[834] | 1 | SUBROUTINE soil_tifeedback(ngrid,nsoil,icecover,newtherm_i) |
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[1036] | 2 | |
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| 3 | use tracer_mod, only: nqmx, igcm_h2o_ice, rho_ice |
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[1047] | 4 | use comsoil_h, only: layer, inertiedat |
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| 5 | use surfdat_h, only: watercaptag, inert_h2o_ice |
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[834] | 6 | IMPLICIT NONE |
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| 7 | |
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| 8 | c======================================================================= |
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| 9 | c Description : |
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| 10 | c Surface water ice / Thermal inertia feedback. |
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| 11 | c |
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| 12 | c When surface water-ice is thick enough, this routine creates a new |
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| 13 | c soil thermal inertia with three different layers : |
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| 14 | c - One layer of surface water ice (the thickness is given |
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| 15 | c by the variable icecover (in kg of ice per m2) and the thermal |
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[1224] | 16 | c inertia is prescribed by inert_h2o_ice (see surfdat_h)); |
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[834] | 17 | c - A transitional layer of mixed thermal inertia; |
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| 18 | c - A last layer of regolith below the ice cover whose thermal inertia |
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| 19 | c is equal to inertiedat. |
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| 20 | c |
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| 21 | c To use the model : |
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| 22 | c SET THE tifeedback LOGICAL TO ".true." in callphys.def. |
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| 23 | c |
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| 24 | c Author: J.-B. Madeleine Mars 2008 - Updated November 2012 |
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| 25 | c======================================================================= |
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| 26 | |
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| 27 | #include "dimensions.h" |
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| 28 | |
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| 29 | c Local variables |
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| 30 | c --------------- |
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| 31 | |
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| 32 | INTEGER :: ig ! Grid point (ngrid) |
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| 33 | INTEGER :: ik ! Grid point (nsoil) |
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| 34 | INTEGER :: iref ! Ice/Regolith boundary index |
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| 35 | INTEGER :: ngrid ! Number of horizontal grid points |
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| 36 | INTEGER :: nsoil ! Number of soil layers |
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| 37 | REAL :: icedepth ! Ice cover thickness (m) |
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| 38 | |
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| 39 | c Inputs |
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| 40 | c ------ |
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| 41 | |
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| 42 | REAL icecover(ngrid,nqmx) ! tracer on the surface (kg.m-2) |
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[1036] | 43 | ! (iq=igcm_h2o_ice) is surface |
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[834] | 44 | ! water ice |
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| 45 | c Outputs |
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| 46 | c ------- |
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| 47 | |
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| 48 | REAL newtherm_i(ngrid,nsoil) ! New soil thermal inertia |
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| 49 | |
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| 50 | c Initialization |
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| 51 | c -------------- |
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| 52 | |
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| 53 | newtherm_i(1:ngrid,1:nsoil) = 0 |
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| 54 | |
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| 55 | c Creating the new soil thermal inertia table |
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| 56 | c ------------------------------------------- |
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| 57 | DO ig=1,ngrid |
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| 58 | c Calculating the ice cover thickness |
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| 59 | icedepth=icecover(ig,igcm_h2o_ice)/rho_ice |
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[857] | 60 | c If the ice cover is too thick or watercaptag=true, |
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| 61 | c the entire column is changed : |
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| 62 | IF ((icedepth.ge.layer(nsoil)).or.(watercaptag(ig))) THEN |
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[834] | 63 | DO ik=1,nsoil |
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| 64 | newtherm_i(ig,ik)=inert_h2o_ice |
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| 65 | ENDDO |
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| 66 | c We neglect the effect of a very thin ice cover : |
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| 67 | ELSE IF (icedepth.lt.layer(1)) THEN |
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| 68 | DO ik=1,nsoil |
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| 69 | newtherm_i(ig,ik)=inertiedat(ig,ik) |
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| 70 | ENDDO |
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| 71 | ELSE |
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| 72 | c Ice/regolith boundary index : |
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| 73 | iref=1 |
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| 74 | c Otherwise, we find the ice/regolith boundary: |
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| 75 | DO ik=1,nsoil-1 |
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| 76 | IF ((icedepth.ge.layer(ik)).and. |
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| 77 | & (icedepth.lt.layer(ik+1))) THEN |
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| 78 | iref=ik+1 |
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| 79 | EXIT |
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| 80 | ENDIF |
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| 81 | ENDDO |
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| 82 | c And we change the thermal inertia: |
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| 83 | DO ik=1,iref-1 |
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| 84 | newtherm_i(ig,ik)=inert_h2o_ice |
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| 85 | ENDDO |
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| 86 | c Transition (based on the equations of thermal conduction): |
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| 87 | newtherm_i(ig,iref)=sqrt( (layer(iref)-layer(iref-1)) / |
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| 88 | & ( ((icedepth-layer(iref-1))/inert_h2o_ice**2) + |
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| 89 | & ((layer(iref)-icedepth)/inertiedat(ig,ik)**2) ) ) |
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| 90 | c Underlying regolith: |
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| 91 | DO ik=iref+1,nsoil |
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| 92 | newtherm_i(ig,ik)=inertiedat(ig,ik) |
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| 93 | ENDDO |
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| 94 | ENDIF ! icedepth |
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| 95 | ENDDO ! ig |
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| 96 | |
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| 97 | c======================================================================= |
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| 98 | RETURN |
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| 99 | END |
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