
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78 | Dv = Dv / (1. + lambda * knudsen) |
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79 | |
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80 | c - Compute Rk |
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81 | Rk = Lv**2 * rho_ice * mh2o / (k*rgp*temp*temp) |
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82 | c - Compute Rd |
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83 | Rd = rgp * temp *rho_ice / (Dv*psat*mh2o) |
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84 | |
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85 | c - Compute growth=rdr/dt, then r(t+1)= sqrt(r(t)**2.+2.*growth*dt) |
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86 | growth = 1. / (seq*Rk+Rd) |
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87 | c growth = (ph2o/psat-seq) / (seq*Rk+Rd) |
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88 | c rf = sqrt( max( r**2.+2.*growth*timestep , 0. ) ) |
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89 | c dr = rf-r |
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90 | |
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91 | RETURN |
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92 | END |
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93 | |
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