| 1 | MODULE evol_h2o_ice_s_mod |
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| 2 | |
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| 3 | IMPLICIT NONE |
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| 4 | |
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| 5 | CONTAINS |
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| 6 | |
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| 7 | SUBROUTINE evol_h2o_ice_s(qsurf,tendencies_h2o_ice_phys,& |
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| 8 | iim_input,jjm_input,ngrid,cell_area,STOPPING,nslope) |
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| 9 | |
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| 10 | USE temps_mod_evol, ONLY: dt_pem |
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| 11 | use comslope_mod, ONLY: subslope_dist |
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| 12 | use criterion_pem_stop_mod, only: criterion_waterice_stop |
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| 13 | |
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| 14 | IMPLICIT NONE |
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| 15 | |
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| 16 | !======================================================================= |
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| 17 | ! |
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| 18 | ! Routine that compute the evolution of the water ice |
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| 19 | ! |
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| 20 | !======================================================================= |
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| 21 | |
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| 22 | ! arguments: |
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| 23 | ! ---------- |
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| 24 | |
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| 25 | ! INPUT |
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| 26 | |
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| 27 | INTEGER, intent(in) :: iim_input,jjm_input, ngrid,nslope ! # of grid points along longitude/latitude/ total |
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| 28 | REAL, intent(in) :: cell_area(ngrid) ! Area of each mesh grid |
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| 29 | |
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| 30 | ! OUTPUT |
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| 31 | REAL, INTENT(INOUT) :: qsurf(ngrid,nslope) ! physical point field : Previous and actual density of water ice |
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| 32 | LOGICAL, INTENT(INOUT) :: STOPPING ! Stopping criterion |
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| 33 | REAL, intent(inout) :: tendencies_h2o_ice_phys(ngrid,nslope) ! physical point field : Evolution of perenial ice over one year |
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| 34 | |
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| 35 | ! local: |
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| 36 | ! ---- |
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| 37 | |
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| 38 | INTEGER :: i,j,ig0,islope ! loop variable |
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| 39 | REAL :: pos_tend, neg_tend, real_coefficient,negative_part ! Variable to conserve water |
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| 40 | REAL :: new_tendencies(ngrid,nslope) ! Tendencies computed in order to conserve water ice on the surface, only exchange between surface are done |
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| 41 | |
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| 42 | !======================================================================= |
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| 43 | |
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| 44 | STOPPING=.false. |
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| 45 | |
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| 46 | pos_tend=0. |
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| 47 | neg_tend=0. |
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| 48 | if (ngrid.NE.1) then ! to make sure we are not in 1D |
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| 49 | ! We compute the amount of water accumulating and sublimating |
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| 50 | do i=1,ngrid |
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| 51 | do islope=1,nslope |
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| 52 | if (qsurf(i,islope).GT.0) then |
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| 53 | if (tendencies_h2o_ice_phys(i,islope).GT.0) then |
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| 54 | pos_tend=pos_tend+tendencies_h2o_ice_phys(i,islope)*cell_area(i)*subslope_dist(i,islope) |
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| 55 | else |
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| 56 | neg_tend=neg_tend-tendencies_h2o_ice_phys(i,islope)*cell_area(i)*subslope_dist(i,islope) |
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| 57 | endif |
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| 58 | endif |
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| 59 | enddo |
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| 60 | enddo |
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| 61 | ! We adapt the tendencies to conserve water and do only exchange between grid points |
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| 62 | if(neg_tend.GT.pos_tend .and. pos_tend.GT.0) then ! We are sublimating more in the planet than condensing |
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| 63 | do i=1,ngrid |
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| 64 | do islope=1,nslope |
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| 65 | if(tendencies_h2o_ice_phys(i,islope).LT.0) then ! We lower the sublimating rate by a coefficient |
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| 66 | new_tendencies(i,islope)=tendencies_h2o_ice_phys(i,islope)*(pos_tend/neg_tend) |
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| 67 | else ! We dont't change the accumulating rate |
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| 68 | new_tendencies(i,islope)=tendencies_h2o_ice_phys(i,islope) |
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| 69 | endif |
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| 70 | enddo |
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| 71 | enddo |
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| 72 | elseif(neg_tend.LT.pos_tend .and. neg_tend.GT.0) then ! We are condensing more in the planet than sublimating |
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| 73 | do i=1,ngrid |
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| 74 | do islope=1,nslope |
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| 75 | if(tendencies_h2o_ice_phys(i,islope).LT.0) then ! We dont't change the sublimating rate |
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| 76 | new_tendencies(i,islope)=tendencies_h2o_ice_phys(i,islope) |
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| 77 | else ! We lower the condensing rate by a coefficient |
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| 78 | new_tendencies(i,islope)=tendencies_h2o_ice_phys(i,islope)*(neg_tend/pos_tend) |
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| 79 | endif |
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| 80 | enddo |
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| 81 | enddo |
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| 82 | elseif(pos_tend.EQ.0 .OR. neg_tend.EQ.0) then |
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| 83 | print *, "Reason of stopping : There is either no water ice sublimating or no water ice increasing !!" |
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| 84 | print *, "Tendencies on ice sublimating=", neg_tend |
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| 85 | print *, "Tendencies on ice increasing=", pos_tend |
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| 86 | print *, "This can be due to the absence of water ice in the PCM run!!" |
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| 87 | call criterion_waterice_stop(cell_area,1.,qsurf(:,:)*0.,STOPPING,ngrid,qsurf(:,:)*0.) |
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| 88 | do i=1,ngrid |
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| 89 | do islope=1,nslope |
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| 90 | new_tendencies(i,islope)=0 |
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| 91 | enddo |
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| 92 | enddo |
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| 93 | endif |
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| 94 | negative_part = 0. |
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| 95 | |
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| 96 | ! Evolution of the water ice for each physical point |
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| 97 | do i=1,ngrid |
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| 98 | do islope=1, nslope |
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| 99 | qsurf(i,islope)=qsurf(i,islope)+new_tendencies(i,islope)*dt_pem |
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| 100 | ! We compute the amount of water that is sublimated in excess |
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| 101 | if (qsurf(i,islope).lt.0) then |
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| 102 | negative_part=negative_part-qsurf(i,islope)*cell_area(i)*subslope_dist(i,islope) |
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| 103 | qsurf(i,islope)=0. |
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| 104 | tendencies_h2o_ice_phys(i,islope)=0. |
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| 105 | endif |
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| 106 | enddo |
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| 107 | enddo |
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| 108 | |
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| 109 | |
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| 110 | if(pos_tend.eq.0) then |
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| 111 | real_coefficient = 0. |
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| 112 | else |
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| 113 | real_coefficient = negative_part/pos_tend ! We compute a coefficient by which we should remove the ice that has been added |
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| 114 | ! to places even if this ice was contributing to an unphysical negative amount |
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| 115 | ! of ice at other places |
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| 116 | endif |
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| 117 | do i=1,ngrid |
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| 118 | do islope=1, nslope |
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| 119 | if(new_tendencies(i,islope).GT.0) then ! In the place of accumulation of ice, we remove a bit of ice in order to conserve water |
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| 120 | qsurf(i,islope)=qsurf(i,islope)-new_tendencies(i,islope)*real_coefficient*dt_pem |
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| 121 | endif |
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| 122 | enddo |
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| 123 | enddo |
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| 124 | else ! ngrid==1; |
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| 125 | do islope=1, nslope |
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| 126 | qsurf(1,islope)=qsurf(1,islope)+tendencies_h2o_ice_phys(1,islope)*dt_pem |
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| 127 | enddo |
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| 128 | endif |
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| 129 | |
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| 130 | END SUBROUTINE evol_h2o_ice_s |
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| 131 | |
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| 132 | END MODULE evol_h2o_ice_s_mod |
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