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zdftke.F90

Last change on this file was 15071, checked in by clem, 3 years ago
make tke and gls work with tiling in debug mode. But it needs to be checked over
Property svn:keywords set to `Id`
File size: 50.2 KB

Rev	Line
[1531]	1	MODULE zdftke
[1239]	2	!!======================================================================
[1531]	3	!! * MODULE zdftke *
[14072]	4	!! Ocean physics: vertical mixing coefficient computed from the tke
[1239]	5	!! turbulent closure parameterization
	6	!!=====================================================================
[1492]	7	!! History : OPA ! 1991-03 (b. blanke) Original code
	8	!! 7.0 ! 1991-11 (G. Madec) bug fix
	9	!! 7.1 ! 1992-10 (G. Madec) new mixing length and eav
	10	!! 7.2 ! 1993-03 (M. Guyon) symetrical conditions
	11	!! 7.3 ! 1994-08 (G. Madec, M. Imbard) nn_pdl flag
	12	!! 7.5 ! 1996-01 (G. Madec) s-coordinates
	13	!! 8.0 ! 1997-07 (G. Madec) lbc
	14	!! 8.1 ! 1999-01 (E. Stretta) new option for the mixing length
	15	!! NEMO 1.0 ! 2002-06 (G. Madec) add tke_init routine
	16	!! - ! 2004-10 (C. Ethe ) 1D configuration
	17	!! 2.0 ! 2006-07 (S. Masson) distributed restart using iom
	18	!! 3.0 ! 2008-05 (C. Ethe, G.Madec) : update TKE physics:
	19	!! ! - tke penetration (wind steering)
	20	!! ! - suface condition for tke & mixing length
	21	!! ! - Langmuir cells
	22	!! - ! 2008-05 (J.-M. Molines, G. Madec) 2D form of avtb
	23	!! - ! 2008-06 (G. Madec) style + DOCTOR name for namelist parameters
[14072]	24	!! - ! 2008-12 (G. Reffray) stable discretization of the production term
	25	!! 3.2 ! 2009-06 (G. Madec, S. Masson) TKE restart compatible with key_cpl
[1492]	26	!! ! + cleaning of the parameters + bugs correction
[2528]	27	!! 3.3 ! 2010-10 (C. Ethe, G. Madec) reorganisation of initialisation phase
[5120]	28	!! 3.6 ! 2014-11 (P. Mathiot) add ice shelf capability
[14072]	29	!! 4.0 ! 2017-04 (G. Madec) remove CPP ddm key & avm at t-point only
[13461]	30	!! - ! 2017-05 (G. Madec) add top/bottom friction as boundary condition
[14007]	31	!! 4.2 ! 2020-12 (G. Madec, E. Clementi) add wave coupling
	32	! ! following Couvelard et al., 2019
[1239]	33	!!----------------------------------------------------------------------
[9019]	34
[1239]	35	!!----------------------------------------------------------------------
[3625]	36	!! zdf_tke : update momentum and tracer Kz from a tke scheme
	37	!! tke_tke : tke time stepping: update tke at now time step (en)
	38	!! tke_avn : compute mixing length scale and deduce avm and avt
	39	!! zdf_tke_init : initialization, namelist read, and parameters control
	40	!! tke_rst : read/write tke restart in ocean restart file
[1239]	41	!!----------------------------------------------------------------------
[2528]	42	USE oce ! ocean: dynamics and active tracers variables
	43	USE phycst ! physical constants
	44	USE dom_oce ! domain: ocean
	45	USE domvvl ! domain: variable volume layer
[1492]	46	USE sbc_oce ! surface boundary condition: ocean
[9019]	47	USE zdfdrg ! vertical physics: top/bottom drag coef.
[2528]	48	USE zdfmxl ! vertical physics: mixed layer
[13007]	49	#if defined key_si3
	50	USE ice, ONLY: hm_i, h_i
	51	#endif
	52	#if defined key_cice
	53	USE sbc_ice, ONLY: h_i
	54	#endif
[9019]	55	!
[1492]	56	USE in_out_manager ! I/O manager
	57	USE iom ! I/O manager library
[2715]	58	USE lib_mpp ! MPP library
[9019]	59	USE lbclnk ! ocean lateral boundary conditions (or mpp link)
	60	USE prtctl ! Print control
[14072]	61	USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined)
[14007]	62	USE sbcwave ! Surface boundary waves
[1239]	63
	64	IMPLICIT NONE
	65	PRIVATE
	66
[2528]	67	PUBLIC zdf_tke ! routine called in step module
	68	PUBLIC zdf_tke_init ! routine called in opa module
	69	PUBLIC tke_rst ! routine called in step module
[1239]	70
[4147]	71	! !! Namelist namzdf_tke
	72	LOGICAL :: ln_mxl0 ! mixing length scale surface value as function of wind stress or not
[14007]	73	LOGICAL :: ln_mxhsw ! mixing length scale surface value as a fonction of wave height
[13472]	74	INTEGER :: nn_mxlice ! type of scaling under sea-ice (=0/1/2/3)
	75	REAL(wp) :: rn_mxlice ! ice thickness value when scaling under sea-ice
[4147]	76	INTEGER :: nn_mxl ! type of mixing length (=0/1/2/3)
	77	REAL(wp) :: rn_mxl0 ! surface min value of mixing length (kappaz_o=0.40.1 m) [m]
	78	INTEGER :: nn_pdl ! Prandtl number or not (ratio avt/avm) (=0/1)
	79	REAL(wp) :: rn_ediff ! coefficient for avt: avt=rn_ediffmxlsqrt(e)
[14072]	80	REAL(wp) :: rn_ediss ! coefficient of the Kolmogoroff dissipation
[4147]	81	REAL(wp) :: rn_ebb ! coefficient of the surface input of tke
	82	REAL(wp) :: rn_emin ! minimum value of tke [m2/s2]
	83	REAL(wp) :: rn_emin0 ! surface minimum value of tke [m2/s2]
	84	REAL(wp) :: rn_bshear ! background shear (>0) currently a numerical threshold (do not change it)
	85	INTEGER :: nn_etau ! type of depth penetration of surface tke (=0/1/2/3)
[9019]	86	INTEGER :: nn_htau ! type of tke profile of penetration (=0/1)
[14007]	87	INTEGER :: nn_bc_surf! surface condition (0/1=Dir/Neum) ! Only applicable for wave coupling
	88	INTEGER :: nn_bc_bot ! surface condition (0/1=Dir/Neum) ! Only applicable for wave coupling
[9019]	89	REAL(wp) :: rn_efr ! fraction of TKE surface value which penetrates in the ocean
[4147]	90	LOGICAL :: ln_lc ! Langmuir cells (LC) as a source term of TKE or not
[9019]	91	REAL(wp) :: rn_lc ! coef to compute vertical velocity of Langmuir cells
[14072]	92	INTEGER :: nn_eice ! attenutaion of langmuir & surface wave breaking under ice (=0/1/2/3)
[1239]	93
[4147]	94	REAL(wp) :: ri_cri ! critic Richardson number (deduced from rn_ediff and rn_ediss values)
	95	REAL(wp) :: rmxl_min ! minimum mixing length value (deduced from rn_ediff and rn_emin values) [m]
[2528]	96	REAL(wp) :: rhftau_add = 1.e-3_wp ! add offset applied to HF part of taum (nn_etau=3)
	97	REAL(wp) :: rhftau_scl = 1.0_wp ! scale factor applied to HF part of taum (nn_etau=3)
[1239]	98
[9019]	99	REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:) :: htau ! depth of tke penetration (nn_htau)
	100	REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:,:) :: dissl ! now mixing lenght of dissipation
	101	REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:,:) :: apdlr ! now mixing lenght of dissipation
[1492]	102
[1239]	103	!! * Substitutions
[12377]	104	# include "do_loop_substitute.h90"
[13237]	105	# include "domzgr_substitute.h90"
[1239]	106	!!----------------------------------------------------------------------
[9598]	107	!! NEMO/OCE 4.0 , NEMO Consortium (2018)
[2528]	108	!! $Id$
[10068]	109	!! Software governed by the CeCILL license (see ./LICENSE)
[1239]	110	!!----------------------------------------------------------------------
	111	CONTAINS
	112
[2715]	113	INTEGER FUNCTION zdf_tke_alloc()
	114	!!----------------------------------------------------------------------
	115	!! * FUNCTION zdf_tke_alloc *
	116	!!----------------------------------------------------------------------
[9019]	117	ALLOCATE( htau(jpi,jpj) , dissl(jpi,jpj,jpk) , apdlr(jpi,jpj,jpk) , STAT= zdf_tke_alloc )
	118	!
[10425]	119	CALL mpp_sum ( 'zdftke', zdf_tke_alloc )
	120	IF( zdf_tke_alloc /= 0 ) CALL ctl_stop( 'STOP', 'zdf_tke_alloc: failed to allocate arrays' )
[2715]	121	!
	122	END FUNCTION zdf_tke_alloc
	123
	124
[12377]	125	SUBROUTINE zdf_tke( kt, Kbb, Kmm, p_sh2, p_avm, p_avt )
[1239]	126	!!----------------------------------------------------------------------
[1531]	127	!! * ROUTINE zdf_tke *
[1239]	128	!!
	129	!! ** Purpose : Compute the vertical eddy viscosity and diffusivity
[1492]	130	!! coefficients using a turbulent closure scheme (TKE).
[1239]	131	!!
[1492]	132	!! ** Method : The time evolution of the turbulent kinetic energy (tke)
	133	!! is computed from a prognostic equation :
	134	!! d(en)/dt = avm (d(u)/dz)**2 ! shear production
	135	!! + d( avm d(en)/dz )/dz ! diffusion of tke
	136	!! + avt N^2 ! stratif. destruc.
	137	!! - rn_ediss / emxl en**(2/3) ! Kolmogoroff dissipation
[1239]	138	!! with the boundary conditions:
[1695]	139	!! surface: en = max( rn_emin0, rn_ebb * taum )
[1239]	140	!! bottom : en = rn_emin
[14072]	141	!! The associated critical Richardson number is: ri_cri = 2/(2+rn_ediss/rn_ediff)
[1492]	142	!!
[14072]	143	!! The now Turbulent kinetic energy is computed using the following
[1492]	144	!! time stepping: implicit for vertical diffusion term, linearized semi
[14072]	145	!! implicit for kolmogoroff dissipation term, and explicit forward for
	146	!! both buoyancy and shear production terms. Therefore a tridiagonal
[1492]	147	!! linear system is solved. Note that buoyancy and shear terms are
	148	!! discretized in a energy conserving form (Bruchard 2002).
	149	!!
	150	!! The dissipative and mixing length scale are computed from en and
	151	!! the stratification (see tke_avn)
	152	!!
	153	!! The now vertical eddy vicosity and diffusivity coefficients are
[14072]	154	!! given by:
[1492]	155	!! avm = max( avtb, rn_ediff * zmxlm * en^1/2 )
[14072]	156	!! avt = max( avmb, pdl * avm )
[1239]	157	!! eav = max( avmb, avm )
[1492]	158	!! where pdl, the inverse of the Prandtl number is 1 if nn_pdl=0 and
[14072]	159	!! given by an empirical funtion of the localRichardson number if nn_pdl=1
[1239]	160	!!
	161	!! ** Action : compute en (now turbulent kinetic energy)
[9019]	162	!! update avt, avm (before vertical eddy coef.)
[1239]	163	!!
	164	!! References : Gaspar et al., JGR, 1990,
	165	!! Blanke and Delecluse, JPO, 1991
	166	!! Mellor and Blumberg, JPO 2004
	167	!! Axell, JGR, 2002
[1492]	168	!! Bruchard OM 2002
[1239]	169	!!----------------------------------------------------------------------
[14834]	170	INTEGER , INTENT(in ) :: kt ! ocean time step
	171	INTEGER , INTENT(in ) :: Kbb, Kmm ! ocean time level indices
	172	REAL(wp), DIMENSION(A2D(nn_hls),jpk), INTENT(in ) :: p_sh2 ! shear production term
	173	REAL(wp), DIMENSION(:,:,:) , INTENT(inout) :: p_avm, p_avt ! momentum and tracer Kz (w-points)
[1492]	174	!!----------------------------------------------------------------------
[1481]	175	!
[12377]	176	CALL tke_tke( Kbb, Kmm, p_sh2, p_avm, p_avt ) ! now tke (en)
[5656]	177	!
[12377]	178	CALL tke_avn( Kbb, Kmm, p_avm, p_avt ) ! now avt, avm, dissl
[3632]	179	!
[5656]	180	END SUBROUTINE zdf_tke
[1239]	181
[1492]	182
[12377]	183	SUBROUTINE tke_tke( Kbb, Kmm, p_sh2, p_avm, p_avt )
[1239]	184	!!----------------------------------------------------------------------
[1492]	185	!! * ROUTINE tke_tke *
	186	!!
	187	!! ** Purpose : Compute the now Turbulente Kinetic Energy (TKE)
	188	!!
	189	!! ** Method : - TKE surface boundary condition
[2528]	190	!! - source term due to Langmuir cells (Axell JGR 2002) (ln_lc=T)
[9019]	191	!! - source term due to shear (= Kz dz[Ub] * dz[Un] )
[1492]	192	!! - Now TKE : resolution of the TKE equation by inverting
	193	!! a tridiagonal linear system by a "methode de chasse"
	194	!! - increase TKE due to surface and internal wave breaking
[14072]	195	!! NB: when sea-ice is present, both LC parameterization
	196	!! and TKE penetration are turned off when the ice fraction
	197	!! is smaller than 0.25
[1492]	198	!!
	199	!! ** Action : - en : now turbulent kinetic energy)
[1239]	200	!! ---------------------------------------------------------------------
[9019]	201	USE zdf_oce , ONLY : en ! ocean vertical physics
	202	!!
[14834]	203	INTEGER , INTENT(in ) :: Kbb, Kmm ! ocean time level indices
	204	REAL(wp), DIMENSION(A2D(nn_hls),jpk) , INTENT(in ) :: p_sh2 ! shear production term
	205	REAL(wp), DIMENSION(:,:,:) , INTENT(in ) :: p_avm, p_avt ! vertical eddy viscosity & diffusivity (w-points)
[9019]	206	!
[13472]	207	INTEGER :: ji, jj, jk ! dummy loop arguments
[9019]	208	REAL(wp) :: zetop, zebot, zmsku, zmskv ! local scalars
	209	REAL(wp) :: zrhoa = 1.22 ! Air density kg/m3
	210	REAL(wp) :: zcdrag = 1.5e-3 ! drag coefficient
[13472]	211	REAL(wp) :: zbbrau, zbbirau, zri ! local scalars
	212	REAL(wp) :: zfact1, zfact2, zfact3 ! - -
	213	REAL(wp) :: ztx2 , zty2 , zcof ! - -
	214	REAL(wp) :: ztau , zdif ! - -
	215	REAL(wp) :: zus , zwlc , zind ! - -
	216	REAL(wp) :: zzd_up, zzd_lw ! - -
[14007]	217	REAL(wp) :: ztaui, ztauj, z1_norm
[14834]	218	INTEGER , DIMENSION(A2D(nn_hls)) :: imlc
	219	REAL(wp), DIMENSION(A2D(nn_hls)) :: zice_fra, zhlc, zus3, zWlc2
	220	REAL(wp), DIMENSION(A2D(nn_hls),jpk) :: zpelc, zdiag, zd_up, zd_lw
[14983]	221	REAL(wp), DIMENSION(:,:,:), ALLOCATABLE :: ztmp ! for diags
[1239]	222	!!--------------------------------------------------------------------
[1492]	223	!
[13472]	224	zbbrau = rn_ebb / rho0 ! Local constant initialisation
	225	zbbirau = 3.75_wp / rho0
[14072]	226	zfact1 = -.5_wp * rn_Dt
[13472]	227	zfact2 = 1.5_wp * rn_Dt * rn_ediss
	228	zfact3 = 0.5_wp * rn_ediss
[1492]	229	!
[14007]	230	zpelc(:,:,:) = 0._wp ! need to be initialised in case ln_lc is not used
	231	!
[13472]	232	! ice fraction considered for attenuation of langmuir & wave breaking
	233	SELECT CASE ( nn_eice )
	234	CASE( 0 ) ; zice_fra(:,:) = 0._wp
[14834]	235	CASE( 1 ) ; zice_fra(:,:) = TANH( fr_i(A2D(nn_hls)) * 10._wp )
	236	CASE( 2 ) ; zice_fra(:,:) = fr_i(A2D(nn_hls))
	237	CASE( 3 ) ; zice_fra(:,:) = MIN( 4._wp * fr_i(A2D(nn_hls)) , 1._wp )
[13472]	238	END SELECT
	239	!
[1492]	240	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[9019]	241	! ! Surface/top/bottom boundary condition on tke
[1492]	242	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[13472]	243	!
[14834]	244	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14057]	245	en(ji,jj,1) = MAX( rn_emin0, zbbrau * taum(ji,jj) )
[14007]	246	zdiag(ji,jj,1) = 1._wp/en(ji,jj,1)
[14072]	247	zd_lw(ji,jj,1) = 1._wp
[14007]	248	zd_up(ji,jj,1) = 0._wp
[12377]	249	END_2D
[9019]	250	!
[1492]	251	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	252	! ! Bottom boundary condition on tke
	253	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[1719]	254	!
[12489]	255	! en(bot) = (ebb0/rho0)0.5sqrt(u_botfr^2+v_botfr^2) (min value rn_emin)
[9019]	256	! where ebb0 does not includes surface wave enhancement (i.e. ebb0=3.75)
	257	! Note that stress averaged is done using an wet-only calculation of u and v at t-point like in zdfsh2
[1492]	258	!
[13461]	259	IF( .NOT.ln_drg_OFF ) THEN !== friction used as top/bottom boundary condition on TKE
[9019]	260	!
[14834]	261	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! bottom friction
[12377]	262	zmsku = ( 2. - umask(ji-1,jj,mbkt(ji,jj)) * umask(ji,jj,mbkt(ji,jj)) )
	263	zmskv = ( 2. - vmask(ji,jj-1,mbkt(ji,jj)) * vmask(ji,jj,mbkt(ji,jj)) )
[12489]	264	! ! where 0.001875 = (rn_ebb0/rho0) * 0.5 = 3.75*0.5/1000. (CAUTION CdU<0)
[12377]	265	zebot = - 0.001875_wp * rCdU_bot(ji,jj) * SQRT( ( zmsku( uu(ji,jj,mbkt(ji,jj),Kbb)+uu(ji-1,jj,mbkt(ji,jj),Kbb) ) )*2 &
	266	& + ( zmskv( vv(ji,jj,mbkt(ji,jj),Kbb)+vv(ji,jj-1,mbkt(ji,jj),Kbb) ) )*2 )
	267	en(ji,jj,mbkt(ji,jj)+1) = MAX( zebot, rn_emin ) * ssmask(ji,jj)
	268	END_2D
[13461]	269	IF( ln_isfcav ) THEN
[14834]	270	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! top friction
[12377]	271	zmsku = ( 2. - umask(ji-1,jj,mikt(ji,jj)) * umask(ji,jj,mikt(ji,jj)) )
	272	zmskv = ( 2. - vmask(ji,jj-1,mikt(ji,jj)) * vmask(ji,jj,mikt(ji,jj)) )
[12489]	273	! ! where 0.001875 = (rn_ebb0/rho0) * 0.5 = 3.75*0.5/1000. (CAUTION CdU<0)
[12377]	274	zetop = - 0.001875_wp * rCdU_top(ji,jj) * SQRT( ( zmsku( uu(ji,jj,mikt(ji,jj),Kbb)+uu(ji-1,jj,mikt(ji,jj),Kbb) ) )*2 &
	275	& + ( zmskv( vv(ji,jj,mikt(ji,jj),Kbb)+vv(ji,jj-1,mikt(ji,jj),Kbb) ) )*2 )
[12702]	276	! (1._wp - tmask(ji,jj,1)) * ssmask(ji,jj) = 1 where ice shelves are present
	277	en(ji,jj,mikt(ji,jj)) = en(ji,jj,1) * tmask(ji,jj,1) &
	278	& + MAX( zetop, rn_emin ) * (1._wp - tmask(ji,jj,1)) * ssmask(ji,jj)
[12377]	279	END_2D
[9019]	280	ENDIF
	281	!
	282	ENDIF
	283	!
[1492]	284	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[14007]	285	IF( ln_lc ) THEN ! Langmuir circulation source term added to tke (Axell JGR 2002)
[1492]	286	! !>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>
[1239]	287	!
[14007]	288	! !* Langmuir velocity scale
	289	!
	290	IF ( cpl_sdrftx ) THEN ! Surface Stokes Drift available
	291	! ! Craik-Leibovich velocity scale Wlc = ( u* u_s )^1/2 with u* = (taum/rho0)^1/2
	292	! ! associated kinetic energy : 1/2 (Wlc)^2 = u* u_s
	293	! ! more precisely, it is the dot product that must be used :
	294	! ! 1/2 (W_lc)^2 = MAX( u* u_s + v* v_s , 0 ) only the positive part
	295	!!gm ! PS: currently we don't have neither the 2 stress components at t-point !nor the angle between u* and u_s
	296	!!gm ! so we will overestimate the LC velocity.... !!gm I will do the work if !LC have an effect !
[14834]	297	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	298	!!XC zWlc2(ji,jj) = 0.5_wp * SQRT( taum(ji,jj) * r1_rho0 * ( ut0sd(ji,jj)2 +vt0sd(ji,jj)2 ) )
	299	zWlc2(ji,jj) = 0.5_wp * ( ut0sd(ji,jj)2 +vt0sd(ji,jj)2 )
	300	END_2D
	301	!
	302	! Projection of Stokes drift in the wind stress direction
	303	!
[14834]	304	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	305	ztaui = 0.5_wp * ( utau(ji,jj) + utau(ji-1,jj) )
	306	ztauj = 0.5_wp * ( vtau(ji,jj) + vtau(ji,jj-1) )
	307	z1_norm = 1._wp / MAX( SQRT(ztauiztaui+ztaujztauj), 1.e-12 ) * tmask(ji,jj,1)
	308	zWlc2(ji,jj) = 0.5_wp * z1_norm * ( MAX( ut0sd(ji,jj)ztaui + vt0sd(ji,jj)ztauj, 0._wp ) )**2
	309	END_2D
	310	ELSE ! Surface Stokes drift deduced from surface stress
	311	! ! Wlc = u_s with u_s = 0.016*U_10m, the surface stokes drift (Axell 2002, Eq.44)
	312	! ! using \|tau\| = rho_air Cd \|U_10m\|^2 , it comes:
	313	! ! Wlc = 0.016 * [\|tau\|/(rho_air Cdrag) ]^1/2 and thus:
	314	! ! 1/2 Wlc^2 = 0.5 * 0.016 * 0.016 \|tau\| /( rho_air Cdrag )
	315	zcof = 0.5 * 0.016 * 0.016 / ( zrhoa * zcdrag ) ! to convert stress in 10m wind using a constant drag
[14834]	316	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	317	zWlc2(ji,jj) = zcof * taum(ji,jj)
	318	END_2D
	319	!
	320	ENDIF
	321	!
	322	! !* Depth of the LC circulation (Axell 2002, Eq.47)
	323	! !- LHS of Eq.47
[14834]	324	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
	325	zpelc(ji,jj,1) = MAX( rn2b(ji,jj,1), 0._wp ) * gdepw(ji,jj,1,Kmm) * e3w(ji,jj,1,Kmm)
	326	END_2D
	327	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpk )
	328	zpelc(ji,jj,jk) = zpelc(ji,jj,jk-1) + &
	329	& MAX( rn2b(ji,jj,jk), 0._wp ) * gdepw(ji,jj,jk,Kmm) * e3w(ji,jj,jk,Kmm)
	330	END_3D
[14007]	331	!
	332	! !- compare LHS to RHS of Eq.47
[14834]	333	imlc(:,:) = mbkt(A2D(nn_hls)) + 1 ! Initialization to the number of w ocean point (=2 over land)
	334	DO_3DS( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, jpkm1, 2, -1 )
[14007]	335	IF( zpelc(ji,jj,jk) > zWlc2(ji,jj) ) imlc(ji,jj) = jk
[12377]	336	END_3D
[1492]	337	! ! finite LC depth
[14834]	338	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[12377]	339	zhlc(ji,jj) = gdepw(ji,jj,imlc(ji,jj),Kmm)
	340	END_2D
[14007]	341	!
[1705]	342	zcof = 0.016 / SQRT( zrhoa * zcdrag )
[14834]	343	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	344	zus = SQRT( 2. * zWlc2(ji,jj) ) ! Stokes drift
[13472]	345	zus3(ji,jj) = MAX( 0._wp, 1._wp - zice_fra(ji,jj) ) * zus * zus * zus * tmask(ji,jj,1) ! zus > 0. ok
[12377]	346	END_2D
[14834]	347	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) !* TKE Langmuir circulation source term added to en
[14072]	348	IF ( zus3(ji,jj) /= 0._wp ) THEN
[12377]	349	IF ( gdepw(ji,jj,jk,Kmm) - zhlc(ji,jj) < 0 .AND. wmask(ji,jj,jk) /= 0. ) THEN
	350	! ! vertical velocity due to LC
[13472]	351	zwlc = rn_lc * SIN( rpi * gdepw(ji,jj,jk,Kmm) / zhlc(ji,jj) )
[12377]	352	! ! TKE Langmuir circulation source term
[13472]	353	en(ji,jj,jk) = en(ji,jj,jk) + rn_Dt * zus3(ji,jj) * ( zwlc * zwlc * zwlc ) / zhlc(ji,jj)
[12377]	354	ENDIF
	355	ENDIF
	356	END_3D
[1239]	357	!
	358	ENDIF
[1492]	359	!
	360	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	361	! ! Now Turbulent kinetic energy (output in en)
	362	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	363	! ! Resolution of a tridiagonal linear system by a "methode de chasse"
	364	! ! computation from level 2 to jpkm1 (e(1) already computed and e(jpk)=0 ).
	365	! ! zdiag : diagonal zd_up : upper diagonal zd_lw : lower diagonal
	366	!
[13497]	367	IF( nn_pdl == 1 ) THEN !* Prandtl number = F( Ri )
[14834]	368	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	369	! ! local Richardson number
[13226]	370	IF (rn2b(ji,jj,jk) <= 0.0_wp) then
	371	zri = 0.0_wp
	372	ELSE
	373	zri = rn2b(ji,jj,jk) * p_avm(ji,jj,jk) / ( p_sh2(ji,jj,jk) + rn_bshear )
	374	ENDIF
[12377]	375	! ! inverse of Prandtl number
	376	apdlr(ji,jj,jk) = MAX( 0.1_wp, ri_cri / MAX( ri_cri , zri ) )
	377	END_3D
[5656]	378	ENDIF
[14072]	379	!
[14834]	380	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) !* Matrix and right hand side in en
[12377]	381	zcof = zfact1 * tmask(ji,jj,jk)
	382	! ! A minimum of 2.e-5 m2/s is imposed on TKE vertical
	383	! ! eddy coefficient (ensure numerical stability)
	384	zzd_up = zcof * MAX( p_avm(ji,jj,jk+1) + p_avm(ji,jj,jk ) , 2.e-5_wp ) & ! upper diagonal
[13472]	385	& / ( e3t(ji,jj,jk ,Kmm) * e3w(ji,jj,jk ,Kmm) )
[12377]	386	zzd_lw = zcof * MAX( p_avm(ji,jj,jk ) + p_avm(ji,jj,jk-1) , 2.e-5_wp ) & ! lower diagonal
[13472]	387	& / ( e3t(ji,jj,jk-1,Kmm) * e3w(ji,jj,jk ,Kmm) )
[12377]	388	!
	389	zd_up(ji,jj,jk) = zzd_up ! Matrix (zdiag, zd_up, zd_lw)
	390	zd_lw(ji,jj,jk) = zzd_lw
	391	zdiag(ji,jj,jk) = 1._wp - zzd_lw - zzd_up + zfact2 * dissl(ji,jj,jk) * wmask(ji,jj,jk)
	392	!
	393	! ! right hand side in en
[12489]	394	en(ji,jj,jk) = en(ji,jj,jk) + rn_Dt * ( p_sh2(ji,jj,jk) & ! shear
[12377]	395	& - p_avt(ji,jj,jk) * rn2(ji,jj,jk) & ! stratification
	396	& + zfact3 * dissl(ji,jj,jk) * en(ji,jj,jk) & ! dissipation
	397	& ) * wmask(ji,jj,jk)
	398	END_3D
[14007]	399	!
	400	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	401	! ! Surface boundary condition on tke if
	402	! ! coupling with waves
	403	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	404	!
	405	IF ( cpl_phioc .and. ln_phioc ) THEN
[14072]	406	SELECT CASE (nn_bc_surf) ! Boundary Condition using surface TKE flux from waves
[14007]	407
	408	CASE ( 0 ) ! Dirichlet BC
[14834]	409	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! en(1) = rn_ebb taum / rho0 (min value rn_emin0)
[14007]	410	IF ( phioc(ji,jj) < 0 ) phioc(ji,jj) = 0._wp
	411	en(ji,jj,1) = MAX( rn_emin0, .5 * ( 15.8 * phioc(ji,jj) / rho0 )*(2./3.) ) tmask(ji,jj,1)
	412	zdiag(ji,jj,1) = 1._wp/en(ji,jj,1) ! choose to keep coherence with former estimation of
	413	END_2D
	414
	415	CASE ( 1 ) ! Neumann BC
[14834]	416	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	417	IF ( phioc(ji,jj) < 0 ) phioc(ji,jj) = 0._wp
	418	en(ji,jj,2) = en(ji,jj,2) + ( rn_Dt * phioc(ji,jj) / rho0 ) /e3w(ji,jj,2,Kmm)
	419	en(ji,jj,1) = en(ji,jj,2) + (2 * e3t(ji,jj,1,Kmm) * phioc(ji,jj)/rho0) / ( p_avm(ji,jj,1) + p_avm(ji,jj,2) )
	420	zdiag(ji,jj,2) = zdiag(ji,jj,2) + zd_lw(ji,jj,2)
	421	zdiag(ji,jj,1) = 1._wp
	422	zd_lw(ji,jj,2) = 0._wp
	423	END_2D
	424
	425	END SELECT
	426
	427	ENDIF
	428	!
[5120]	429	! !* Matrix inversion from level 2 (tke prescribed at level 1)
[15071]	430	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1
[12377]	431	zdiag(ji,jj,jk) = zdiag(ji,jj,jk) - zd_lw(ji,jj,jk) * zd_up(ji,jj,jk-1) / zdiag(ji,jj,jk-1)
	432	END_3D
[14007]	433	!XC : commented to allow for neumann boundary condition
	434	! DO_2D( 0, 0, 0, 0 )
	435	! zd_lw(ji,jj,2) = en(ji,jj,2) - zd_lw(ji,jj,2) * en(ji,jj,1) ! Surface boudary conditions on tke
	436	! END_2D
[15071]	437	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	438	zd_lw(ji,jj,jk) = en(ji,jj,jk) - zd_lw(ji,jj,jk) / zdiag(ji,jj,jk-1) *zd_lw(ji,jj,jk-1)
	439	END_3D
[14834]	440	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! thrid recurrence : Ek = ( Lk - Uk * Ek+1 ) / Dk
[12377]	441	en(ji,jj,jpkm1) = zd_lw(ji,jj,jpkm1) / zdiag(ji,jj,jpkm1)
	442	END_2D
[14834]	443	DO_3DS_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, jpk-2, 2, -1 )
[12377]	444	en(ji,jj,jk) = ( zd_lw(ji,jj,jk) - zd_up(ji,jj,jk) * en(ji,jj,jk+1) ) / zdiag(ji,jj,jk)
	445	END_3D
[14834]	446	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) ! set the minimum value of tke
[12377]	447	en(ji,jj,jk) = MAX( en(ji,jj,jk), rn_emin ) * wmask(ji,jj,jk)
	448	END_3D
[9019]	449	!
[14983]	450	! Kolmogorov energy of dissipation (W/kg)
	451	! ediss = Cesqrt(en)/Len
	452	! dissl = sqrt(en)/L
	453	IF( iom_use('ediss_k') ) THEN
	454	ALLOCATE( ztmp(A2D(nn_hls),jpk) )
[14985]	455	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 1, jpkm1 )
	456	ztmp(ji,jj,jk) = zfact3 * dissl(ji,jj,jk) * en(ji,jj,jk) * wmask(ji,jj,jk)
	457	END_3D
	458	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
	459	ztmp(ji,jj,jpk) = 0._wp
	460	END_2D
[14983]	461	CALL iom_put( 'ediss_k', ztmp )
	462	DEALLOCATE( ztmp )
	463	ENDIF
	464	!
[1492]	465	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	466	! ! TKE due to surface and internal wave breaking
	467	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[6140]	468	!!gm BUG : in the exp remove the depth of ssh !!!
[12377]	469	!!gm i.e. use gde3w in argument (gdepw(:,:,:,Kmm))
[13530]	470	!
	471	! penetration is partly switched off below sea-ice if nn_eice/=0
	472	!
[2528]	473	IF( nn_etau == 1 ) THEN !* penetration below the mixed layer (rn_efr fraction)
[14834]	474	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	475	en(ji,jj,jk) = en(ji,jj,jk) + rn_efr * en(ji,jj,1) * EXP( -gdepw(ji,jj,jk,Kmm) / htau(ji,jj) ) &
[13472]	476	& * MAX( 0._wp, 1._wp - zice_fra(ji,jj) ) * wmask(ji,jj,jk) * tmask(ji,jj,1)
[12377]	477	END_3D
[2528]	478	ELSEIF( nn_etau == 2 ) THEN !* act only at the base of the mixed layer (jk=nmln) (rn_efr fraction)
[14834]	479	DO_2D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[12377]	480	jk = nmln(ji,jj)
	481	en(ji,jj,jk) = en(ji,jj,jk) + rn_efr * en(ji,jj,1) * EXP( -gdepw(ji,jj,jk,Kmm) / htau(ji,jj) ) &
[13472]	482	& * MAX( 0._wp, 1._wp - zice_fra(ji,jj) ) * wmask(ji,jj,jk) * tmask(ji,jj,1)
[12377]	483	END_2D
[2528]	484	ELSEIF( nn_etau == 3 ) THEN !* penetration belox the mixed layer (HF variability)
[14834]	485	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	486	ztx2 = utau(ji-1,jj ) + utau(ji,jj)
	487	zty2 = vtau(ji ,jj-1) + vtau(ji,jj)
[14072]	488	ztau = 0.5_wp * SQRT( ztx2 * ztx2 + zty2 * zty2 ) * tmask(ji,jj,1) ! module of the mean stress
	489	zdif = taum(ji,jj) - ztau ! mean of modulus - modulus of the mean
[12377]	490	zdif = rhftau_scl * MAX( 0._wp, zdif + rhftau_add ) ! apply some modifications...
	491	en(ji,jj,jk) = en(ji,jj,jk) + zbbrau * zdif * EXP( -gdepw(ji,jj,jk,Kmm) / htau(ji,jj) ) &
[13472]	492	& * MAX( 0._wp, 1._wp - zice_fra(ji,jj) ) * wmask(ji,jj,jk) * tmask(ji,jj,1)
[12377]	493	END_3D
[1239]	494	ENDIF
[1492]	495	!
[1239]	496	END SUBROUTINE tke_tke
	497
[1492]	498
[12377]	499	SUBROUTINE tke_avn( Kbb, Kmm, p_avm, p_avt )
[1239]	500	!!----------------------------------------------------------------------
[1492]	501	!! * ROUTINE tke_avn *
[1239]	502	!!
[1492]	503	!! ** Purpose : Compute the vertical eddy viscosity and diffusivity
	504	!!
[14072]	505	!! ** Method : At this stage, en, the now TKE, is known (computed in
	506	!! the tke_tke routine). First, the now mixing lenth is
[1492]	507	!! computed from en and the strafification (N^2), then the mixings
	508	!! coefficients are computed.
	509	!! - Mixing length : a first evaluation of the mixing lengh
	510	!! scales is:
[14072]	511	!! mxl = sqrt(2*en) / N
[1492]	512	!! where N is the brunt-vaisala frequency, with a minimum value set
[2528]	513	!! to rmxl_min (rn_mxl0) in the interior (surface) ocean.
[14072]	514	!! The mixing and dissipative length scale are bound as follow :
[1492]	515	!! nn_mxl=0 : mxl bounded by the distance to surface and bottom.
	516	!! zmxld = zmxlm = mxl
	517	!! nn_mxl=1 : mxl bounded by the e3w and zmxld = zmxlm = mxl
[14072]	518	!! nn_mxl=2 : mxl bounded such that the vertical derivative of mxl is
[1492]	519	!! less than 1 (\|d/dz(mxl)\|<1) and zmxld = zmxlm = mxl
	520	!! nn_mxl=3 : mxl is bounded from the surface to the bottom usings
[14072]	521	!! \|d/dz(xml)\|<1 to obtain lup, and from the bottom to
	522	!! the surface to obtain ldown. the resulting length
[1492]	523	!! scales are:
[14072]	524	!! zmxld = sqrt( lup * ldown )
[1492]	525	!! zmxlm = min ( lup , ldown )
	526	!! - Vertical eddy viscosity and diffusivity:
	527	!! avm = max( avtb, rn_ediff * zmxlm * en^1/2 )
[14072]	528	!! avt = max( avmb, pdlr * avm )
[1492]	529	!! with pdlr=1 if nn_pdl=0, pdlr=1/pdl=F(Ri) otherwise.
	530	!!
[9019]	531	!! ** Action : - avt, avm : now vertical eddy diffusivity and viscosity (w-point)
[1239]	532	!!----------------------------------------------------------------------
[9019]	533	USE zdf_oce , ONLY : en, avtb, avmb, avtb_2d ! ocean vertical physics
	534	!!
[12377]	535	INTEGER , INTENT(in ) :: Kbb, Kmm ! ocean time level indices
[9019]	536	REAL(wp), DIMENSION(:,:,:), INTENT( out) :: p_avm, p_avt ! vertical eddy viscosity & diffusivity (w-points)
	537	!
[2715]	538	INTEGER :: ji, jj, jk ! dummy loop indices
[9019]	539	REAL(wp) :: zrn2, zraug, zcoef, zav ! local scalars
	540	REAL(wp) :: zdku, zdkv, zsqen ! - -
[13007]	541	REAL(wp) :: zemxl, zemlm, zemlp, zmaxice ! - -
[14834]	542	REAL(wp), DIMENSION(A2D(nn_hls),jpk) :: zmxlm, zmxld ! 3D workspace
[1239]	543	!!--------------------------------------------------------------------
[3294]	544	!
[1492]	545	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	546	! ! Mixing length
	547	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
	548	!
	549	! !* Buoyancy length scale: l=sqrt(2e/n*2)
	550	!
[5120]	551	! initialisation of interior minimum value (avoid a 2d loop with mikt)
[14072]	552	zmxlm(:,:,:) = rmxl_min
[7753]	553	zmxld(:,:,:) = rmxl_min
[14007]	554	!
	555	IF(ln_sdw .AND. ln_mxhsw) THEN
	556	zmxlm(:,:,1)= vkarmn * MAX ( 1.6 * hsw(:,:) , 0.02 ) ! surface mixing length = F(wave height)
	557	! from terray et al 1999 and mellor and blumberg 2004 it should be 0.85 and not 1.6
	558	zcoef = vkarmn * ( (rn_ediffrn_ediss)*0.25 ) / rn_ediff
	559	zmxlm(:,:,1)= zcoef * MAX ( 1.6 * hsw(:,:) , 0.02 ) ! surface mixing length = F(wave height)
	560	ELSE
[14072]	561	!
[14007]	562	IF( ln_mxl0 ) THEN ! surface mixing length = F(stress) : l=vkarmn2.e5taum/(rho0*g)
[13007]	563	!
[14007]	564	zraug = vkarmn * 2.e5_wp / ( rho0 * grav )
[13007]	565	#if ! defined key_si3 && ! defined key_cice
[14834]	566	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) ! No sea-ice
[14007]	567	zmxlm(ji,jj,1) = zraug * taum(ji,jj) * tmask(ji,jj,1)
	568	END_2D
[13007]	569	#else
[14007]	570	SELECT CASE( nn_mxlice ) ! Type of scaling under sea-ice
[13007]	571	!
[14007]	572	CASE( 0 ) ! No scaling under sea-ice
[14834]	573	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	574	zmxlm(ji,jj,1) = zraug * taum(ji,jj) * tmask(ji,jj,1)
	575	END_2D
	576	!
	577	CASE( 1 ) ! scaling with constant sea-ice thickness
[14834]	578	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	579	zmxlm(ji,jj,1) = ( ( 1._wp - fr_i(ji,jj) ) * zraug * taum(ji,jj) + &
	580	& fr_i(ji,jj) * rn_mxlice ) * tmask(ji,jj,1)
	581	END_2D
	582	!
	583	CASE( 2 ) ! scaling with mean sea-ice thickness
[14834]	584	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[13007]	585	#if defined key_si3
[14007]	586	zmxlm(ji,jj,1) = ( ( 1._wp - fr_i(ji,jj) ) * zraug * taum(ji,jj) + &
	587	& fr_i(ji,jj) * hm_i(ji,jj) * 2._wp ) * tmask(ji,jj,1)
[13007]	588	#elif defined key_cice
[14007]	589	zmaxice = MAXVAL( h_i(ji,jj,:) )
	590	zmxlm(ji,jj,1) = ( ( 1._wp - fr_i(ji,jj) ) * zraug * taum(ji,jj) + &
	591	& fr_i(ji,jj) * zmaxice ) * tmask(ji,jj,1)
[13007]	592	#endif
[14007]	593	END_2D
	594	!
	595	CASE( 3 ) ! scaling with max sea-ice thickness
[14834]	596	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	597	zmaxice = MAXVAL( h_i(ji,jj,:) )
	598	zmxlm(ji,jj,1) = ( ( 1._wp - fr_i(ji,jj) ) * zraug * taum(ji,jj) + &
	599	& fr_i(ji,jj) * zmaxice ) * tmask(ji,jj,1)
	600	END_2D
	601	!
	602	END SELECT
	603	#endif
[13007]	604	!
[14834]	605	DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 )
[14007]	606	zmxlm(ji,jj,1) = MAX( rn_mxl0, zmxlm(ji,jj,1) )
[13007]	607	END_2D
	608	!
[14007]	609	ELSE
	610	zmxlm(:,:,1) = rn_mxl0
	611	ENDIF
[1239]	612	ENDIF
	613	!
[14834]	614	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	615	zrn2 = MAX( rn2(ji,jj,jk), rsmall )
	616	zmxlm(ji,jj,jk) = MAX( rmxl_min, SQRT( 2._wp * en(ji,jj,jk) / zrn2 ) )
	617	END_3D
[1492]	618	!
	619	! !* Physical limits for the mixing length
	620	!
[14072]	621	zmxld(:,:, 1 ) = zmxlm(:,:,1) ! surface set to the minimum value
[7753]	622	zmxld(:,:,jpk) = rmxl_min ! last level set to the minimum value
[1492]	623	!
[1239]	624	SELECT CASE ( nn_mxl )
	625	!
[5836]	626	!!gm Not sure of that coding for ISF....
[12377]	627	! where wmask = 0 set zmxlm == e3w(:,:,:,Kmm)
[1239]	628	CASE ( 0 ) ! bounded by the distance to surface and bottom
[14834]	629	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	630	zemxl = MIN( gdepw(ji,jj,jk,Kmm) - gdepw(ji,jj,mikt(ji,jj),Kmm), zmxlm(ji,jj,jk), &
	631	& gdepw(ji,jj,mbkt(ji,jj)+1,Kmm) - gdepw(ji,jj,jk,Kmm) )
	632	! wmask prevent zmxlm = 0 if jk = mikt(ji,jj)
[13237]	633	zmxlm(ji,jj,jk) = zemxl * wmask(ji,jj,jk) &
	634	& + MIN( zmxlm(ji,jj,jk) , e3w(ji,jj,jk,Kmm) ) * (1 - wmask(ji,jj,jk))
	635	zmxld(ji,jj,jk) = zemxl * wmask(ji,jj,jk) &
	636	& + MIN( zmxlm(ji,jj,jk) , e3w(ji,jj,jk,Kmm) ) * (1 - wmask(ji,jj,jk))
[12377]	637	END_3D
[1239]	638	!
	639	CASE ( 1 ) ! bounded by the vertical scale factor
[14834]	640	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	641	zemxl = MIN( e3w(ji,jj,jk,Kmm), zmxlm(ji,jj,jk) )
	642	zmxlm(ji,jj,jk) = zemxl
	643	zmxld(ji,jj,jk) = zemxl
	644	END_3D
[1239]	645	!
	646	CASE ( 2 ) ! \|dk[xml]\| bounded by e3t :
[14834]	647	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) ! from the surface to the bottom :
[13237]	648	zmxlm(ji,jj,jk) = &
	649	& MIN( zmxlm(ji,jj,jk-1) + e3t(ji,jj,jk-1,Kmm), zmxlm(ji,jj,jk) )
[12377]	650	END_3D
[14834]	651	DO_3DS( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, jpkm1, 2, -1 ) ! from the bottom to the surface :
[12377]	652	zemxl = MIN( zmxlm(ji,jj,jk+1) + e3t(ji,jj,jk+1,Kmm), zmxlm(ji,jj,jk) )
	653	zmxlm(ji,jj,jk) = zemxl
	654	zmxld(ji,jj,jk) = zemxl
	655	END_3D
[1239]	656	!
	657	CASE ( 3 ) ! lup and ldown, \|dk[xml]\| bounded by e3t :
[14834]	658	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 ) ! from the surface to the bottom : lup
[13237]	659	zmxld(ji,jj,jk) = &
	660	& MIN( zmxld(ji,jj,jk-1) + e3t(ji,jj,jk-1,Kmm), zmxlm(ji,jj,jk) )
[12377]	661	END_3D
[14834]	662	DO_3DS( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, jpkm1, 2, -1 ) ! from the bottom to the surface : ldown
[13237]	663	zmxlm(ji,jj,jk) = &
	664	& MIN( zmxlm(ji,jj,jk+1) + e3t(ji,jj,jk+1,Kmm), zmxlm(ji,jj,jk) )
[12377]	665	END_3D
[14834]	666	DO_3D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12377]	667	zemlm = MIN ( zmxld(ji,jj,jk), zmxlm(ji,jj,jk) )
	668	zemlp = SQRT( zmxld(ji,jj,jk) * zmxlm(ji,jj,jk) )
	669	zmxlm(ji,jj,jk) = zemlm
	670	zmxld(ji,jj,jk) = zemlp
	671	END_3D
[1239]	672	!
	673	END SELECT
[1492]	674	!
	675	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[9019]	676	! ! Vertical eddy viscosity and diffusivity (avm and avt)
[1492]	677	! !<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<
[14834]	678	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 1, jpkm1 ) !* vertical eddy viscosity & diffivity at w-points
[12377]	679	zsqen = SQRT( en(ji,jj,jk) )
	680	zav = rn_ediff * zmxlm(ji,jj,jk) * zsqen
	681	p_avm(ji,jj,jk) = MAX( zav, avmb(jk) ) * wmask(ji,jj,jk)
	682	p_avt(ji,jj,jk) = MAX( zav, avtb_2d(ji,jj) * avtb(jk) ) * wmask(ji,jj,jk)
	683	dissl(ji,jj,jk) = zsqen / zmxld(ji,jj,jk)
	684	END_3D
[1492]	685	!
	686	!
[13497]	687	IF( nn_pdl == 1 ) THEN !* Prandtl number case: update avt
[14834]	688	DO_3D_OVR( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1, 2, jpkm1 )
[12698]	689	p_avt(ji,jj,jk) = MAX( apdlr(ji,jj,jk) * p_avt(ji,jj,jk), avtb_2d(ji,jj) * avtb(jk) ) * wmask(ji,jj,jk)
[12377]	690	END_3D
[1239]	691	ENDIF
[9019]	692	!
[12377]	693	IF(sn_cfctl%l_prtctl) THEN
[9440]	694	CALL prt_ctl( tab3d_1=en , clinfo1=' tke - e: ', tab3d_2=p_avt, clinfo2=' t: ', kdim=jpk)
	695	CALL prt_ctl( tab3d_1=p_avm, clinfo1=' tke - m: ', kdim=jpk )
[1239]	696	ENDIF
	697	!
[1492]	698	END SUBROUTINE tke_avn
[1239]	699
[1492]	700
[12377]	701	SUBROUTINE zdf_tke_init( Kmm )
[1239]	702	!!----------------------------------------------------------------------
[2528]	703	!! * ROUTINE zdf_tke_init *
[14072]	704	!!
	705	!! ** Purpose : Initialization of the vertical eddy diffivity and
[1492]	706	!! viscosity when using a tke turbulent closure scheme
[1239]	707	!!
[1601]	708	!! ** Method : Read the namzdf_tke namelist and check the parameters
[1492]	709	!! called at the first timestep (nit000)
[1239]	710	!!
[1601]	711	!! ** input : Namlist namzdf_tke
[1239]	712	!!
	713	!! ** Action : Increase by 1 the nstop flag is setting problem encounter
	714	!!----------------------------------------------------------------------
[9019]	715	USE zdf_oce , ONLY : ln_zdfiwm ! Internal Wave Mixing flag
	716	!!
[12377]	717	INTEGER, INTENT(in) :: Kmm ! time level index
	718	INTEGER :: ji, jj, jk ! dummy loop indices
	719	INTEGER :: ios
[1239]	720	!!
[13007]	721	NAMELIST/namzdf_tke/ rn_ediff, rn_ediss , rn_ebb , rn_emin , &
	722	& rn_emin0, rn_bshear, nn_mxl , ln_mxl0 , &
	723	& rn_mxl0 , nn_mxlice, rn_mxlice, &
[13461]	724	& nn_pdl , ln_lc , rn_lc , &
[14072]	725	& nn_etau , nn_htau , rn_efr , nn_eice , &
[14007]	726	& nn_bc_surf, nn_bc_bot, ln_mxhsw
[1239]	727	!!----------------------------------------------------------------------
[2715]	728	!
[4147]	729	READ ( numnam_ref, namzdf_tke, IOSTAT = ios, ERR = 901)
[11536]	730	901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namzdf_tke in reference namelist' )
[4147]	731
	732	READ ( numnam_cfg, namzdf_tke, IOSTAT = ios, ERR = 902 )
[11536]	733	902 IF( ios > 0 ) CALL ctl_nam ( ios , 'namzdf_tke in configuration namelist' )
[4624]	734	IF(lwm) WRITE ( numond, namzdf_tke )
[2715]	735	!
[2528]	736	ri_cri = 2._wp / ( 2._wp + rn_ediss / rn_ediff ) ! resulting critical Richardson number
[2715]	737	!
[1492]	738	IF(lwp) THEN !* Control print
[1239]	739	WRITE(numout,*)
[2528]	740	WRITE(numout,*) 'zdf_tke_init : tke turbulent closure scheme - initialisation'
	741	WRITE(numout,*) '~~~~~~~~~~~~'
[1601]	742	WRITE(numout,*) ' Namelist namzdf_tke : set tke mixing parameters'
[1705]	743	WRITE(numout,*) ' coef. to compute avt rn_ediff = ', rn_ediff
	744	WRITE(numout,*) ' Kolmogoroff dissipation coef. rn_ediss = ', rn_ediss
	745	WRITE(numout,*) ' tke surface input coef. rn_ebb = ', rn_ebb
	746	WRITE(numout,*) ' minimum value of tke rn_emin = ', rn_emin
	747	WRITE(numout,*) ' surface minimum value of tke rn_emin0 = ', rn_emin0
[9019]	748	WRITE(numout,*) ' prandl number flag nn_pdl = ', nn_pdl
[1705]	749	WRITE(numout,*) ' background shear (>0) rn_bshear = ', rn_bshear
	750	WRITE(numout,*) ' mixing length type nn_mxl = ', nn_mxl
[9019]	751	WRITE(numout,*) ' surface mixing length = F(stress) or not ln_mxl0 = ', ln_mxl0
	752	WRITE(numout,*) ' surface mixing length minimum value rn_mxl0 = ', rn_mxl0
[13472]	753	IF( ln_mxl0 ) THEN
	754	WRITE(numout,*) ' type of scaling under sea-ice nn_mxlice = ', nn_mxlice
	755	IF( nn_mxlice == 1 ) &
	756	WRITE(numout,*) ' ice thickness when scaling under sea-ice rn_mxlice = ', rn_mxlice
	757	SELECT CASE( nn_mxlice ) ! Type of scaling under sea-ice
	758	CASE( 0 ) ; WRITE(numout,*) ' ==>>> No scaling under sea-ice'
	759	CASE( 1 ) ; WRITE(numout,*) ' ==>>> scaling with constant sea-ice thickness'
	760	CASE( 2 ) ; WRITE(numout,*) ' ==>>> scaling with mean sea-ice thickness'
	761	CASE( 3 ) ; WRITE(numout,*) ' ==>>> scaling with max sea-ice thickness'
	762	CASE DEFAULT
	763	CALL ctl_stop( 'zdf_tke_init: wrong value for nn_mxlice, should be 0,1,2,3 or 4')
	764	END SELECT
	765	ENDIF
[9019]	766	WRITE(numout,*) ' Langmuir cells parametrization ln_lc = ', ln_lc
	767	WRITE(numout,*) ' coef to compute vertical velocity of LC rn_lc = ', rn_lc
[14007]	768	IF ( cpl_phioc .and. ln_phioc ) THEN
	769	SELECT CASE( nn_bc_surf) ! Type of scaling under sea-ice
	770	CASE( 0 ) ; WRITE(numout,*) ' nn_bc_surf=0 ==>>> DIRICHLET SBC using surface TKE flux from waves'
	771	CASE( 1 ) ; WRITE(numout,*) ' nn_bc_surf=1 ==>>> NEUMANN SBC using surface TKE flux from waves'
	772	END SELECT
	773	ENDIF
[1705]	774	WRITE(numout,*) ' test param. to add tke induced by wind nn_etau = ', nn_etau
[9019]	775	WRITE(numout,*) ' type of tke penetration profile nn_htau = ', nn_htau
	776	WRITE(numout,*) ' fraction of TKE that penetrates rn_efr = ', rn_efr
[13472]	777	WRITE(numout,*) ' langmuir & surface wave breaking under ice nn_eice = ', nn_eice
[14072]	778	SELECT CASE( nn_eice )
[13472]	779	CASE( 0 ) ; WRITE(numout,*) ' ==>>> no impact of ice cover on langmuir & surface wave breaking'
	780	CASE( 1 ) ; WRITE(numout,) ' ==>>> weigthed by 1-TANH( fr_i(:,:) 10 )'
	781	CASE( 2 ) ; WRITE(numout,*) ' ==>>> weighted by 1-fr_i(:,:)'
	782	CASE( 3 ) ; WRITE(numout,) ' ==>>> weighted by 1-MIN( 1, 4 fr_i(:,:) )'
	783	CASE DEFAULT
	784	CALL ctl_stop( 'zdf_tke_init: wrong value for nn_eice, should be 0,1,2, or 3')
[14072]	785	END SELECT
[9019]	786	WRITE(numout,*)
[9190]	787	WRITE(numout,*) ' ==>>> critical Richardson nb with your parameters ri_cri = ', ri_cri
[9019]	788	WRITE(numout,*)
[1239]	789	ENDIF
[2715]	790	!
[9019]	791	IF( ln_zdfiwm ) THEN ! Internal wave-driven mixing
	792	rn_emin = 1.e-10_wp ! specific values of rn_emin & rmxl_min are used
	793	rmxl_min = 1.e-03_wp ! associated avt minimum = molecular salt diffusivity (10^-9 m2/s)
[9190]	794	IF(lwp) WRITE(numout,*) ' ==>>> Internal wave-driven mixing case: force rn_emin = 1.e-10 and rmxl_min = 1.e-3'
[9019]	795	ELSE ! standard case : associated avt minimum = molecular viscosity (10^-6 m2/s)
	796	rmxl_min = 1.e-6_wp / ( rn_ediff * SQRT( rn_emin ) ) ! resulting minimum length to recover molecular viscosity
[9190]	797	IF(lwp) WRITE(numout,*) ' ==>>> minimum mixing length with your parameters rmxl_min = ', rmxl_min
[9019]	798	ENDIF
	799	!
[2715]	800	! ! allocate tke arrays
	801	IF( zdf_tke_alloc() /= 0 ) CALL ctl_stop( 'STOP', 'zdf_tke_init : unable to allocate arrays' )
	802	!
[1492]	803	! !* Check of some namelist values
[14834]	804	IF( nn_mxl < 0 .OR. nn_mxl > 3 ) CALL ctl_stop( 'bad flag: nn_mxl is 0, 1, 2 or 3' )
	805	IF( nn_pdl < 0 .OR. nn_pdl > 1 ) CALL ctl_stop( 'bad flag: nn_pdl is 0 or 1' )
	806	IF( nn_htau < 0 .OR. nn_htau > 1 ) CALL ctl_stop( 'bad flag: nn_htau is 0 or 1' )
[5407]	807	IF( nn_etau == 3 .AND. .NOT. ln_cpl ) CALL ctl_stop( 'nn_etau == 3 : HF taum only known in coupled mode' )
[9019]	808	!
[2528]	809	IF( ln_mxl0 ) THEN
[9169]	810	IF(lwp) WRITE(numout,*)
[9190]	811	IF(lwp) WRITE(numout,*) ' ==>>> use a surface mixing length = F(stress) : set rn_mxl0 = rmxl_min'
[2528]	812	rn_mxl0 = rmxl_min
	813	ENDIF
[1492]	814	! !* depth of penetration of surface tke
[14072]	815	IF( nn_etau /= 0 ) THEN
[1601]	816	SELECT CASE( nn_htau ) ! Choice of the depth of penetration
[2528]	817	CASE( 0 ) ! constant depth penetration (here 10 meters)
[7753]	818	htau(:,:) = 10._wp
[2528]	819	CASE( 1 ) ! F(latitude) : 0.5m to 30m poleward of 40 degrees
[14072]	820	htau(:,:) = MAX( 0.5_wp, MIN( 30._wp, 45._wp* ABS( SIN( rpi/180._wp * gphit(:,:) ) ) ) )
[1492]	821	END SELECT
	822	ENDIF
[9019]	823	! !* read or initialize all required files
[14072]	824	CALL tke_rst( nit000, 'READ' ) ! (en, avt_k, avm_k, dissl)
[1239]	825	!
[2528]	826	END SUBROUTINE zdf_tke_init
[1239]	827
	828
[1531]	829	SUBROUTINE tke_rst( kt, cdrw )
[9019]	830	!!---------------------------------------------------------------------
	831	!! * ROUTINE tke_rst *
[14072]	832	!!
[9019]	833	!! ** Purpose : Read or write TKE file (en) in restart file
	834	!!
	835	!! ** Method : use of IOM library
[14072]	836	!! if the restart does not contain TKE, en is either
	837	!! set to rn_emin or recomputed
[9019]	838	!!----------------------------------------------------------------------
	839	USE zdf_oce , ONLY : en, avt_k, avm_k ! ocean vertical physics
	840	!!
	841	INTEGER , INTENT(in) :: kt ! ocean time-step
	842	CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag
	843	!
	844	INTEGER :: jit, jk ! dummy loop indices
	845	INTEGER :: id1, id2, id3, id4 ! local integers
	846	!!----------------------------------------------------------------------
	847	!
[14072]	848	IF( TRIM(cdrw) == 'READ' ) THEN ! Read/initialise
[9019]	849	! ! ---------------
	850	IF( ln_rstart ) THEN !* Read the restart file
	851	id1 = iom_varid( numror, 'en' , ldstop = .FALSE. )
	852	id2 = iom_varid( numror, 'avt_k', ldstop = .FALSE. )
	853	id3 = iom_varid( numror, 'avm_k', ldstop = .FALSE. )
	854	id4 = iom_varid( numror, 'dissl', ldstop = .FALSE. )
	855	!
	856	IF( MIN( id1, id2, id3, id4 ) > 0 ) THEN ! fields exist
[13970]	857	CALL iom_get( numror, jpdom_auto, 'en' , en )
	858	CALL iom_get( numror, jpdom_auto, 'avt_k', avt_k )
	859	CALL iom_get( numror, jpdom_auto, 'avm_k', avm_k )
	860	CALL iom_get( numror, jpdom_auto, 'dissl', dissl )
[9019]	861	ELSE ! start TKE from rest
[9169]	862	IF(lwp) WRITE(numout,*)
[9190]	863	IF(lwp) WRITE(numout,*) ' ==>>> previous run without TKE scheme, set en to background values'
[9019]	864	en (:,:,:) = rn_emin * wmask(:,:,:)
	865	dissl(:,:,:) = 1.e-12_wp
	866	! avt_k, avm_k already set to the background value in zdf_phy_init
	867	ENDIF
	868	ELSE !* Start from rest
[9169]	869	IF(lwp) WRITE(numout,*)
[9190]	870	IF(lwp) WRITE(numout,*) ' ==>>> start from rest: set en to the background value'
[9019]	871	en (:,:,:) = rn_emin * wmask(:,:,:)
	872	dissl(:,:,:) = 1.e-12_wp
	873	! avt_k, avm_k already set to the background value in zdf_phy_init
	874	ENDIF
	875	!
	876	ELSEIF( TRIM(cdrw) == 'WRITE' ) THEN ! Create restart file
	877	! ! -------------------
[9169]	878	IF(lwp) WRITE(numout,*) '---- tke_rst ----'
[13970]	879	CALL iom_rstput( kt, nitrst, numrow, 'en' , en )
	880	CALL iom_rstput( kt, nitrst, numrow, 'avt_k', avt_k )
	881	CALL iom_rstput( kt, nitrst, numrow, 'avm_k', avm_k )
	882	CALL iom_rstput( kt, nitrst, numrow, 'dissl', dissl )
[9019]	883	!
	884	ENDIF
	885	!
[1531]	886	END SUBROUTINE tke_rst
[1239]	887
	888	!!======================================================================
[1531]	889	END MODULE zdftke

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source: NEMO/trunk/src/OCE/ZDF/zdftke.F90

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