1 | subroutine spreadglacier_simple(ngrid,nq,pqsurf,timstep) |
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2 | |
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3 | use geometry_mod, only: latitude, longitude, cell_area |
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4 | use surfdat_h, only: phisfi |
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5 | use tracer_h, only: igcm_n2 |
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6 | |
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7 | implicit none |
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8 | |
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9 | !================================================================== |
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10 | ! Purpose |
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11 | ! ------- |
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12 | ! Spreading the glacier in a circular crater using a speed of flow |
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13 | ! |
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14 | ! Inputs |
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15 | ! ------ |
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16 | ! ngrid Number of vertical columns |
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17 | ! pqsurf(ngrid,nq) N2 ice tracer on surface kg/m2 |
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18 | ! |
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19 | ! Outputs |
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20 | ! ------- |
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21 | ! pqsurf(ngrid,nq) new value for N2 ice tracer on surface kg/m2 |
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22 | ! |
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23 | ! Authors |
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24 | ! ------- |
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25 | ! Tanguy Bertrand (2015) |
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26 | ! |
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27 | !================================================================== |
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28 | |
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29 | #include "dimensions.h" |
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30 | |
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31 | !----------------------------------------------------------------------- |
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32 | ! Arguments |
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33 | |
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34 | INTEGER ngrid, nq, ig, ig2 |
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35 | REAL :: pqsurf(ngrid,nq) |
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36 | REAL timstep |
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37 | !----------------------------------------------------------------------- |
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38 | ! Local variables |
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39 | |
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40 | REAL :: zdqsurf(ngrid) |
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41 | REAL phiref |
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42 | REAL dist |
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43 | REAL locdist |
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44 | REAL tau |
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45 | REAL speed |
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46 | REAL dist_pluto2 ! function |
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47 | LOGICAL firstcall |
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48 | DATA firstcall/.true./ |
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49 | INTEGER,SAVE,ALLOCATABLE :: indglac(:) |
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50 | INTEGER, SAVE :: nglac |
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51 | |
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52 | !---------------- INPUT ------------------------------------------------ |
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53 | ! Defined for Tombaugh crater : |
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54 | |
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55 | dist=300. ! reference radius km |
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56 | phiref=-1000. ! geopotential reference |
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57 | ! tau=1.e10 |
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58 | speed=6.4e-7 ! glacier speed km/s |
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59 | ! tau=1. ! direct redistribution glacier |
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60 | |
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61 | !--------------- FIRSTCALL : define crater index ----------------------- |
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62 | IF (firstcall) then |
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63 | ALLOCATE(indglac(ngrid)) |
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64 | nglac=0 |
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65 | indglac(:)=0 |
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66 | DO ig=1,ngrid |
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67 | IF (phisfi(ig).lt.phiref) THEN |
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68 | nglac=nglac+1 |
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69 | indglac(nglac)=ig |
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70 | ENDIF |
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71 | ENDDO |
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72 | firstcall=.false. |
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73 | |
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74 | ENDIF |
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75 | !--------------- redistribution ------------------------------------- |
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76 | DO ig=1,nglac |
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77 | ! redistribution if large amount of ice only : detection of reservoirs |
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78 | IF (pqsurf(indglac(ig),igcm_n2).gt.50.) THEN |
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79 | ! looking where to redistribute : if less ice, lower altitude |
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80 | ! and close to the reservoir |
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81 | DO ig2=1,nglac |
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82 | IF ((pqsurf(indglac(ig2),igcm_n2).lt.pqsurf(indglac(ig),igcm_n2)*0.8)) THEN |
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83 | !write(*,*) 'loop=',latitude(indglac(ig2))*180/3.14,longitude(indglac(ig2))*180/3.14 |
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84 | !.and.(phisfi(indglac(ig2)).le.phisfi(indglac(ig)))) THEN |
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85 | locdist=dist_pluto2(latitude(indglac(ig2)),longitude(indglac(ig2)),latitude(indglac(ig)),longitude(indglac(ig))) |
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86 | !write(*,*) 'dist=',locdist |
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87 | IF (locdist.lt.dist) THEN |
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88 | !write(*,*) 'calcul=',latitude(indglac(ig2))*180/3.14,longitude(indglac(ig2))*180/3.14,latitude(indglac(ig))*180/3.14,longitude(indglac(ig))*180/3.14 |
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89 | tau=locdist/speed ! characteristic time for redistribution |
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90 | zdqsurf(indglac(ig2))=pqsurf(indglac(ig),igcm_n2)*(1.-exp(-timstep/tau))/timstep*cell_area(indglac(ig))/cell_area(indglac(ig2)) |
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91 | zdqsurf(indglac(ig))=pqsurf(indglac(ig),igcm_n2)*(exp(-timstep/tau)-1.)/timstep |
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92 | pqsurf(indglac(ig2),igcm_n2)=pqsurf(indglac(ig2),igcm_n2)+zdqsurf(indglac(ig2))*timstep |
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93 | pqsurf(indglac(ig),igcm_n2)=pqsurf(indglac(ig),igcm_n2)+zdqsurf(indglac(ig))*timstep |
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94 | ENDIF |
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95 | ENDIF |
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96 | ENDDO |
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97 | ENDIF |
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98 | ENDDO |
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99 | |
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100 | end subroutine spreadglacier_simple |
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101 | |
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102 | real function dist_pluto2(lat1,lon1,lat2,lon2) |
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103 | implicit none |
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104 | !#include "comcstfi.h" |
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105 | real, intent(in) :: lat1,lon1,lat2,lon2 |
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106 | real dlon,dlat |
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107 | real a,c,d |
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108 | real rad |
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109 | rad=1187. ! planetary radius (km) 1187 km sur Pluton |
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110 | |
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111 | dlon = lon2 - lon1 |
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112 | dlat = lat2 - lat1 |
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113 | a = (sin(dlat/2))**2 + cos(lat1) * cos(lat2) * (sin(dlon/2))**2 |
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114 | c = 2 * atan2( sqrt(a), sqrt(1-a) ) |
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115 | dist_pluto2 = rad * c |
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116 | return |
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117 | end function dist_pluto2 |
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118 | |
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119 | |
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