| [2017] | 1 | !--------------------------------------------------------------------- |
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| 2 | ! Interpolation forcing in time and onto model levels |
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| 3 | !--------------------------------------------------------------------- |
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| 4 | if (forcing_GCSSold) then |
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| 5 | |
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| [2019] | 6 | call get_uvd(it,timestep,fich_gcssold_ctl,fich_gcssold_dat, & |
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| 7 | & ht_gcssold,hq_gcssold,hw_gcssold, & |
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| 8 | & hu_gcssold,hv_gcssold, & |
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| 9 | & hthturb_gcssold,hqturb_gcssold,Ts_gcssold, & |
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| 10 | & imp_fcg_gcssold,ts_fcg_gcssold, & |
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| 11 | & Tp_fcg_gcssold,Turb_fcg_gcssold) |
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| [2017] | 12 | if (prt_level.ge.1) then |
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| 13 | print *,' get_uvd -> hqturb_gcssold ',it,hqturb_gcssold |
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| 14 | endif |
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| 15 | ! large-scale forcing : |
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| 16 | !!! tsurf = ts_gcssold |
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| 17 | do l = 1, llm |
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| 18 | ! u(l) = hu_gcssold(l) ! on prescrit le vent |
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| 19 | ! v(l) = hv_gcssold(l) ! on prescrit le vent |
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| 20 | ! omega(l) = hw_gcssold(l) |
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| 21 | ! rho(l) = play(l)/(rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))) |
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| 22 | ! omega2(l)=-rho(l)*omega(l) |
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| 23 | omega(l) = hw_gcssold(l) |
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| 24 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
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| 25 | |
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| 26 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
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| 27 | d_th_adv(l) = ht_gcssold(l) |
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| 28 | d_q_adv(l,1) = hq_gcssold(l) |
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| 29 | dt_cooling(l) = 0.0 |
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| 30 | enddo |
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| 31 | |
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| 32 | endif ! forcing_GCSSold |
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| 33 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 34 | !--------------------------------------------------------------------- |
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| 35 | ! Interpolation Toga forcing |
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| 36 | !--------------------------------------------------------------------- |
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| 37 | if (forcing_toga) then |
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| 38 | |
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| 39 | if (prt_level.ge.1) then |
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| [2019] | 40 | print*, & |
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| 41 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_toga=', & |
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| 42 | & day,day1,(day-day1)*86400.,(day-day1)*86400/dt_toga |
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| [2017] | 43 | endif |
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| 44 | |
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| 45 | ! time interpolation: |
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| [2019] | 46 | CALL interp_toga_time(daytime,day1,annee_ref & |
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| 47 | & ,year_ini_toga,day_ju_ini_toga,nt_toga,dt_toga & |
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| 48 | & ,nlev_toga,ts_toga,plev_toga,t_toga,q_toga,u_toga & |
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| 49 | & ,v_toga,w_toga,ht_toga,vt_toga,hq_toga,vq_toga & |
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| 50 | & ,ts_prof,plev_prof,t_prof,q_prof,u_prof,v_prof,w_prof & |
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| 51 | & ,ht_prof,vt_prof,hq_prof,vq_prof) |
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| [2017] | 52 | |
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| 53 | if (type_ts_forcing.eq.1) ts_cur = ts_prof ! SST used in read_tsurf1d |
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| 54 | |
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| 55 | ! vertical interpolation: |
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| [2019] | 56 | CALL interp_toga_vertical(play,nlev_toga,plev_prof & |
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| 57 | & ,t_prof,q_prof,u_prof,v_prof,w_prof & |
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| 58 | & ,ht_prof,vt_prof,hq_prof,vq_prof & |
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| 59 | & ,t_mod,q_mod,u_mod,v_mod,w_mod & |
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| 60 | & ,ht_mod,vt_mod,hq_mod,vq_mod,mxcalc) |
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| [2017] | 61 | |
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| 62 | ! large-scale forcing : |
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| 63 | tsurf = ts_prof |
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| 64 | do l = 1, llm |
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| 65 | u(l) = u_mod(l) ! sb: on prescrit le vent |
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| 66 | v(l) = v_mod(l) ! sb: on prescrit le vent |
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| 67 | ! omega(l) = w_prof(l) |
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| 68 | ! rho(l) = play(l)/(rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))) |
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| 69 | ! omega2(l)=-rho(l)*omega(l) |
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| 70 | omega(l) = w_mod(l) |
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| 71 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
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| 72 | |
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| 73 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
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| 74 | d_th_adv(l) = alpha*omega(l)/rcpd-(ht_mod(l)+vt_mod(l)) |
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| 75 | d_q_adv(l,1) = -(hq_mod(l)+vq_mod(l)) |
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| 76 | dt_cooling(l) = 0.0 |
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| 77 | enddo |
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| 78 | |
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| 79 | endif ! forcing_toga |
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| 80 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| [2126] | 81 | ! Interpolation DICE forcing |
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| [2017] | 82 | !--------------------------------------------------------------------- |
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| [2126] | 83 | if (forcing_dice) then |
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| 84 | |
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| 85 | if (prt_level.ge.1) then |
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| 86 | print*,'#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_dice=',& |
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| 87 | & day,day1,(day-day1)*86400.,(day-day1)*86400/dt_dice |
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| 88 | endif |
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| 89 | |
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| 90 | ! time interpolation: |
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| 91 | CALL interp_dice_time(daytime,day1,annee_ref & |
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| 92 | & ,year_ini_dice,day_ju_ini_dice,nt_dice,dt_dice & |
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| 93 | & ,nlev_dice,shf_dice,lhf_dice,lwup_dice,swup_dice & |
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| 94 | & ,tg_dice,ustar_dice,psurf_dice,ug_dice,vg_dice & |
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| 95 | & ,ht_dice,hq_dice,hu_dice,hv_dice,w_dice,omega_dice & |
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| 96 | & ,shf_prof,lhf_prof,lwup_prof,swup_prof,tg_prof & |
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| 97 | & ,ustar_prof,psurf_prof,ug_profd,vg_profd & |
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| 98 | & ,ht_profd,hq_profd,hu_profd,hv_profd,w_profd & |
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| 99 | & ,omega_profd) |
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| 100 | ! do l = 1, llm |
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| 101 | ! print *,'llm l omega_profd',llm,l,omega_profd(l) |
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| 102 | ! enddo |
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| 103 | |
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| 104 | if (type_ts_forcing.eq.1) ts_cur = tg_prof ! SST used in read_tsurf1d |
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| 105 | |
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| 106 | ! vertical interpolation: |
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| 107 | CALL interp_dice_vertical(play,nlev_dice,nt_dice,plev_dice & |
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| 108 | & ,th_dice,qv_dice,u_dice,v_dice,o3_dice & |
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| 109 | & ,ht_profd,hq_profd,hu_profd,hv_profd,w_profd,omega_profd & |
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| 110 | & ,th_mod,qv_mod,u_mod,v_mod,o3_mod & |
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| 111 | & ,ht_mod,hq_mod,hu_mod,hv_mod,w_mod,omega_mod,mxcalc) |
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| 112 | ! do l = 1, llm |
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| 113 | ! print *,'llm l omega_mod',llm,l,omega_mod(l) |
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| 114 | ! enddo |
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| 115 | |
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| 116 | ! Les forcages DICE sont donnes /jour et non /seconde ! |
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| 117 | ht_mod(:)=ht_mod(:)/86400. |
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| 118 | hq_mod(:)=hq_mod(:)/86400. |
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| 119 | hu_mod(:)=hu_mod(:)/86400. |
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| 120 | hv_mod(:)=hv_mod(:)/86400. |
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| 121 | |
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| 122 | !calcul de l'advection verticale a partir du omega (repris cas TWPICE, MPL 05082013) |
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| 123 | !Calcul des gradients verticaux |
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| 124 | !initialisation |
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| 125 | d_t_z(:)=0. |
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| 126 | d_q_z(:)=0. |
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| 127 | d_u_z(:)=0. |
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| 128 | d_v_z(:)=0. |
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| 129 | DO l=2,llm-1 |
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| 130 | d_t_z(l)=(temp(l+1)-temp(l-1))/(play(l+1)-play(l-1)) |
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| 131 | d_q_z(l)=(q(l+1,1)-q(l-1,1)) /(play(l+1)-play(l-1)) |
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| 132 | d_u_z(l)=(u(l+1)-u(l-1))/(play(l+1)-play(l-1)) |
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| 133 | d_v_z(l)=(v(l+1)-v(l-1))/(play(l+1)-play(l-1)) |
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| 134 | ENDDO |
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| 135 | d_t_z(1)=d_t_z(2) |
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| 136 | d_q_z(1)=d_q_z(2) |
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| 137 | ! d_u_z(1)=u(2)/(play(2)-psurf)/5. |
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| 138 | ! d_v_z(1)=v(2)/(play(2)-psurf)/5. |
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| 139 | d_u_z(1)=0. |
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| 140 | d_v_z(1)=0. |
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| 141 | d_t_z(llm)=d_t_z(llm-1) |
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| 142 | d_q_z(llm)=d_q_z(llm-1) |
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| 143 | d_u_z(llm)=d_u_z(llm-1) |
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| 144 | d_v_z(llm)=d_v_z(llm-1) |
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| 145 | |
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| 146 | !Calcul de l advection verticale: |
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| 147 | ! utiliser omega (Pa/s) et non w (m/s) !! MP 20131108 |
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| 148 | d_t_dyn_z(:)=omega_mod(:)*d_t_z(:) |
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| 149 | d_q_dyn_z(:)=omega_mod(:)*d_q_z(:) |
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| 150 | d_u_dyn_z(:)=omega_mod(:)*d_u_z(:) |
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| 151 | d_v_dyn_z(:)=omega_mod(:)*d_v_z(:) |
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| 152 | |
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| 153 | ! large-scale forcing : |
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| 154 | ! tsurf = tg_prof MPL 20130925 commente |
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| 155 | psurf = psurf_prof |
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| 156 | ! For this case, fluxes are imposed |
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| 157 | fsens=-1*shf_prof |
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| 158 | flat=-1*lhf_prof |
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| 159 | ust=ustar_prof |
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| 160 | tg=tg_prof |
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| 161 | print *,'ust= ',ust |
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| 162 | do l = 1, llm |
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| 163 | ug(l)= ug_profd |
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| 164 | vg(l)= vg_profd |
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| 165 | ! omega(l) = w_prof(l) |
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| 166 | ! rho(l) = play(l)/(rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))) |
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| 167 | ! omega2(l)=-rho(l)*omega(l) |
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| 168 | ! omega(l) = w_mod(l)*(-rg*rho(l)) |
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| 169 | omega(l) = omega_mod(l) |
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| 170 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
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| 171 | |
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| 172 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
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| 173 | d_th_adv(l) = alpha*omega(l)/rcpd+ht_mod(l)-d_t_dyn_z(l) |
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| 174 | d_q_adv(l,1) = hq_mod(l)-d_q_dyn_z(l) |
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| 175 | d_u_adv(l) = hu_mod(l)-d_u_dyn_z(l) |
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| 176 | d_v_adv(l) = hv_mod(l)-d_v_dyn_z(l) |
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| 177 | dt_cooling(l) = 0.0 |
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| 178 | enddo |
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| 179 | |
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| 180 | endif ! forcing_dice |
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| 181 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 182 | !--------------------------------------------------------------------- |
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| 183 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 184 | !--------------------------------------------------------------------- |
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| [2017] | 185 | ! Interpolation forcing TWPice |
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| 186 | !--------------------------------------------------------------------- |
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| 187 | if (forcing_twpice) then |
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| 188 | |
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| [2019] | 189 | print*, & |
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| 190 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_twpi=', & |
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| 191 | & daytime,day1,(daytime-day1)*86400., & |
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| 192 | & (daytime-day1)*86400/dt_twpi |
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| [2017] | 193 | |
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| 194 | ! time interpolation: |
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| [2019] | 195 | CALL interp_toga_time(daytime,day1,annee_ref & |
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| 196 | & ,year_ini_twpi,day_ju_ini_twpi,nt_twpi,dt_twpi,nlev_twpi & |
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| 197 | & ,ts_twpi,plev_twpi,t_twpi,q_twpi,u_twpi,v_twpi,w_twpi & |
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| 198 | & ,ht_twpi,vt_twpi,hq_twpi,vq_twpi & |
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| 199 | & ,ts_proftwp,plev_proftwp,t_proftwp,q_proftwp,u_proftwp & |
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| 200 | & ,v_proftwp,w_proftwp & |
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| 201 | & ,ht_proftwp,vt_proftwp,hq_proftwp,vq_proftwp) |
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| [2017] | 202 | |
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| 203 | ! vertical interpolation: |
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| [2019] | 204 | CALL interp_toga_vertical(play,nlev_twpi,plev_proftwp & |
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| 205 | & ,t_proftwp,q_proftwp,u_proftwp,v_proftwp,w_proftwp & |
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| 206 | & ,ht_proftwp,vt_proftwp,hq_proftwp,vq_proftwp & |
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| 207 | & ,t_mod,q_mod,u_mod,v_mod,w_mod & |
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| 208 | & ,ht_mod,vt_mod,hq_mod,vq_mod,mxcalc) |
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| [2017] | 209 | |
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| 210 | |
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| 211 | !calcul de l'advection verticale a partir du omega |
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| [2019] | 212 | !Calcul des gradients verticaux |
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| 213 | !initialisation |
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| [2017] | 214 | d_t_z(:)=0. |
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| 215 | d_q_z(:)=0. |
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| 216 | d_t_dyn_z(:)=0. |
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| 217 | d_q_dyn_z(:)=0. |
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| 218 | DO l=2,llm-1 |
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| [2019] | 219 | d_t_z(l)=(temp(l+1)-temp(l-1))/(play(l+1)-play(l-1)) |
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| 220 | d_q_z(l)=(q(l+1,1)-q(l-1,1))/(play(l+1)-play(l-1)) |
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| [2017] | 221 | ENDDO |
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| 222 | d_t_z(1)=d_t_z(2) |
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| 223 | d_q_z(1)=d_q_z(2) |
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| 224 | d_t_z(llm)=d_t_z(llm-1) |
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| 225 | d_q_z(llm)=d_q_z(llm-1) |
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| 226 | |
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| [2019] | 227 | !Calcul de l advection verticale |
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| [2017] | 228 | d_t_dyn_z(:)=w_mod(:)*d_t_z(:) |
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| 229 | d_q_dyn_z(:)=w_mod(:)*d_q_z(:) |
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| 230 | |
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| 231 | !wind nudging above 500m with a 2h time scale |
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| 232 | do l=1,llm |
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| 233 | if (nudge_wind) then |
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| 234 | ! if (phi(l).gt.5000.) then |
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| 235 | if (phi(l).gt.0.) then |
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| [2019] | 236 | u(l)=u(l)+timestep*(u_mod(l)-u(l))/(2.*3600.) |
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| 237 | v(l)=v(l)+timestep*(v_mod(l)-v(l))/(2.*3600.) |
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| [2017] | 238 | endif |
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| 239 | else |
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| 240 | u(l) = u_mod(l) |
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| 241 | v(l) = v_mod(l) |
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| 242 | endif |
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| 243 | enddo |
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| 244 | |
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| 245 | !CR:nudging of q and theta with a 6h time scale above 15km |
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| 246 | if (nudge_thermo) then |
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| 247 | do l=1,llm |
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| 248 | zz(l)=phi(l)/9.8 |
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| 249 | if ((zz(l).le.16000.).and.(zz(l).gt.15000.)) then |
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| 250 | zfact=(zz(l)-15000.)/1000. |
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| [2019] | 251 | q(l,1)=q(l,1)+timestep*(q_mod(l)-q(l,1))/(6.*3600.)*zfact |
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| 252 | temp(l)=temp(l)+timestep*(t_mod(l)-temp(l))/(6.*3600.)*zfact |
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| [2017] | 253 | else if (zz(l).gt.16000.) then |
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| [2019] | 254 | q(l,1)=q(l,1)+timestep*(q_mod(l)-q(l,1))/(6.*3600.) |
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| 255 | temp(l)=temp(l)+timestep*(t_mod(l)-temp(l))/(6.*3600.) |
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| [2017] | 256 | endif |
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| 257 | enddo |
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| 258 | endif |
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| 259 | |
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| 260 | do l = 1, llm |
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| 261 | omega(l) = w_mod(l) |
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| 262 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
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| 263 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
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| 264 | !calcul de l'advection totale |
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| 265 | if (cptadvw) then |
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| 266 | d_th_adv(l) = alpha*omega(l)/rcpd+ht_mod(l)-d_t_dyn_z(l) |
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| 267 | ! print*,'temp vert adv',l,ht_mod(l),vt_mod(l),-d_t_dyn_z(l) |
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| 268 | d_q_adv(l,1) = hq_mod(l)-d_q_dyn_z(l) |
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| 269 | ! print*,'q vert adv',l,hq_mod(l),vq_mod(l),-d_q_dyn_z(l) |
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| 270 | else |
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| 271 | d_th_adv(l) = alpha*omega(l)/rcpd+(ht_mod(l)+vt_mod(l)) |
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| 272 | d_q_adv(l,1) = (hq_mod(l)+vq_mod(l)) |
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| 273 | endif |
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| 274 | dt_cooling(l) = 0.0 |
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| 275 | enddo |
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| 276 | |
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| 277 | endif ! forcing_twpice |
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| 278 | |
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| 279 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 280 | !--------------------------------------------------------------------- |
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| 281 | ! Interpolation forcing AMMA |
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| 282 | !--------------------------------------------------------------------- |
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| 283 | |
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| 284 | if (forcing_amma) then |
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| 285 | |
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| [2019] | 286 | print*, & |
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| 287 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_amma=', & |
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| 288 | & daytime,day1,(daytime-day1)*86400., & |
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| 289 | & (daytime-day1)*86400/dt_amma |
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| [2017] | 290 | |
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| 291 | ! time interpolation using TOGA interpolation routine |
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| [2019] | 292 | CALL interp_amma_time(daytime,day1,annee_ref & |
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| 293 | & ,year_ini_amma,day_ju_ini_amma,nt_amma,dt_amma,nlev_amma & |
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| 294 | & ,vitw_amma,ht_amma,hq_amma,lat_amma,sens_amma & |
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| 295 | & ,vitw_profamma,ht_profamma,hq_profamma,lat_profamma & |
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| 296 | & ,sens_profamma) |
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| [2017] | 297 | |
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| 298 | print*,'apres interpolation temporelle AMMA' |
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| 299 | |
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| 300 | do k=1,nlev_amma |
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| 301 | th_profamma(k)=0. |
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| 302 | q_profamma(k)=0. |
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| 303 | u_profamma(k)=0. |
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| 304 | v_profamma(k)=0. |
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| 305 | vt_profamma(k)=0. |
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| 306 | vq_profamma(k)=0. |
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| 307 | enddo |
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| 308 | ! vertical interpolation using TOGA interpolation routine: |
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| 309 | ! write(*,*)'avant interp vert', t_proftwp |
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| [2019] | 310 | CALL interp_toga_vertical(play,nlev_amma,plev_amma & |
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| 311 | & ,th_profamma,q_profamma,u_profamma,v_profamma & |
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| 312 | & ,vitw_profamma & |
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| 313 | & ,ht_profamma,vt_profamma,hq_profamma,vq_profamma & |
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| 314 | & ,t_mod,q_mod,u_mod,v_mod,w_mod & |
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| 315 | & ,ht_mod,vt_mod,hq_mod,vq_mod,mxcalc) |
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| [2017] | 316 | write(*,*) 'Profil initial forcing AMMA interpole' |
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| 317 | |
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| 318 | |
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| 319 | !calcul de l'advection verticale a partir du omega |
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| [2019] | 320 | !Calcul des gradients verticaux |
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| 321 | !initialisation |
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| [2017] | 322 | do l=1,llm |
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| 323 | d_t_z(l)=0. |
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| 324 | d_q_z(l)=0. |
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| 325 | enddo |
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| 326 | |
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| 327 | DO l=2,llm-1 |
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| [2019] | 328 | d_t_z(l)=(temp(l+1)-temp(l-1))/(play(l+1)-play(l-1)) |
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| 329 | d_q_z(l)=(q(l+1,1)-q(l-1,1))/(play(l+1)-play(l-1)) |
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| [2017] | 330 | ENDDO |
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| 331 | d_t_z(1)=d_t_z(2) |
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| 332 | d_q_z(1)=d_q_z(2) |
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| 333 | d_t_z(llm)=d_t_z(llm-1) |
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| 334 | d_q_z(llm)=d_q_z(llm-1) |
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| 335 | |
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| 336 | |
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| 337 | do l = 1, llm |
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| 338 | rho(l) = play(l)/(rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))) |
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| 339 | omega(l) = w_mod(l)*(-rg*rho(l)) |
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| 340 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
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| 341 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
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| 342 | !calcul de l'advection totale |
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| 343 | ! d_th_adv(l) = alpha*omega(l)/rcpd+ht_mod(l)-omega(l)*d_t_z(l) |
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| 344 | !attention: on impose dth |
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| [2019] | 345 | d_th_adv(l) = alpha*omega(l)/rcpd+ & |
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| [2017] | 346 | & ht_mod(l)*(play(l)/pzero)**rkappa-omega(l)*d_t_z(l) |
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| 347 | ! d_th_adv(l) = 0. |
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| 348 | ! print*,'temp vert adv',l,ht_mod(l),vt_mod(l),-d_t_dyn_z(l) |
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| 349 | d_q_adv(l,1) = hq_mod(l)-omega(l)*d_q_z(l) |
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| 350 | ! d_q_adv(l,1) = 0. |
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| 351 | ! print*,'q vert adv',l,hq_mod(l),vq_mod(l),-d_q_dyn_z(l) |
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| 352 | |
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| 353 | dt_cooling(l) = 0.0 |
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| 354 | enddo |
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| 355 | |
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| 356 | |
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| 357 | ! ok_flux_surf=.false. |
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| 358 | fsens=-1.*sens_profamma |
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| 359 | flat=-1.*lat_profamma |
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| 360 | |
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| 361 | endif ! forcing_amma |
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| 362 | |
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| 363 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
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| 364 | !--------------------------------------------------------------------- |
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| 365 | ! Interpolation forcing Rico |
|---|
| 366 | !--------------------------------------------------------------------- |
|---|
| 367 | if (forcing_rico) then |
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| 368 | ! call lstendH(llm,omega,dt_dyn,dq_dyn,du_dyn, dv_dyn, |
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| 369 | ! : q,temp,u,v,play) |
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| [2019] | 370 | call lstendH(llm,nqtot,omega,dt_dyn,dq_dyn,q,temp,u,v,play) |
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| [2017] | 371 | |
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| 372 | do l=1,llm |
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| 373 | d_th_adv(l) = (dth_rico(l) + dt_dyn(l)) |
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| 374 | d_q_adv(l,1) = (dqh_rico(l) + dq_dyn(l,1)) |
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| 375 | d_q_adv(l,2) = 0. |
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| 376 | enddo |
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| 377 | endif ! forcing_rico |
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| 378 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 379 | !--------------------------------------------------------------------- |
|---|
| 380 | ! Interpolation forcing Arm_cu |
|---|
| 381 | !--------------------------------------------------------------------- |
|---|
| 382 | if (forcing_armcu) then |
|---|
| 383 | |
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| [2019] | 384 | print*, & |
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| 385 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_armcu=', & |
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| 386 | & day,day1,(day-day1)*86400.,(day-day1)*86400/dt_armcu |
|---|
| [2017] | 387 | |
|---|
| 388 | ! time interpolation: |
|---|
| 389 | ! ATTENTION, cet appel ne convient pas pour TOGA !! |
|---|
| 390 | ! revoir 1DUTILS.h et les arguments |
|---|
| [2019] | 391 | CALL interp_armcu_time(daytime,day1,annee_ref & |
|---|
| 392 | & ,year_ini_armcu,day_ju_ini_armcu,nt_armcu,dt_armcu & |
|---|
| 393 | & ,nlev_armcu,sens_armcu,flat_armcu,adv_theta_armcu & |
|---|
| 394 | & ,rad_theta_armcu,adv_qt_armcu,sens_prof,flat_prof & |
|---|
| 395 | & ,adv_theta_prof,rad_theta_prof,adv_qt_prof) |
|---|
| [2017] | 396 | |
|---|
| 397 | ! vertical interpolation: |
|---|
| 398 | ! No vertical interpolation if nlev imposed to 19 or 40 |
|---|
| 399 | |
|---|
| 400 | ! For this case, fluxes are imposed |
|---|
| 401 | fsens=-1*sens_prof |
|---|
| 402 | flat=-1*flat_prof |
|---|
| 403 | |
|---|
| 404 | ! Advective forcings are given in K or g/kg ... BY HOUR |
|---|
| 405 | do l = 1, llm |
|---|
| 406 | ug(l)= u_mod(l) |
|---|
| 407 | vg(l)= v_mod(l) |
|---|
| 408 | IF((phi(l)/RG).LT.1000) THEN |
|---|
| 409 | d_th_adv(l) = (adv_theta_prof + rad_theta_prof)/3600. |
|---|
| 410 | d_q_adv(l,1) = adv_qt_prof/1000./3600. |
|---|
| 411 | d_q_adv(l,2) = 0.0 |
|---|
| 412 | ! print *,'INF1000: phi dth dq1 dq2', |
|---|
| 413 | ! : phi(l)/RG,d_th_adv(l),d_q_adv(l,1),d_q_adv(l,2) |
|---|
| 414 | ELSEIF ((phi(l)/RG).GE.1000.AND.(phi(l)/RG).lt.3000) THEN |
|---|
| 415 | fact=((phi(l)/RG)-1000.)/2000. |
|---|
| 416 | fact=1-fact |
|---|
| 417 | d_th_adv(l) = (adv_theta_prof + rad_theta_prof)*fact/3600. |
|---|
| 418 | d_q_adv(l,1) = adv_qt_prof*fact/1000./3600. |
|---|
| 419 | d_q_adv(l,2) = 0.0 |
|---|
| 420 | ! print *,'SUP1000: phi fact dth dq1 dq2', |
|---|
| 421 | ! : phi(l)/RG,fact,d_th_adv(l),d_q_adv(l,1),d_q_adv(l,2) |
|---|
| 422 | ELSE |
|---|
| 423 | d_th_adv(l) = 0.0 |
|---|
| 424 | d_q_adv(l,1) = 0.0 |
|---|
| 425 | d_q_adv(l,2) = 0.0 |
|---|
| 426 | ! print *,'SUP3000: phi dth dq1 dq2', |
|---|
| 427 | ! : phi(l)/RG,d_th_adv(l),d_q_adv(l,1),d_q_adv(l,2) |
|---|
| 428 | ENDIF |
|---|
| 429 | dt_cooling(l) = 0.0 |
|---|
| 430 | ! print *,'Interp armcu: phi dth dq1 dq2', |
|---|
| 431 | ! : l,phi(l),d_th_adv(l),d_q_adv(l,1),d_q_adv(l,2) |
|---|
| 432 | enddo |
|---|
| 433 | endif ! forcing_armcu |
|---|
| 434 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 435 | !--------------------------------------------------------------------- |
|---|
| 436 | ! Interpolation forcing in time and onto model levels |
|---|
| 437 | !--------------------------------------------------------------------- |
|---|
| 438 | if (forcing_sandu) then |
|---|
| 439 | |
|---|
| [2019] | 440 | print*, & |
|---|
| 441 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_sandu=', & |
|---|
| 442 | & day,day1,(day-day1)*86400.,(day-day1)*86400/dt_sandu |
|---|
| [2017] | 443 | |
|---|
| 444 | ! time interpolation: |
|---|
| 445 | ! ATTENTION, cet appel ne convient pas pour TOGA !! |
|---|
| 446 | ! revoir 1DUTILS.h et les arguments |
|---|
| [2019] | 447 | CALL interp_sandu_time(daytime,day1,annee_ref & |
|---|
| 448 | & ,year_ini_sandu,day_ju_ini_sandu,nt_sandu,dt_sandu & |
|---|
| 449 | & ,nlev_sandu & |
|---|
| 450 | & ,ts_sandu,ts_prof) |
|---|
| [2017] | 451 | |
|---|
| 452 | if (type_ts_forcing.eq.1) ts_cur = ts_prof ! SST used in read_tsurf1d |
|---|
| 453 | |
|---|
| 454 | ! vertical interpolation: |
|---|
| [2019] | 455 | CALL interp_sandu_vertical(play,nlev_sandu,plev_profs & |
|---|
| 456 | & ,t_profs,thl_profs,q_profs,u_profs,v_profs,w_profs & |
|---|
| 457 | & ,omega_profs,o3mmr_profs & |
|---|
| 458 | & ,t_mod,thl_mod,q_mod,u_mod,v_mod,w_mod & |
|---|
| 459 | & ,omega_mod,o3mmr_mod,mxcalc) |
|---|
| [2017] | 460 | !calcul de l'advection verticale |
|---|
| [2019] | 461 | !Calcul des gradients verticaux |
|---|
| 462 | !initialisation |
|---|
| [2017] | 463 | d_t_z(:)=0. |
|---|
| 464 | d_q_z(:)=0. |
|---|
| 465 | d_t_dyn_z(:)=0. |
|---|
| 466 | d_q_dyn_z(:)=0. |
|---|
| 467 | ! schema centre |
|---|
| 468 | ! DO l=2,llm-1 |
|---|
| 469 | ! d_t_z(l)=(temp(l+1)-temp(l-1)) |
|---|
| 470 | ! & /(play(l+1)-play(l-1)) |
|---|
| 471 | ! d_q_z(l)=(q(l+1,1)-q(l-1,1)) |
|---|
| 472 | ! & /(play(l+1)-play(l-1)) |
|---|
| 473 | ! schema amont |
|---|
| 474 | DO l=2,llm-1 |
|---|
| 475 | d_t_z(l)=(temp(l+1)-temp(l))/(play(l+1)-play(l)) |
|---|
| 476 | d_q_z(l)=(q(l+1,1)-q(l,1))/(play(l+1)-play(l)) |
|---|
| 477 | ! print *,'l temp2 temp0 play2 play0 omega_mod', |
|---|
| 478 | ! & temp(l+1),temp(l-1),play(l+1),play(l-1),omega_mod(l) |
|---|
| 479 | ENDDO |
|---|
| 480 | d_t_z(1)=d_t_z(2) |
|---|
| 481 | d_q_z(1)=d_q_z(2) |
|---|
| 482 | d_t_z(llm)=d_t_z(llm-1) |
|---|
| 483 | d_q_z(llm)=d_q_z(llm-1) |
|---|
| 484 | |
|---|
| 485 | ! calcul de l advection verticale |
|---|
| 486 | ! Confusion w (m/s) et omega (Pa/s) !! |
|---|
| 487 | d_t_dyn_z(:)=omega_mod(:)*d_t_z(:) |
|---|
| 488 | d_q_dyn_z(:)=omega_mod(:)*d_q_z(:) |
|---|
| 489 | ! do l=1,llm |
|---|
| 490 | ! print *,'d_t_dyn omega_mod d_t_z d_q_dyn d_q_z', |
|---|
| 491 | ! :l,d_t_dyn_z(l),omega_mod(l),d_t_z(l),d_q_dyn_z(l),d_q_z(l) |
|---|
| 492 | ! enddo |
|---|
| 493 | |
|---|
| 494 | |
|---|
| 495 | ! large-scale forcing : pour le cas Sandu ces forcages sont la SST |
|---|
| 496 | ! et une divergence constante -> profil de omega |
|---|
| 497 | tsurf = ts_prof |
|---|
| 498 | write(*,*) 'SST suivante: ',tsurf |
|---|
| 499 | do l = 1, llm |
|---|
| 500 | omega(l) = omega_mod(l) |
|---|
| 501 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
|---|
| 502 | |
|---|
| 503 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
|---|
| 504 | ! |
|---|
| 505 | ! d_th_adv(l) = 0.0 |
|---|
| 506 | ! d_q_adv(l,1) = 0.0 |
|---|
| 507 | !CR:test advection=0 |
|---|
| 508 | !calcul de l'advection verticale |
|---|
| 509 | d_th_adv(l) = alpha*omega(l)/rcpd-d_t_dyn_z(l) |
|---|
| 510 | ! print*,'temp adv',l,-d_t_dyn_z(l) |
|---|
| 511 | d_q_adv(l,1) = -d_q_dyn_z(l) |
|---|
| 512 | ! print*,'q adv',l,-d_q_dyn_z(l) |
|---|
| 513 | dt_cooling(l) = 0.0 |
|---|
| 514 | enddo |
|---|
| 515 | endif ! forcing_sandu |
|---|
| 516 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 517 | !--------------------------------------------------------------------- |
|---|
| 518 | ! Interpolation forcing in time and onto model levels |
|---|
| 519 | !--------------------------------------------------------------------- |
|---|
| 520 | if (forcing_astex) then |
|---|
| 521 | |
|---|
| [2019] | 522 | print*, & |
|---|
| 523 | & '#### ITAP,day,day1,(day-day1)*86400,(day-day1)*86400/dt_astex=', & |
|---|
| 524 | & day,day1,(day-day1)*86400.,(day-day1)*86400/dt_astex |
|---|
| [2017] | 525 | |
|---|
| 526 | ! time interpolation: |
|---|
| 527 | ! ATTENTION, cet appel ne convient pas pour TOGA !! |
|---|
| 528 | ! revoir 1DUTILS.h et les arguments |
|---|
| [2019] | 529 | CALL interp_astex_time(daytime,day1,annee_ref & |
|---|
| 530 | & ,year_ini_astex,day_ju_ini_astex,nt_astex,dt_astex & |
|---|
| 531 | & ,nlev_astex,div_astex,ts_astex,ug_astex,vg_astex & |
|---|
| 532 | & ,ufa_astex,vfa_astex,div_prof,ts_prof,ug_prof,vg_prof & |
|---|
| 533 | & ,ufa_prof,vfa_prof) |
|---|
| [2017] | 534 | |
|---|
| 535 | if (type_ts_forcing.eq.1) ts_cur = ts_prof ! SST used in read_tsurf1d |
|---|
| 536 | |
|---|
| 537 | ! vertical interpolation: |
|---|
| [2019] | 538 | CALL interp_astex_vertical(play,nlev_astex,plev_profa & |
|---|
| 539 | & ,t_profa,thl_profa,qv_profa,ql_profa,qt_profa & |
|---|
| 540 | & ,u_profa,v_profa,w_profa,tke_profa,o3mmr_profa & |
|---|
| 541 | & ,t_mod,thl_mod,qv_mod,ql_mod,qt_mod,u_mod,v_mod,w_mod & |
|---|
| 542 | & ,tke_mod,o3mmr_mod,mxcalc) |
|---|
| [2017] | 543 | !calcul de l'advection verticale |
|---|
| 544 | !Calcul des gradients verticaux |
|---|
| 545 | !initialisation |
|---|
| 546 | d_t_z(:)=0. |
|---|
| 547 | d_q_z(:)=0. |
|---|
| 548 | d_t_dyn_z(:)=0. |
|---|
| 549 | d_q_dyn_z(:)=0. |
|---|
| 550 | ! schema centre |
|---|
| 551 | ! DO l=2,llm-1 |
|---|
| 552 | ! d_t_z(l)=(temp(l+1)-temp(l-1)) |
|---|
| 553 | ! & /(play(l+1)-play(l-1)) |
|---|
| 554 | ! d_q_z(l)=(q(l+1,1)-q(l-1,1)) |
|---|
| 555 | ! & /(play(l+1)-play(l-1)) |
|---|
| 556 | ! schema amont |
|---|
| 557 | DO l=2,llm-1 |
|---|
| 558 | d_t_z(l)=(temp(l+1)-temp(l))/(play(l+1)-play(l)) |
|---|
| 559 | d_q_z(l)=(q(l+1,1)-q(l,1))/(play(l+1)-play(l)) |
|---|
| 560 | ! print *,'l temp2 temp0 play2 play0 omega_mod', |
|---|
| 561 | ! & temp(l+1),temp(l-1),play(l+1),play(l-1),omega_mod(l) |
|---|
| 562 | ENDDO |
|---|
| 563 | d_t_z(1)=d_t_z(2) |
|---|
| 564 | d_q_z(1)=d_q_z(2) |
|---|
| 565 | d_t_z(llm)=d_t_z(llm-1) |
|---|
| 566 | d_q_z(llm)=d_q_z(llm-1) |
|---|
| 567 | |
|---|
| 568 | ! calcul de l advection verticale |
|---|
| 569 | ! Confusion w (m/s) et omega (Pa/s) !! |
|---|
| 570 | d_t_dyn_z(:)=w_mod(:)*d_t_z(:) |
|---|
| 571 | d_q_dyn_z(:)=w_mod(:)*d_q_z(:) |
|---|
| 572 | ! do l=1,llm |
|---|
| 573 | ! print *,'d_t_dyn omega_mod d_t_z d_q_dyn d_q_z', |
|---|
| 574 | ! :l,d_t_dyn_z(l),omega_mod(l),d_t_z(l),d_q_dyn_z(l),d_q_z(l) |
|---|
| 575 | ! enddo |
|---|
| 576 | |
|---|
| 577 | |
|---|
| 578 | ! large-scale forcing : pour le cas Astex ces forcages sont la SST |
|---|
| 579 | ! la divergence,ug,vg,ufa,vfa |
|---|
| 580 | tsurf = ts_prof |
|---|
| 581 | write(*,*) 'SST suivante: ',tsurf |
|---|
| 582 | do l = 1, llm |
|---|
| 583 | omega(l) = w_mod(l) |
|---|
| 584 | omega2(l)= omega(l)/rg*airefi ! flxmass_w calcule comme ds physiq |
|---|
| 585 | |
|---|
| 586 | alpha = rd*temp(l)*(1.+(rv/rd-1.)*q(l,1))/play(l) |
|---|
| 587 | ! |
|---|
| 588 | ! d_th_adv(l) = 0.0 |
|---|
| 589 | ! d_q_adv(l,1) = 0.0 |
|---|
| 590 | !CR:test advection=0 |
|---|
| 591 | !calcul de l'advection verticale |
|---|
| 592 | d_th_adv(l) = alpha*omega(l)/rcpd-d_t_dyn_z(l) |
|---|
| 593 | ! print*,'temp adv',l,-d_t_dyn_z(l) |
|---|
| 594 | d_q_adv(l,1) = -d_q_dyn_z(l) |
|---|
| 595 | ! print*,'q adv',l,-d_q_dyn_z(l) |
|---|
| 596 | dt_cooling(l) = 0.0 |
|---|
| 597 | enddo |
|---|
| 598 | endif ! forcing_astex |
|---|
| 599 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 600 | |
|---|
