module hbtm_mod

  USE yomcst_mod_h
    IMPLICIT NONE

contains

  SUBROUTINE hbtm(knon, paprs, pplay, t2m, t10m, q2m, q10m, ustar, wstar, &
       flux_t, flux_q, u, v, t, q, pblh, cape, eauliq, ctei, pblt, therm, &
       trmb1, trmb2, trmb3, plcl)
    USE dimphy
    USE yoethf_mod_h

    ! ***************************************************************
    ! *                                                             *
    ! * HBTM2   D'apres Holstag&Boville et Troen&Mahrt              *
    ! *                 JAS 47              BLM                     *
    ! * Algorithme These Anne Mathieu                               *
    ! * Critere d'Entrainement Peter Duynkerke (JAS 50)             *
    ! * written by  : Anne MATHIEU & Alain LAHELLEC, 22/11/99       *
    ! * features : implem. exces Mathieu                            *
    ! ***************************************************************
    ! * mods : decembre 99 passage th a niveau plus bas. voir fixer *
    ! * la prise du th a z/Lambda = -.2 (max Ray)                   *
    ! * Autre algo : entrainement ~ Theta+v =cste mais comment=>The?*
    ! * on peut fixer q a .7qsat(cf non adiab)=>T2 et The2          *
    ! * voir aussi //KE pblh = niveau The_e ou l = env.             *
    ! ***************************************************************
    ! * fin therm a la HBTM passage a forme Mathieu 12/09/2001      *
    ! ***************************************************************
    ! *


    ! AM Fev 2003
    ! Adaptation a LMDZ version couplee

    ! Pour le moment on fait passer en argument les grdeurs de surface :
    ! flux, t,q2m, t,q10m, on va utiliser systematiquement les grdeurs a 2m ms
    ! on garde la possibilite de changer si besoin est (jusqu'a present la
    ! forme de HB avec le 1er niveau modele etait conservee)





    REAL rlvcp, reps
    ! Arguments:

    INTEGER knon ! nombre de points a calculer
    ! AM
    REAL t2m(klon), t10m(klon) ! temperature a 2 et 10m
    REAL q2m(klon), q10m(klon) ! q a 2 et 10m
    REAL ustar(klon)
    REAL wstar(klon) ! w*, convective velocity scale
    REAL paprs(klon, klev+1) ! pression a inter-couche (Pa)
    REAL pplay(klon, klev) ! pression au milieu de couche (Pa)
    REAL flux_t(klon, klev), flux_q(klon, klev) ! Flux
    REAL u(klon, klev) ! vitesse U (m/s)
    REAL v(klon, klev) ! vitesse V (m/s)
    REAL t(klon, klev) ! temperature (K)
    REAL q(klon, klev) ! vapeur d'eau (kg/kg)
    ! AM      REAL cd_h(klon) ! coefficient de friction au sol pour chaleur
    ! AM      REAL cd_m(klon) ! coefficient de friction au sol pour vitesse

    INTEGER isommet
    ! um      PARAMETER (isommet=klev) ! limite max sommet pbl
    REAL, PARAMETER :: vk = 0.35 ! Von Karman => passer a .41 ! cf U.Olgstrom
    REAL, PARAMETER :: ricr = 0.4
    REAL, PARAMETER :: fak = 8.5 ! b calcul du Prandtl et de dTetas
    REAL, PARAMETER :: fakn = 7.2 ! a
    REAL, PARAMETER :: onet = 1.0/3.0
    REAL, PARAMETER :: t_coup = 273.15
    REAL, PARAMETER :: zkmin = 0.01
    REAL, PARAMETER :: betam = 15.0 ! pour Phim / h dans la S.L stable
    REAL, PARAMETER :: betah = 15.0

    REAL, PARAMETER :: betas = 5.0
    ! Phit dans la S.L. stable (mais 2 formes / z/OBL<>1

    REAL, PARAMETER :: sffrac = 0.1 ! S.L. = z/h < .1
    REAL, PARAMETER :: usmin = 1.E-12
    REAL, PARAMETER :: binm = betam*sffrac
    REAL, PARAMETER :: binh = betah*sffrac
    REAL, PARAMETER :: ccon = fak*sffrac*vk
    REAL, PARAMETER :: b1 = 70., b2 = 20.
    REAL, PARAMETER :: zref = 2. ! Niveau de ref a 2m peut eventuellement
    ! etre choisi a 10m
    REAL q_star, t_star
    REAL b212, b2sr ! Lambert correlations T' q' avec T* q*

    REAL z(klon, klev)
    ! AM      REAL pcfm(klon,klev), pcfh(klon,klev)
    INTEGER i, k, j
    REAL zxt
    ! AM      REAL zxt, zxq, zxu, zxv, zxmod, taux, tauy
    ! AM      REAL zx_alf1, zx_alf2 ! parametres pour extrapolation
    REAL khfs(klon) ! surface kinematic heat flux [mK/s]
    REAL kqfs(klon) ! sfc kinematic constituent flux [m/s]
    REAL heatv(klon) ! surface virtual heat flux
    REAL rhino(klon, klev) ! bulk Richardon no. mais en Theta_v
    LOGICAL unstbl(klon) ! pts w/unstbl pbl (positive virtual ht flx)
    LOGICAL stblev(klon) ! stable pbl with levels within pbl
    LOGICAL unslev(klon) ! unstbl pbl with levels within pbl
    LOGICAL unssrf(klon) ! unstb pbl w/lvls within srf pbl lyr
    LOGICAL unsout(klon) ! unstb pbl w/lvls in outer pbl lyr
    LOGICAL check(klon) ! True=>chk if Richardson no.>critcal
    LOGICAL omegafl(klon) ! flag de prolongerment cape pour pt Omega
    REAL pblh(klon)
    REAL pblt(klon)
    REAL plcl(klon)
    ! AM      REAL cgh(klon,2:klev) ! counter-gradient term for heat [K/m]
    ! AM      REAL cgq(klon,2:klev) ! counter-gradient term for constituents
    ! AM      REAL cgs(klon,2:klev) ! counter-gradient star (cg/flux)
    REAL unsobklen(klon) ! Monin-Obukhov lengh
    ! AM      REAL ztvd, ztvu,
    REAL zdu2
    REAL, intent(out):: therm(:) ! (klon) thermal virtual temperature excess
    REAL trmb1(klon), trmb2(klon), trmb3(klon)
    ! Algorithme thermique
    REAL s(klon, klev) ! [P/Po]^Kappa milieux couches
    REAL th_th(klon) ! potential temperature of thermal
    REAL the_th(klon) ! equivalent potential temperature of thermal
    REAL qt_th(klon) ! total water  of thermal
    REAL tbef(klon) ! T thermique niveau precedent
    REAL qsatbef(klon)
    LOGICAL zsat(klon) ! le thermique est sature
    REAL cape(klon) ! Cape du thermique
    REAL kape(klon) ! Cape locale
    REAL eauliq(klon) ! Eau liqu integr du thermique
    REAL ctei(klon) ! Critere d'instab d'entrainmt des nuages de CL
    REAL the1, the2, aa, bb, zthvd, zthvu, xintpos, qqsat
    ! IM 091204 BEG
    REAL a1, a2, a3
    ! IM 091204 END
    REAL xhis, rnum, denom, th1, th2, thv1, thv2, ql2
    REAL dqsat_dt, qsat2, qt1, q2, t1, t2, xnull, delt_the
    REAL delt_qt, delt_2, quadsat, spblh, reduc

    REAL phiminv(klon) ! inverse phi function for momentum
    REAL phihinv(klon) ! inverse phi function for heat
    REAL wm(klon) ! turbulent velocity scale for momentum
    REAL fak1(klon) ! k*ustar*pblh
    REAL fak2(klon) ! k*wm*pblh
    REAL fak3(klon) ! fakn*wstar/wm
    REAL pblk(klon) ! level eddy diffusivity for momentum
    REAL pr(klon) ! Prandtl number for eddy diffusivities
    REAL zl(klon) ! zmzp / Obukhov length
    REAL zh(klon) ! zmzp / pblh
    REAL zzh(klon) ! (1-(zmzp/pblh))**2
    REAL zm(klon) ! current level height
    REAL zp(klon) ! current level height + one level up
    REAL zcor, zdelta, zcvm5
    ! AM      REAL zxqs
    REAL fac, pblmin, zmzp, term

    include "FCTTRE.h"

    ! initialisations (Anne)
    isommet = klev
    th_th(:) = 0.
    q_star = 0
    t_star = 0
    therm = 0.

    b212 = sqrt(b1*b2)
    b2sr = sqrt(b2)

    ! ============================================================
    ! Fonctions thermo implicites
    ! ============================================================
    ! +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! Tetens : pression partielle de vap d'eau e_sat(T)
    ! =================================================
    ! ++ e_sat(T) = r2*exp( r3*(T-Tf)/(T-r4) ) id a r2*FOEWE
    ! ++ avec :
    ! ++ Tf = 273.16 K  (Temp de fusion de la glace)
    ! ++ r2 = 611.14 Pa
    ! ++ r3 = 17.269 (liquide) 21.875 (solide) adim
    ! ++ r4 = 35.86             7.66           Kelvin
    ! ++  q_sat = eps*e_sat/(p-(1-eps)*e_sat)
    ! ++ deriv� :
    ! ++ =========
    ! ++                   r3*(Tf-r4)*q_sat(T,p)
    ! ++ d_qsat_dT = --------------------------------
    ! ++             (T-r4)^2*( 1-(1-eps)*e_sat(T)/p )
    ! ++ pour zcvm5=Lv, c'est FOEDE
    ! ++ Rq :(1.-REPS)*esarg/Parg id a RETV*Qsat
    ! ------------------------------------------------------------------

    ! Initialisation
    rlvcp = rlvtt/rcpd
    reps = rd/rv


    ! DO i = 1, klon
    ! pcfh(i,1) = cd_h(i)
    ! pcfm(i,1) = cd_m(i)
    ! ENDDO
    ! DO k = 2, klev
    ! DO i = 1, klon
    ! pcfh(i,k) = zkmin
    ! pcfm(i,k) = zkmin
    ! cgs(i,k) = 0.0
    ! cgh(i,k) = 0.0
    ! cgq(i,k) = 0.0
    ! ENDDO
    ! ENDDO

    ! Calculer les hauteurs de chaque couche
    ! (geopotentielle Int_dp/ro = Int_[Rd.T.dp/p] z = geop/g)
    ! pourquoi ne pas utiliser Phi/RG ?
    DO i = 1, knon
       z(i, 1) = rd*t(i, 1)/(0.5*(paprs(i,1)+pplay(i,1)))&
            *(paprs(i,1)-pplay(i,1))/rg
       s(i, 1) = (pplay(i,1)/paprs(i,1))**rkappa
    END DO
    ! s(k) = [pplay(k)/ps]^kappa
    ! + + + + + + + + + pplay  <-> s(k)   t  dp=pplay(k-1)-pplay(k)

    ! -----------------  paprs <-> sig(k)

    ! + + + + + + + + + pplay  <-> s(k-1)


    ! + + + + + + + + + pplay  <-> s(1)   t  dp=paprs-pplay   z(1)

    ! -----------------  paprs <-> sig(1)

    DO k = 2, klev
       DO i = 1, knon
          z(i, k) = z(i, k-1) + rd*0.5*(t(i,k-1)+t(i,k))/paprs(i, k)&
               *(pplay(i,k-1)-pplay(i,k))/rg
          s(i, k) = (pplay(i,k)/paprs(i,1))**rkappa
       END DO
    END DO
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! +++  Determination des grandeurs de surface  +++++++++++++++++++++
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    DO i = 1, knon
       ! AM         IF (thermcep) THEN
       ! AM           zdelta=MAX(0.,SIGN(1.,RTT-tsol(i)))
       ! zcvm5 = R5LES*RLVTT*(1.-zdelta) + R5IES*RLSTT*zdelta
       ! zcvm5 = zcvm5 / RCPD / (1.0+RVTMP2*q(i,1))
       ! AM           zxqs= r2es * FOEEW(tsol(i),zdelta)/paprs(i,1)
       ! AM           zxqs=MIN(0.5,zxqs)
       ! AM           zcor=1./(1.-retv*zxqs)
       ! AM           zxqs=zxqs*zcor
       ! AM         ELSE
       ! AM           IF (tsol(i).LT.t_coup) THEN
       ! AM              zxqs = qsats(tsol(i)) / paprs(i,1)
       ! AM           ELSE
       ! AM              zxqs = qsatl(tsol(i)) / paprs(i,1)
       ! AM           ENDIF
       ! AM         ENDIF
       ! niveau de reference bulk; mais ici, c,a pourrait etre le niveau de ref
       ! du thermique
       ! AM        zx_alf1 = 1.0
       ! AM        zx_alf2 = 1.0 - zx_alf1
       ! AM        zxt = (t(i,1)+z(i,1)*RG/RCPD/(1.+RVTMP2*q(i,1)))
       ! AM     .        *(1.+RETV*q(i,1))*zx_alf1
       ! AM     .      + (t(i,2)+z(i,2)*RG/RCPD/(1.+RVTMP2*q(i,2)))
       ! AM     .        *(1.+RETV*q(i,2))*zx_alf2
       ! AM        zxu = u(i,1)*zx_alf1+u(i,2)*zx_alf2
       ! AM        zxv = v(i,1)*zx_alf1+v(i,2)*zx_alf2
       ! AM        zxq = q(i,1)*zx_alf1+q(i,2)*zx_alf2
       ! AM
       ! AMAM           zxu = u10m(i)
       ! AMAM           zxv = v10m(i)
       ! AMAM           zxmod = 1.0+SQRT(zxu**2+zxv**2)
       ! AM Niveau de ref choisi a 2m
       zxt = t2m(i)

       ! ***************************************************
       ! attention, il doit s'agir de <w'theta'>
       ! ;Calcul de tcls virtuel et de w'theta'virtuel
       ! ;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;
       ! tcls=tcls*(1+.608*qcls)

       ! ;Pour avoir w'theta',
       ! ; il faut diviser par ro.Cp
       ! Cp=Cpd*(1+0.84*qcls)
       ! fcs=fcs/(ro_surf*Cp)
       ! ;On transforme w'theta' en w'thetav'
       ! Lv=(2.501-0.00237*(tcls-273.15))*1.E6
       ! xle=xle/(ro_surf*Lv)
       ! fcsv=fcs+.608*xle*tcls
       ! ***************************************************
       ! AM        khfs(i) = (tsol(i)*(1.+RETV*q(i,1))-zxt) *zxmod*cd_h(i)
       ! AM        kqfs(i) = (zxqs-zxq) *zxmod*cd_h(i) * beta(i)
       ! AM
       ! dif khfs est deja w't'_v / heatv(i) = khfs(i) + RETV*zxt*kqfs(i)
       ! AM calcule de Ro = paprs(i,1)/Rd zxt
       ! AM convention >0 vers le bas ds lmdz
       khfs(i) = -flux_t(i, 1)*zxt*rd/(rcpd*paprs(i,1))
       kqfs(i) = -flux_q(i, 1)*zxt*rd/(paprs(i,1))
       ! AM   verifier que khfs et kqfs sont bien de la forme w'l'
       heatv(i) = khfs(i) + 0.608*zxt*kqfs(i)
       ! a comparer aussi aux sorties de clqh : flux_T/RoCp et flux_q/RoLv
       ! AM        heatv(i) = khfs(i)
       ! AM ustar est en entree
       ! AM        taux = zxu *zxmod*cd_m(i)
       ! AM        tauy = zxv *zxmod*cd_m(i)
       ! AM        ustar(i) = SQRT(taux**2+tauy**2)
       ! AM        ustar(i) = MAX(SQRT(ustar(i)),0.01)
       ! Theta et qT du thermique sans exces (interpolin vers surf)
       ! chgt de niveau du thermique (jeudi 30/12/1999)
       ! (interpolation lineaire avant integration phi_h)
       ! AM        qT_th(i) = zxqs*beta(i) + 4./z(i,1)*(q(i,1)-zxqs*beta(i))
       ! AM        qT_th(i) = max(qT_th(i),q(i,1))
       qt_th(i) = q2m(i)
       ! n The_th restera la Theta du thermique sans exces jusqu'a 2eme calcul
       ! n reste a regler convention P) pour Theta
       ! The_th(i) = tsol(i) + 4./z(i,1)*(t(i,1)-tsol(i))
       ! -                      + RLvCp*qT_th(i)
       ! AM        Th_th(i) = tsol(i) + 4./z(i,1)*(t(i,1)-tsol(i))
       th_th(i) = t2m(i)
    END DO

    DO i = 1, knon
       rhino(i, 1) = 0.0 ! Global Richardson
       check(i) = .TRUE.
       pblh(i) = z(i, 1) ! on initialise pblh a l'altitude du 1er niveau
       plcl(i) = 6000.
       ! Lambda = -u*^3 / (alpha.g.kvon.<w'Theta'v>
       unsobklen(i) = -rg*vk*heatv(i)/(t(i,1)*max(ustar(i),usmin)**3)
       trmb1(i) = 0.
       trmb2(i) = 0.
       trmb3(i) = 0.
    END DO


    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! PBL height calculation:
    ! Search for level of pbl. Scan upward until the Richardson number between
    ! the first level and the current level exceeds the "critical" value.
    ! (bonne idee Nu de separer le Ric et l'exces de temp du thermique)
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    fac = 100.0
    DO k = 2, isommet
       DO i = 1, knon
          IF (check(i)) THEN
             ! pourquoi / niveau 1 (au lieu du sol) et le terme en u*^2 ?
             ! test     zdu2 =
             ! (u(i,k)-u(i,1))**2+(v(i,k)-v(i,1))**2+fac*ustar(i)**2
             zdu2 = u(i, k)**2 + v(i, k)**2
             zdu2 = max(zdu2, 1.0E-20)
             ! Theta_v environnement
             zthvd = t(i, k)/s(i, k)*(1.+retv*q(i,k))

             ! therm Theta_v sans exces (avec hypothese fausse de H&B, sinon,
             ! passer par Theta_e et virpot)
             ! zthvu=t(i,1)/s(i,1)*(1.+RETV*q(i,1))
             ! AM         zthvu = Th_th(i)*(1.+RETV*q(i,1))
             zthvu = th_th(i)*(1.+retv*qt_th(i))
             ! Le Ri par Theta_v
             ! AM         rhino(i,k) = (z(i,k)-z(i,1))*RG*(zthvd-zthvu)
             ! AM     .               /(zdu2*0.5*(zthvd+zthvu))
             ! AM On a nveau de ref a 2m ???
             rhino(i, k) = (z(i,k)-zref)*rg*(zthvd-zthvu)/(zdu2*0.5&
                  *(zthvd+zthvu))

             IF (rhino(i,k)>=ricr) THEN
                pblh(i) = z(i, k-1) + (z(i,k-1)-z(i,k))*(ricr-rhino(i,k-1))&
                     /(rhino(i,k-1)-rhino(i,k))
                ! test04
                pblh(i) = pblh(i) + 100.
                pblt(i) = t(i, k-1) + (t(i,k)-t(i,k-1))*(pblh(i)-z(i,k-1))&
                     /(z(i,k)- z(i,k-1))
                check(i) = .FALSE.
             END IF
          END IF
       END DO
    END DO


    ! Set pbl height to maximum value where computation exceeds number of
    ! layers allowed

    DO i = 1, knon
       IF (check(i)) pblh(i) = z(i, isommet)
    END DO

    ! Improve estimate of pbl height for the unstable points.
    ! Find unstable points (sensible heat flux is upward):

    DO i = 1, knon
       IF (heatv(i)>0.) THEN
          unstbl(i) = .TRUE.
          check(i) = .TRUE.
       ELSE
          unstbl(i) = .FALSE.
          check(i) = .FALSE.
       END IF
    END DO

    ! For the unstable case, compute velocity scale and the
    ! convective temperature excess:

    DO i = 1, knon
       IF (check(i)) THEN
          phiminv(i) = (1.-binm*pblh(i)*unsobklen(i))**onet
          ! ***************************************************
          ! Wm ? et W* ? c'est la formule pour z/h < .1
          ! ;Calcul de w* ;;
          ! ;;;;;;;;;;;;;;;;
          ! w_star=((g/tcls)*fcsv*z(ind))^(1/3.) [ou prendre la premiere approx
          ! de h)
          ! ;; CALCUL DE wm ;;
          ! ;;;;;;;;;;;;;;;;;;
          ! ; Ici on considerera que l'on est dans la couche de surf jusqu'a
          ! 100 m
          ! ; On prend svt couche de surface=0.1*h mais on ne connait pas h
          ! ;;;;;;;;;;;Dans la couche de surface
          ! if (z(ind) le 20) then begin
          ! Phim=(1.-15.*(z(ind)/L))^(-1/3.)
          ! wm=u_star/Phim
          ! ;;;;;;;;;;;En dehors de la couche de surface
          ! endif else if (z(ind) gt 20) then begin
          ! wm=(u_star^3+c1*w_star^3)^(1/3.)
          ! endif
          ! ***************************************************
          wm(i) = ustar(i)*phiminv(i)
          ! ===================================================================
          ! valeurs de Dominique Lambert de la campagne SEMAPHORE :
          ! <T'^2> = 100.T*^2; <q'^2> = 20.q*^2 a 10m
          ! <Tv'^2> = (1+1.2q).100.T* + 1.2Tv.sqrt(20*100).T*.q* +
          ! (.608*Tv)^2*20.q*^2;
          ! et dTetavS = sqrt(<Tv'^2>) ainsi calculee.
          ! avec : T*=<w'T'>_s/w* et q*=<w'q'>/w*
          ! !!! on peut donc utiliser w* pour les fluctuations <-> Lambert
          ! (leur corellation pourrait dependre de beta par ex)
          ! if fcsv(i,j) gt 0 then begin
          ! dTetavs=b1*(1.+2.*.608*q_10(i,j))*(fcs(i,j)/wm(i,j))^2+$
          ! (.608*Thetav_10(i,j))^2*b2*(xle(i,j)/wm(i,j))^2+$
          ! 2.*.608*thetav_10(i,j)*sqrt(b1*b2)*(xle(i,j)/wm(i,j))*(fcs(i,j)
          ! /wm(i,j))
          ! dqs=b2*(xle(i,j)/wm(i,j))^2
          ! theta_s(i,j)=thetav_10(i,j)+sqrt(dTetavs)
          ! q_s(i,j)=q_10(i,j)+sqrt(dqs)
          ! endif else begin
          ! Theta_s(i,j)=thetav_10(i,j)
          ! q_s(i,j)=q_10(i,j)
          ! endelse
          ! ===================================================================

          ! HBTM        therm(i) = heatv(i)*fak/wm(i)
          ! forme Mathieu :
          q_star = kqfs(i)/wm(i)
          t_star = khfs(i)/wm(i)
          ! IM 091204 BEG
          IF (1==0) THEN
             IF (t_star<0. .OR. q_star<0.) THEN
                PRINT *, 'i t_star q_star khfs kqfs wm', i, t_star, q_star, &
                     khfs(i), kqfs(i), wm(i)
             END IF
          END IF
          ! IM 091204 END
          ! AM Nveau cde ref 2m =>
          ! AM        therm(i) = sqrt( b1*(1.+2.*RETV*q(i,1))*t_star**2
          ! AM     +             + (RETV*T(i,1))**2*b2*q_star**2
          ! AM     +             + 2.*RETV*T(i,1)*b212*q_star*t_star
          ! AM     +                 )
          ! IM 091204 BEG
          a1 = b1*(1.+2.*retv*qt_th(i))*t_star**2
          a2 = (retv*th_th(i))**2*b2*q_star*q_star
          a3 = 2.*retv*th_th(i)*b212*q_star*t_star
          aa = a1 + a2 + a3
          IF (1==0) THEN
             IF (aa<0.) THEN
                PRINT *, 'i a1 a2 a3 aa', i, a1, a2, a3, aa
                PRINT *, 'i qT_th Th_th t_star q_star RETV b1 b2 b212', i, &
                     qt_th(i), th_th(i), t_star, q_star, retv, b1, b2, b212
             END IF
          END IF
          ! IM 091204 END
          therm(i) = sqrt(b1*(1.+2.*retv*qt_th(i))*t_star**2+(retv*th_th( &
               i))**2*b2*q_star*q_star &  ! IM 101204  +             +
                                ! 2.*RETV*Th_th(i)*b212*q_star*t_star
               +max(0.,2.*retv*th_th(i)*b212*q_star*t_star))

          ! Theta et qT du thermique (forme H&B) avec exces
          ! (attention, on ajoute therm(i) qui est virtuelle ...)
          ! pourquoi pas sqrt(b1)*t_star ?
          ! dqs = b2sr*kqfs(i)/wm(i)
          qt_th(i) = qt_th(i) + b2sr*q_star
          ! new on differre le calcul de Theta_e
          ! The_th(i) = The_th(i) + therm(i) + RLvCp*qT_th(i)
          ! ou:    The_th(i) = The_th(i) + sqrt(b1)*khfs(i)/wm(i) +
          ! RLvCp*qT_th(i)
          rhino(i, 1) = 0.0
       END IF
    END DO

    ! +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! ++ Improve pblh estimate for unstable conditions using the +++++++
    ! ++          convective temperature excess :                +++++++
    ! ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
    ! +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++

    DO k = 2, isommet
       DO i = 1, knon
          IF (check(i)) THEN
             ! test     zdu2 =
             ! (u(i,k)-u(i,1))**2+(v(i,k)-v(i,1))**2+fac*ustar(i)**2
             zdu2 = u(i, k)**2 + v(i, k)**2
             zdu2 = max(zdu2, 1.0E-20)
             ! Theta_v environnement
             zthvd = t(i, k)/s(i, k)*(1.+retv*q(i,k))

             ! et therm Theta_v (avec hypothese de constance de H&B,
             ! zthvu=(t(i,1)+therm(i))/s(i,1)*(1.+RETV*q(i,1))
             zthvu = th_th(i)*(1.+retv*qt_th(i)) + therm(i)


             ! Le Ri par Theta_v
             ! AM Niveau de ref 2m
             ! AM         rhino(i,k) = (z(i,k)-z(i,1))*RG*(zthvd-zthvu)
             ! AM     .               /(zdu2*0.5*(zthvd+zthvu))
             rhino(i, k) = (z(i,k)-zref)*rg*(zthvd-zthvu)/(zdu2*0.5&
                  *(zthvd+zthvu))


             IF (rhino(i,k)>=ricr) THEN
                pblh(i) = z(i, k-1) + (z(i,k-1)-z(i,k))*(ricr-rhino(i,k-1))&
                     /(rhino(i,k-1)-rhino(i,k))
                ! test04
                pblh(i) = pblh(i) + 100.
                pblt(i) = t(i, k-1) + (t(i,k)-t(i,k-1))*(pblh(i)-z(i,k-1))&
                     /(z(i,k)- z(i,k-1))
                check(i) = .FALSE.
                ! IM 170305 BEG
                IF (1==0) THEN
                   ! debug print -120;34       -34-        58 et    0;26 wamp
                   IF (i==950 .OR. i==192 .OR. i==624 .OR. i==118) THEN
                      PRINT *, ' i,Th_th,Therm,qT :', i, th_th(i), therm(i), &
                           qt_th(i)
                      q_star = kqfs(i)/wm(i)
                      t_star = khfs(i)/wm(i)
                      PRINT *, 'q* t*, b1,b2,b212 ', q_star, t_star, &
                           b1*(1.+2.*retv*qt_th(i))*t_star**2, &
                           (retv*th_th(i))**2*b2*q_star**2, 2.*retv*th_th(i)&
                           *b212*q_star *t_star
                      PRINT *, 'zdu2 ,100.*ustar(i)**2', zdu2, fac*ustar(i)**2
                   END IF
                END IF !(1.EQ.0) THEN
                ! IM 170305 END
                ! q_star = kqfs(i)/wm(i)
                ! t_star = khfs(i)/wm(i)
                ! trmb1(i) = b1*(1.+2.*RETV*q(i,1))*t_star**2
                ! trmb2(i) = (RETV*T(i,1))**2*b2*q_star**2
                ! Omega now   trmb3(i) = 2.*RETV*T(i,1)*b212*q_star*t_star
             END IF
          END IF
       END DO
    END DO

    ! Set pbl height to maximum value where computation exceeds number of
    ! layers allowed

    DO i = 1, knon
       IF (check(i)) pblh(i) = z(i, isommet)
    END DO

    ! PBL height must be greater than some minimum mechanical mixing depth
    ! Several investigators have proposed minimum mechanical mixing depth
    ! relationships as a function of the local friction velocity, u*.  We
    ! make use of a linear relationship of the form h = c u* where c=700.
    ! The scaling arguments that give rise to this relationship most often
    ! represent the coefficient c as some constant over the local coriolis
    ! parameter.  Here we make use of the experimental results of Koracin
    ! and Berkowicz (1988) [BLM, Vol 43] for wich they recommend 0.07/f
    ! where f was evaluated at 39.5 N and 52 N.  Thus we use a typical mid
    ! latitude value for f so that c = 0.07/f = 700.

    DO i = 1, knon
       pblmin = 700.0*ustar(i)
       pblh(i) = max(pblh(i), pblmin)
       ! par exemple :
       pblt(i) = t(i, 2) + (t(i,3)-t(i,2))*(pblh(i)-z(i,2))/(z(i,3)-z(i,2))
    END DO

    ! ********************************************************************
    ! pblh is now available; do preparation for diffusivity calculation :
    ! ********************************************************************
    DO i = 1, knon
       check(i) = .TRUE.
       zsat(i) = .FALSE.
       ! omegafl utilise pour prolongement CAPE
       omegafl(i) = .FALSE.
       cape(i) = 0.
       kape(i) = 0.
       eauliq(i) = 0.
       ctei(i) = 0.
       pblk(i) = 0.0
       fak1(i) = ustar(i)*pblh(i)*vk

       ! Do additional preparation for unstable cases only, set temperature
       ! and moisture perturbations depending on stability.
       ! *** Rq: les formule sont prises dans leur forme CS ***
       IF (unstbl(i)) THEN
          ! AM Niveau de ref du thermique
          ! AM          zxt=(t(i,1)-z(i,1)*0.5*RG/RCPD/(1.+RVTMP2*q(i,1)))
          ! AM     .         *(1.+RETV*q(i,1))
          zxt = (th_th(i)-zref*0.5*rg/rcpd/(1.+rvtmp2*qt_th(i)))* &
               (1.+retv*qt_th(i))
          phiminv(i) = (1.-binm*pblh(i)*unsobklen(i))**onet
          phihinv(i) = sqrt(1.-binh*pblh(i)*unsobklen(i))
          wm(i) = ustar(i)*phiminv(i)
          fak2(i) = wm(i)*pblh(i)*vk
          wstar(i) = (heatv(i)*rg*pblh(i)/zxt)**onet
          fak3(i) = fakn*wstar(i)/wm(i)
       ELSE
          wstar(i) = 0.
       END IF
       ! Computes Theta_e for thermal (all cases : to be modified)
       ! attention ajout therm(i) = virtuelle
       the_th(i) = th_th(i) + therm(i) + rlvcp*qt_th(i)
       ! ou:    The_th(i) = Th_th(i) + sqrt(b1)*khfs(i)/wm(i) + RLvCp*qT_th(i)
    END DO

    ! Main level loop to compute the diffusivities and
    ! counter-gradient terms:

    DO k = 2, isommet

       ! Find levels within boundary layer:

       DO i = 1, knon
          unslev(i) = .FALSE.
          stblev(i) = .FALSE.
          zm(i) = z(i, k-1)
          zp(i) = z(i, k)
          IF (zkmin==0.0 .AND. zp(i)>pblh(i)) zp(i) = pblh(i)
          IF (zm(i)<pblh(i)) THEN
             zmzp = 0.5*(zm(i)+zp(i))
             ! debug
             ! if (i.EQ.1864) then
             ! print*,'i,pblh(1864),obklen(1864)',i,pblh(i),obklen(i)
             ! endif

             zh(i) = zmzp/pblh(i)
             zl(i) = zmzp*unsobklen(i)
             zzh(i) = 0.
             IF (zh(i)<=1.0) zzh(i) = (1.-zh(i))**2

             ! stblev for points zm < plbh and stable and neutral
             ! unslev for points zm < plbh and unstable

             IF (unstbl(i)) THEN
                unslev(i) = .TRUE.
             ELSE
                stblev(i) = .TRUE.
             END IF
          END IF
       END DO
       ! print*,'fin calcul niveaux'

       ! Stable and neutral points; set diffusivities; counter-gradient
       ! terms zero for stable case:

       DO i = 1, knon
          IF (stblev(i)) THEN
             IF (zl(i)<=1.) THEN
                pblk(i) = fak1(i)*zh(i)*zzh(i)/(1.+betas*zl(i))
             ELSE
                pblk(i) = fak1(i)*zh(i)*zzh(i)/(betas+zl(i))
             END IF
             ! pcfm(i,k) = pblk(i)
             ! pcfh(i,k) = pcfm(i,k)
          END IF
       END DO

       ! unssrf, unstable within surface layer of pbl
       ! unsout, unstable within outer   layer of pbl

       DO i = 1, knon
          unssrf(i) = .FALSE.
          unsout(i) = .FALSE.
          IF (unslev(i)) THEN
             IF (zh(i)<sffrac) THEN
                unssrf(i) = .TRUE.
             ELSE
                unsout(i) = .TRUE.
             END IF
          END IF
       END DO

       ! Unstable for surface layer; counter-gradient terms zero

       DO i = 1, knon
          IF (unssrf(i)) THEN
             term = (1.-betam*zl(i))**onet
             pblk(i) = fak1(i)*zh(i)*zzh(i)*term
             pr(i) = term/sqrt(1.-betah*zl(i))
          END IF
       END DO
       ! print*,'fin counter-gradient terms zero'

       ! Unstable for outer layer; counter-gradient terms non-zero:

       DO i = 1, knon
          IF (unsout(i)) THEN
             pblk(i) = fak2(i)*zh(i)*zzh(i)
             ! cgs(i,k) = fak3(i)/(pblh(i)*wm(i))
             ! cgh(i,k) = khfs(i)*cgs(i,k)
             pr(i) = phiminv(i)/phihinv(i) + ccon*fak3(i)/fak
             ! cgq(i,k) = kqfs(i)*cgs(i,k)
          END IF
       END DO
       ! print*,'fin counter-gradient terms non zero'

       ! For all unstable layers, compute diffusivities and ctrgrad ter m

       ! DO i = 1, knon
       ! IF (unslev(i)) THEN
       ! pcfm(i,k) = pblk(i)
       ! pcfh(i,k) = pblk(i)/pr(i)
       ! etc cf original
       ! ENDIF
       ! ENDDO

       ! For all layers, compute integral info and CTEI

       DO i = 1, knon
          IF (check(i) .OR. omegafl(i)) THEN
             IF (.NOT. zsat(i)) THEN
                ! Th2 = The_th(i) - RLvCp*qT_th(i)
                th2 = th_th(i)
                t2 = th2*s(i, k)
                ! thermodyn functions
                zdelta = max(0., sign(1.,rtt-t2))
                qqsat = r2es*foeew(t2, zdelta)/pplay(i, k)
                qqsat = min(0.5, qqsat)
                zcor = 1./(1.-retv*qqsat)
                qqsat = qqsat*zcor

                IF (qqsat<qt_th(i)) THEN
                   ! on calcule lcl
                   IF (k==2) THEN
                      plcl(i) = z(i, k)
                   ELSE
                      plcl(i) = z(i, k-1) + (z(i,k-1)-z(i,k))*(qt_th(i)&
                           -qsatbef(i))/(qsatbef(i)-qqsat)
                   END IF
                   zsat(i) = .TRUE.
                   tbef(i) = t2
                END IF

                qsatbef(i) = qqsat ! bug dans la version orig ???
             END IF
             ! amn ???? cette ligne a deja ete faite normalement ?
          END IF
          ! print*,'hbtm2 i,k=',i,k
       END DO
    END DO ! end of level loop
    ! IM 170305 BEG
    IF (1==0) THEN
       PRINT *, 'hbtm2  ok'
    END IF !(1.EQ.0) THEN
    ! IM 170305 END

  END SUBROUTINE hbtm

end module hbtm_mod
