! translated from NN f77 to F90 and put into WRF by Mariusz Pagowski ! NOAA/GSD & CIRA/CSU, Feb 2008 ! changes to original code: ! 1. code is 1d (in z) ! 2. no advection of TKE, covariances and variances ! 3. Cranck-Nicholson replaced with the implicit scheme ! 4. removed terrain dependent grid since input in WRF in actual ! distances in z[m] ! 5. cosmetic changes to adhere to WRF standard (remove common blocks, ! intent etc) !------------------------------------------------------------------- !Modifications implemented by Joseph Olson NOAA/GSD/AMB - CU/CIRES !(approved by Mikio Nakanishi): ! 1. Addition of BouLac mixing length in the free atmosphere. ! 2. Changed the turbulent mixing length to be integrated from the ! surface to the top of the BL + a transition layer depth. ! 3. Option to use Kitamura/Canuto modification which removes the ! critical Richardson number and negative TKE (default). ! 4. Hybrid PBL height diagnostic, which blends a theta-v-based ! definition in neutral/convective BL and a TKE-based definition ! in stable conditions. ! For changes 1 and 3, see "JOE's mods" below: !------------------------------------------------------------------- MODULE module_bl_mynn 3 USE module_model_constants, only: & &karman, g, p1000mb, & &cp, r_d, rcp, xlv, & &svp1, svp2, svp3, svpt0, ep_1, ep_2 !------------------------------------------------------------------- IMPLICIT NONE !------------------------------------------------------------------- ! The parameters below depend on stability functions of module_sf_mynn. REAL, PARAMETER :: cphm_st=5.0, cphm_unst=16.0, & cphh_st=5.0, cphh_unst=16.0 REAL, PARAMETER :: xlvcp=xlv/cp, ev=xlv, rd=r_d, rk=cp/rd, & &svp11=svp1*1.e3, p608=ep_1, ep_3=1.-ep_2 REAL, PARAMETER :: tref=300.0 ! reference temperature (K) REAL, PARAMETER :: tv0=p608*tref, tv1=(1.+p608)*tref, gtr=g/tref ! Closure constants REAL, PARAMETER :: & &vk = karman, & &pr = 0.74, & &g1 = 0.235, & &b1 = 24.0, & &b2 = 15.0, & ! CKmod NN2009 &c2 = 0.729, & ! 0.729, & !0.75, & &c3 = 0.340, & ! 0.340, & !0.352, & &c4 = 0.0, & &c5 = 0.2, & &a1 = b1*( 1.0-3.0*g1 )/6.0, & ! &c1 = g1 -1.0/( 3.0*a1*b1**(1.0/3.0) ), & &c1 = g1 -1.0/( 3.0*a1*2.88449914061481660), & &a2 = a1*( g1-c1 )/( g1*pr ), & &g2 = b2/b1*( 1.0-c3 ) +2.0*a1/b1*( 3.0-2.0*c2 ) REAL, PARAMETER :: & &cc2 = 1.0-c2, & &cc3 = 1.0-c3, & &e1c = 3.0*a2*b2*cc3, & &e2c = 9.0*a1*a2*cc2, & &e3c = 9.0*a2*a2*cc2*( 1.0-c5 ), & &e4c = 12.0*a1*a2*cc2, & &e5c = 6.0*a1*a1 ! Constants for length scale REAL, PARAMETER :: qmin=0.0, zmax=1.0, cns=2.1, & !NN2009: &alp1=0.23, alp2=1.0, alp3=5.0, alp4=100.0, Sqfac=3.0 &alp1=0.23, alp2=0.60, alp3=3.0, alp4=20.0, Sqfac=2.0 ! Constants for gravitational settling ! REAL, PARAMETER :: gno=1.e6/(1.e8)**(2./3.), gpw=5./3., qcgmin=1.e-8 REAL, PARAMETER :: gno=4.64158883361278196 REAL, PARAMETER :: gpw=5./3., qcgmin=1.e-8,qkemin=1.e-12 ! REAL, PARAMETER :: pblh_ref=1500. REAL, PARAMETER :: rr2=0.7071068, rrp=0.3989423 !JOE's mods !Use Canuto/Kitamura mod (remove Ric and negative TKE) (1:yes, 0:no) !For more info, see Canuto et al. (2008 JAS) and Kitamura (Journal of the !Meteorological Society of Japan, Vol. 88, No. 5, pp. 857-864, 2010). !Note that this change required further modification of other parameters !above (c2, c3, alp2, and Sqfac). If you want to remove this option, set these !parameters back to NN2009 values (see commented out lines next to the !parameters above). This only removes the negative TKE problem !but does not necessarily improve performance - neutral impact. REAL, PARAMETER :: CKmod=1. !Use BouLac mixing length in free atmosphere (1:yes, 0:no) !This helps remove excessively large mixing in unstable layers aloft. REAL, PARAMETER :: BLmod=1. !JOE-end INTEGER :: mynn_level CONTAINS ! ********************************************************************** ! * An improved Mellor-Yamada turbulence closure model * ! * * ! * Aug/2005 M. Nakanishi (N.D.A) * ! * Modified: Dec/2005 M. Nakanishi (N.D.A) * ! * naka@nda.ac.jp * ! * * ! * Contents: * ! * 1. mym_initialize (to be called once initially) * ! * gives the closure constants and initializes the turbulent * ! * quantities. * ! * (2) mym_level2 (called in the other subroutines) * ! * calculates the stability functions at Level 2. * ! * (3) mym_length (called in the other subroutines) * ! * calculates the master length scale. * ! * 4. mym_turbulence * ! * calculates the vertical diffusivity coefficients and the * ! * production terms for the turbulent quantities. * ! * 5. mym_predict * ! * predicts the turbulent quantities at the next step. * ! * 6. mym_condensation * ! * determines the liquid water content and the cloud fraction * ! * diagnostically. * ! * * ! * call mym_initialize * ! * | * ! * |<----------------+ * ! * | | * ! * call mym_condensation | * ! * call mym_turbulence | * ! * call mym_predict | * ! * | | * ! * |-----------------+ * ! * | * ! * end * ! * * ! * Variables worthy of special mention: * ! * tref : Reference temperature * ! * thl : Liquid water potential temperature * ! * qw : Total water (water vapor+liquid water) content * ! * ql : Liquid water content * ! * vt, vq : Functions for computing the buoyancy flux * ! * * ! * If the water contents are unnecessary, e.g., in the case of * ! * ocean models, thl is the potential temperature and qw, ql, vt * ! * and vq are all zero. * ! * * ! * Grid arrangement: * ! * k+1 +---------+ * ! * | | i = 1 - nx * ! * (k) | * | j = 1 - ny * ! * | | k = 1 - nz * ! * k +---------+ * ! * i (i) i+1 * ! * * ! * All the predicted variables are defined at the center (*) of * ! * the grid boxes. The diffusivity coefficients are, however, * ! * defined on the walls of the grid boxes. * ! * # Upper boundary values are given at k=nz. * ! * * ! * References: * ! * 1. Nakanishi, M., 2001: * ! * Boundary-Layer Meteor., 99, 349-378. * ! * 2. Nakanishi, M. and H. Niino, 2004: * ! * Boundary-Layer Meteor., 112, 1-31. * ! * 3. Nakanishi, M. and H. Niino, 2006: * ! * Boundary-Layer Meteor., (in press). * ! * 4. Nakanishi, M. and H. Niino, 2009: * ! * Jour. Meteor. Soc. Japan, 87, 895-912. * ! ********************************************************************** ! ! SUBROUTINE mym_initialize: ! ! Input variables: ! iniflag : <>0; turbulent quantities will be initialized ! = 0; turbulent quantities have been already ! given, i.e., they will not be initialized ! mx, my : Maximum numbers of grid boxes ! in the x and y directions, respectively ! nx, ny, nz : Numbers of the actual grid boxes ! in the x, y and z directions, respectively ! tref : Reference temperature (K) ! dz(nz) : Vertical grid spacings (m) ! # dz(nz)=dz(nz-1) ! zw(nz+1) : Heights of the walls of the grid boxes (m) ! # zw(1)=0.0 and zw(k)=zw(k-1)+dz(k-1) ! h(mx,ny) : G^(1/2) in the terrain-following coordinate ! # h=1-zg/zt, where zg is the height of the ! terrain and zt the top of the model domain ! pi0(mx,my,nz) : Exner function at zw*h+zg (J/kg K) ! defined by c_p*( p_basic/1000hPa )^kappa ! This is usually computed by integrating ! d(pi0)/dz = -h*g/tref. ! rmo(mx,ny) : Inverse of the Obukhov length (m^(-1)) ! flt, flq(mx,ny) : Turbulent fluxes of sensible and latent heat, ! respectively, e.g., flt=-u_*Theta_* (K m/s) !! flt - liquid water potential temperature surface flux !! flq - total water flux surface flux ! ust(mx,ny) : Friction velocity (m/s) ! pmz(mx,ny) : phi_m-zeta at z1*h+z0, where z1 (=0.5*dz(1)) ! is the first grid point above the surafce, z0 ! the roughness length and zeta=(z1*h+z0)*rmo ! phh(mx,ny) : phi_h at z1*h+z0 ! u, v(mx,my,nz): Components of the horizontal wind (m/s) ! thl(mx,my,nz) : Liquid water potential temperature ! (K) ! qw(mx,my,nz) : Total water content Q_w (kg/kg) ! ! Output variables: ! ql(mx,my,nz) : Liquid water content (kg/kg) ! v?(mx,my,nz) : Functions for computing the buoyancy flux ! qke(mx,my,nz) : Twice the turbulent kinetic energy q^2 ! (m^2/s^2) ! tsq(mx,my,nz) : Variance of Theta_l (K^2) ! qsq(mx,my,nz) : Variance of Q_w ! cov(mx,my,nz) : Covariance of Theta_l and Q_w (K) ! el(mx,my,nz) : Master length scale L (m) ! defined on the walls of the grid boxes ! bsh : no longer used ! via common : Closure constants ! ! Work arrays: see subroutine mym_level2 ! pd?(mx,my,nz) : Half of the production terms at Level 2 ! defined on the walls of the grid boxes ! qkw(mx,my,nz) : q on the walls of the grid boxes (m/s) ! ! # As to dtl, ...gh, see subroutine mym_turbulence. ! !------------------------------------------------------------------- SUBROUTINE mym_initialize ( kts,kte,& 1 & dz, zw, & & u, v, thl, qw, & ! & ust, rmo, pmz, phh, flt, flq,& !JOE-BouLac/PBLH mod & zi,theta,& !JOE-end & ust, rmo, & & Qke, Tsq, Qsq, Cov) ! !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte ! REAL, INTENT(IN) :: ust, rmo, pmz, phh, flt, flq REAL, INTENT(IN) :: ust, rmo REAL, DIMENSION(kts:kte), INTENT(in) :: dz REAL, DIMENSION(kts:kte+1), INTENT(in) :: zw REAL, DIMENSION(kts:kte), INTENT(in) :: u,v,thl,qw REAL, DIMENSION(kts:kte), INTENT(out) :: qke,tsq,qsq,cov REAL, DIMENSION(kts:kte) :: & &ql,el,pdk,pdt,pdq,pdc,dtl,dqw,dtv,& &gm,gh,sm,sh,qkw,vt,vq INTEGER :: k,l,lmax REAL :: phm,vkz,elq,elv,b1l,b2l,pmz=1.,phh=1.,flt=0.,flq=0.,tmpq !JOE-BouLac and PBLH mod REAL :: zi REAL, DIMENSION(kts:kte) :: theta !JOE-end ! ** At first ql, vt and vq are set to zero. ** DO k = kts,kte ql(k) = 0.0 vt(k) = 0.0 vq(k) = 0.0 END DO ! CALL mym_level2 ( kts,kte,& & dz, & & u, v, thl, qw, & & ql, vt, vq, & & dtl, dqw, dtv, gm, gh, sm, sh ) ! ! ** Preliminary setting ** el (kts) = 0.0 qke(kts) = ust**2 * ( b1*pmz )**(2.0/3.0) ! phm = phh*b2 / ( b1*pmz )**(1.0/3.0) tsq(kts) = phm*( flt/ust )**2 qsq(kts) = phm*( flq/ust )**2 cov(kts) = phm*( flt/ust )*( flq/ust ) ! DO k = kts+1,kte vkz = vk*zw(k) el (k) = vkz/( 1.0 + vkz/100.0 ) qke(k) = 0.0 ! tsq(k) = 0.0 qsq(k) = 0.0 cov(k) = 0.0 END DO ! ! ** Initialization with an iterative manner ** ! ** lmax is the iteration count. This is arbitrary. ** lmax = 5 !!kte +3 ! DO l = 1,lmax ! CALL mym_length ( kts,kte,& & dz, zw, & & rmo, flt, flq, & & vt, vq, & & qke, & & dtv, & & el, & !JOE-added for BouLac/PBHL & zi,theta,& !JOE-end & qkw) ! DO k = kts+1,kte elq = el(k)*qkw(k) pdk(k) = elq*( sm(k)*gm (k)+& &sh(k)*gh (k) ) pdt(k) = elq* sh(k)*dtl(k)**2 pdq(k) = elq* sh(k)*dqw(k)**2 pdc(k) = elq* sh(k)*dtl(k)*dqw(k) END DO ! ! ** Strictly, vkz*h(i,j) -> vk*( 0.5*dz(1)*h(i,j)+z0 ) ** vkz = vk*0.5*dz(kts) ! elv = 0.5*( el(kts+1)+el(kts) ) / vkz qke(kts) = ust**2 * ( b1*pmz*elv )**(2.0/3.0) ! phm = phh*b2 / ( b1*pmz/elv**2 )**(1.0/3.0) tsq(kts) = phm*( flt/ust )**2 qsq(kts) = phm*( flq/ust )**2 cov(kts) = phm*( flt/ust )*( flq/ust ) ! DO k = kts+1,kte-1 b1l = b1*0.25*( el(k+1)+el(k) ) tmpq=MAX(b1l*( pdk(k+1)+pdk(k) ),qkemin) ! PRINT *,'tmpqqqqq',tmpq,pdk(k+1),pdk(k) qke(k) = tmpq**(2.0/3.0) ! IF ( qke(k) .LE. 0.0 ) THEN b2l = 0.0 ELSE b2l = b2*( b1l/b1 ) / SQRT( qke(k) ) END IF ! tsq(k) = b2l*( pdt(k+1)+pdt(k) ) qsq(k) = b2l*( pdq(k+1)+pdq(k) ) cov(k) = b2l*( pdc(k+1)+pdc(k) ) END DO ! END DO !! qke(kts)=qke(kts+1) !! tsq(kts)=tsq(kts+1) !! qsq(kts)=qsq(kts+1) !! cov(kts)=cov(kts+1) qke(kte)=qke(kte-1) tsq(kte)=tsq(kte-1) qsq(kte)=qsq(kte-1) cov(kte)=cov(kte-1) ! ! RETURN END SUBROUTINE mym_initialize ! ! ================================================================== ! SUBROUTINE mym_level2: ! ! Input variables: see subroutine mym_initialize ! ! Output variables: ! dtl(mx,my,nz) : Vertical gradient of Theta_l (K/m) ! dqw(mx,my,nz) : Vertical gradient of Q_w ! dtv(mx,my,nz) : Vertical gradient of Theta_V (K/m) ! gm (mx,my,nz) : G_M divided by L^2/q^2 (s^(-2)) ! gh (mx,my,nz) : G_H divided by L^2/q^2 (s^(-2)) ! sm (mx,my,nz) : Stability function for momentum, at Level 2 ! sh (mx,my,nz) : Stability function for heat, at Level 2 ! ! These are defined on the walls of the grid boxes. ! SUBROUTINE mym_level2 (kts,kte,& 2 & dz, & & u, v, thl, qw, & & ql, vt, vq, & & dtl, dqw, dtv, gm, gh, sm, sh ) ! !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte REAL, DIMENSION(kts:kte), INTENT(in) :: dz REAL, DIMENSION(kts:kte), INTENT(in) :: u,v,thl,qw,ql,vt,vq REAL, DIMENSION(kts:kte), INTENT(out) :: & &dtl,dqw,dtv,gm,gh,sm,sh INTEGER :: k REAL :: rfc,f1,f2,rf1,rf2,smc,shc,& &ri1,ri2,ri3,ri4,duz,dtz,dqz,vtt,vqq,dtq,dzk,afk,abk,ri,rf !JOE-Canuto/Kitamura mod REAL :: a2den !JOE-end ! ev = 2.5e6 ! tv0 = 0.61*tref ! tv1 = 1.61*tref ! gtr = 9.81/tref ! rfc = g1/( g1+g2 ) f1 = b1*( g1-c1 ) +3.0*a2*( 1.0 -c2 )*( 1.0-c5 ) & & +2.0*a1*( 3.0-2.0*c2 ) f2 = b1*( g1+g2 ) -3.0*a1*( 1.0 -c2 ) rf1 = b1*( g1-c1 )/f1 rf2 = b1* g1 /f2 smc = a1 /a2* f1/f2 shc = 3.0*a2*( g1+g2 ) ! ri1 = 0.5/smc ri2 = rf1*smc ri3 = 4.0*rf2*smc -2.0*ri2 ri4 = ri2**2 ! DO k = kts+1,kte dzk = 0.5 *( dz(k)+dz(k-1) ) afk = dz(k)/( dz(k)+dz(k-1) ) abk = 1.0 -afk duz = ( u(k)-u(k-1) )**2 +( v(k)-v(k-1) )**2 duz = duz /dzk**2 dtz = ( thl(k)-thl(k-1) )/( dzk ) dqz = ( qw(k)-qw(k-1) )/( dzk ) ! vtt = 1.0 +vt(k)*abk +vt(k-1)*afk vqq = tv0 +vq(k)*abk +vq(k-1)*afk dtq = vtt*dtz +vqq*dqz ! dtl(k) = dtz dqw(k) = dqz dtv(k) = dtq !? dtv(i,j,k) = dtz +tv0*dqz !? : +( ev/pi0(i,j,k)-tv1 ) !? : *( ql(i,j,k)-ql(i,j,k-1) )/( dzk*h(i,j) ) ! gm (k) = duz gh (k) = -dtq*gtr ! ! ** Gradient Richardson number ** ri = -gh(k)/MAX( duz, 1.0e-10 ) !JOE-Canuto/Kitamura mod IF (CKmod .eq. 1) THEN a2den = 1. + MAX(ri,0.0) ELSE a2den = 1. + 0.0 ENDIF rfc = g1/( g1+g2 ) f1 = b1*( g1-c1 ) +3.0*(a2/a2den)*( 1.0 -c2 )*( 1.0-c5 ) & & +2.0*a1*( 3.0-2.0*c2 ) f2 = b1*( g1+g2 ) -3.0*a1*( 1.0 -c2 ) rf1 = b1*( g1-c1 )/f1 rf2 = b1* g1 /f2 smc = a1 /(a2/a2den)* f1/f2 shc = 3.0*(a2/a2den)*( g1+g2 ) ri1 = 0.5/smc ri2 = rf1*smc ri3 = 4.0*rf2*smc -2.0*ri2 ri4 = ri2**2 !JOE-end ! ** Flux Richardson number ** rf = MIN( ri1*( ri+ri2-SQRT(ri**2-ri3*ri+ri4) ), rfc ) ! sh (k) = shc*( rfc-rf )/( 1.0-rf ) sm (k) = smc*( rf1-rf )/( rf2-rf ) * sh(k) END DO ! RETURN END SUBROUTINE mym_level2 ! ================================================================== ! SUBROUTINE mym_length: ! ! Input variables: see subroutine mym_initialize ! ! Output variables: see subroutine mym_initialize ! ! Work arrays: ! elt(mx,ny) : Length scale depending on the PBL depth (m) ! vsc(mx,ny) : Velocity scale q_c (m/s) ! at first, used for computing elt ! SUBROUTINE mym_length ( kts,kte,& 2 & dz, zw, & & rmo, flt, flq, & & vt, vq, & & qke, & & dtv, & & el, & !JOE-added for BouLac ML (PBLH) & zi,theta,& !JOE-end & qkw) !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte REAL, DIMENSION(kts:kte), INTENT(in) :: dz REAL, DIMENSION(kts:kte+1), INTENT(in) :: zw REAL, INTENT(in) :: rmo,flt,flq REAL, DIMENSION(kts:kte), INTENT(IN) :: qke,vt,vq REAL, DIMENSION(kts:kte), INTENT(out) :: qkw, el REAL, DIMENSION(kts:kte), INTENT(in) :: dtv REAL :: elt,vsc !JOE-added for BouLac ML REAL, DIMENSION(kts:kte), INTENT(IN) :: theta REAL, DIMENSION(kts:kte) :: qtke,elBLmin,elBLavg REAL :: wt,zi,zi2,elt0,h1,h2 !THE FOLLOWING LIMITS DO NOT DIRECTLY AFFECT THE ACTUAL PBLH. !THEY ONLY IMPOSE LIMITS ON THE CALCULATION OF THE MIXING LENGTH !SCALES SO THAT THE BOULAC MIXING LENGTH (IN FREE ATMOS) DOES !NOT ENCROACH UPON THE BOUNDARY LAYER MIXING LENGTH (els, elb & elt). REAL, PARAMETER :: minzi = 300. !min mixed-layer height REAL, PARAMETER :: maxdz = 750. !max (half) transition layer depth !=0.3*2500 m PBLH, so the transition !layer stops growing for PBLHs > 2.5 km. REAL, PARAMETER :: mindz = 300. !min (half) transition layer depth !Joe-end INTEGER :: i,j,k REAL :: afk,abk,zwk,dzk,qdz,vflx,bv,elb,els,elf ! tv0 = 0.61*tref ! gtr = 9.81/tref ! !JOE-added to impose limits on the height integration for elt as well ! as the transition layer depth zi2=MAX(zi,minzi) h1=MAX(0.3*zi2,mindz) h1=MIN(h1,maxdz) ! 1/2 transition layer depth h2=h1/2.0 ! 1/4 transition layer depth !Joe-end !JOE-added for BouLac ML qtke(kts)=MAX(qke(kts)/2.,0.01) !JOE-end DO k = kts+1,kte afk = dz(k)/( dz(k)+dz(k-1) ) abk = 1.0 -afk qkw(k) = SQRT(MAX(qke(k)*abk+qke(k-1)*& &afk,1.0e-10)) !JOE- BouLac Start qtke(k) = MAX(qke(k)/2.,0.001) !JOE- BouLac End END DO ! elt = 1.0e-5 vsc = 1.0e-5 ! ! ** Strictly, zwk*h(i,j) -> ( zwk*h(i,j)+z0 ) ** !JOE-Lt mod: only integrate to top of PBL (+ transition/entrainment ! layer), since TKE aloft is not relevant. Make WHILE loop, so it ! exits after looping through the boundary layer. ! k = kts+1 zwk = zw(k) DO WHILE (zwk .LE. (zi2+h1)) dzk = 0.5*( dz(k)+dz(k-1) ) qdz = MAX( qkw(k)-qmin, 0.02 )*dzk elt = elt +qdz*zwk vsc = vsc +qdz k = k+1 zwk = zw(k) END DO ! elt = alp1*elt/vsc vflx = ( vt(kts)+1.0 )*flt +( vq(kts)+tv0 )*flq vsc = ( gtr*elt*MAX( vflx, 0.0 ) )**(1.0/3.0) ! ! ** Strictly, el(i,j,1) is not zero. ** el(kts) = 0.0 ! !JOE- BouLac Start IF ( BLmod .GT. 0. ) THEN ! COMPUTE BouLac mixing length CALL boulac_length(kts,kte,zw,dz,qtke,theta,elBLmin,elBLavg) ENDIF !JOE- BouLac END DO k = kts+1,kte zwk = zw(k) !JOE- BouLac Start - add blending to only use elt in the boundary ! layer and use the BouLac mixing length in free atmos ! [defined relative to the PBLH (zi) + transition layer (h1)]. IF ( BLmod .GT. 0. ) THEN wt=.5*TANH((zwk - (zi2+h1))/h2) + .5 elt0=elt*(1.-wt) + elBLavg(k)*wt ELSE elt0=elt ENDIF !JOE- BouLac END ! ** Length scale limited by the buoyancy effect ** IF ( dtv(k) .GT. 0.0 ) THEN bv = SQRT( gtr*dtv(k) ) elb = alp2*qkw(k) / bv & & *( 1.0 + alp3/alp2*& &SQRT( vsc/( bv*elt ) ) ) elf = alp2 * qkw(k)/bv ELSE elb = 1.0e10 elf = elb END IF ! !JOE- BouLac Start - only use BL ML in free atmos. IF ( BLmod .GT. 0. ) THEN wt=.5*TANH((zwk - (zi2+h1))/h2) + .5 elb=elb*(1.-wt) + elBLmin(k)*wt !TEST: turn off mixing aloft !elb=elb*(1.-wt) + 0.01*wt ENDIF !!JOE- BouLac END ! ** Length scale in the surface layer ** IF ( rmo .GT. 0.0 ) THEN els = vk*zwk & & /( 1.0 + cns*MIN( zwk*rmo, zmax ) ) ELSE els = vk*zwk & & *( 1.0 - alp4* zwk*rmo )**0.2 END IF ! !JOE- BouLac Start ! el(k) = MIN(elb/( elb/elt+elb/els+1.0 ),elf) el(k) = MIN(elb/( elb/elt0+elb/els+1.0 ),elf) ! el(k) = elb/( elb/elt+elb/els+1.0 ) !JOE- BouLac End END DO ! RETURN END SUBROUTINE mym_length !JOE- BouLac Code Start - ! ================================================================== SUBROUTINE boulac_length(kts,kte,zw,dz,qtke,theta,lb1,lb2) 1,10 ! ! NOTE: This subroutine was taken from the BouLac scheme in WRF-ARW ! and modified for integration into the MYNN PBL scheme. ! WHILE loops were added to reduce the computational expense. ! This subroutine computes the length scales up and down ! and then computes the min, average of the up/down ! length scales, and also considers the distance to the ! surface. ! ! dlu = the distance a parcel can be lifted upwards give a finite ! amount of TKE. ! dld = the distance a parcel can be displaced downwards given a ! finite amount of TKE. ! lb1 = the minimum of the length up and length down ! lb2 = the average of the length up and length down !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte REAL, DIMENSION(kts:kte), INTENT(IN) :: qtke,dz,theta REAL, DIMENSION(kts:kte), INTENT(OUT) :: lb1,lb2 REAL, DIMENSION(kts:kte+1), INTENT(IN) :: zw !LOCAL VARS INTEGER :: iz, izz, found REAL, DIMENSION(kts:kte) :: dlu,dld !REAL, PARAMETER :: g=9.81 REAL :: dzt, zup, beta, zup_inf, bbb, tl, zdo, zdo_sup, zzz !print*,"IN MYNN-BouLac",kts, kte do iz=kts,kte !---------------------------------- ! FIND DISTANCE UPWARD !---------------------------------- zup=0. dlu(iz)=zw(kte+1)-zw(iz)-dz(iz)/2. zzz=0. zup_inf=0. beta=g/theta(iz) !Buoyancy coefficient if (iz .lt. kte) then !cant integrate upwards from highest level !do izz=iz,kte-1 !integrate upwards to find dlu found = 0 izz=iz DO WHILE (found .EQ. 0) if (izz .lt. kte) then dzt=(dz(izz+1)+dz(izz))/2. ! avg layer depth of above and below layer zup=zup-beta*theta(iz)*dzt ! initial PE the parcel has at iz !print*," ",iz,izz,theta(izz) zup=zup+beta*(theta(izz+1)+theta(izz))*dzt/2. ! PE gained by lifting a parcel to izz+1 zzz=zzz+dzt ! depth of layer iz to izz+1 if (qtke(iz).lt.zup .and. qtke(iz).ge.zup_inf) then bbb=(theta(izz+1)-theta(izz))/dzt if (bbb .ne. 0.) then tl=(-beta*(theta(izz)-theta(iz)) + & & sqrt( max(0.,(beta*(theta(izz)-theta(iz)))**2. + & & 2.*bbb*beta*(qtke(iz)-zup_inf))))/bbb/beta else if (theta(izz) .ne. theta(iz))then tl=(qtke(iz)-zup_inf)/(beta*(theta(izz)-theta(iz))) else tl=0. endif endif dlu(iz)=zzz-dzt+tl found = 1 endif zup_inf=zup izz=izz+1 ELSE found = 1 ENDIF ENDDO endif !---------------------------------- ! FIND DISTANCE DOWN !---------------------------------- zdo=0. zdo_sup=0. dld(iz)=zw(iz)+dz(iz)/2. zzz=0. if (iz .gt. kts) then !cant integrate downwards from lowest level !do izz=iz,kts+1,-1 !integrate downwards to find dld found = 0 izz=iz DO WHILE (found .EQ. 0) if (izz .gt. kts) then dzt=(dz(izz-1)+dz(izz))/2. zdo=zdo+beta*theta(iz)*dzt zdo=zdo-beta*(theta(izz-1)+theta(izz))*dzt/2. zzz=zzz+dzt if (qtke(iz).lt.zdo .and. qtke(iz).ge.zdo_sup) then bbb=(theta(izz)-theta(izz-1))/dzt if (bbb .ne. 0.) then tl=(beta*(theta(izz)-theta(iz))+ & & sqrt( max(0.,(beta*(theta(izz)-theta(iz)))**2. + & & 2.*bbb*beta*(qtke(iz)-zdo_sup))))/bbb/beta else if (theta(izz) .ne. theta(iz)) then tl=(qtke(iz)-zdo_sup)/(beta*(theta(izz)-theta(iz))) else tl=0. endif endif dld(iz)=zzz-dzt+tl found = 1 endif zdo_sup=zdo izz=izz-1 ELSE found = 1 ENDIF ENDDO endif !---------------------------------- ! GET MINIMUM (OR AVERAGE) !---------------------------------- !The surface layer length scale can exceed z for large z/L, !so keep maximum distance down > z. dld(iz) = min(dld(iz),zw(iz+1)) lb1(iz) = min(dlu(iz),dld(iz)) !minimum lb2(iz) = sqrt(dlu(iz)*dld(iz)) !average - biased towards smallest !lb2(iz) = 0.5*(dlu(iz)+dld(iz)) !average if (iz .eq. kte) then lb1(kte) = lb1(kte-1) lb2(kte) = lb2(kte-1) endif !print*,"IN MYNN-BouLac",kts, kte,lb1(iz) !print*,"IN MYNN-BouLac",iz,dld(iz),dlu(iz) ENDDO END SUBROUTINE boulac_length ! !JOE-END BOULAC CODE ! ================================================================== ! SUBROUTINE mym_turbulence: ! ! Input variables: see subroutine mym_initialize ! levflag : <>3; Level 2.5 ! = 3; Level 3 ! ! # ql, vt, vq, qke, tsq, qsq and cov are changed to input variables. ! ! Output variables: see subroutine mym_initialize ! dfm(mx,my,nz) : Diffusivity coefficient for momentum, ! divided by dz (not dz*h(i,j)) (m/s) ! dfh(mx,my,nz) : Diffusivity coefficient for heat, ! divided by dz (not dz*h(i,j)) (m/s) ! dfq(mx,my,nz) : Diffusivity coefficient for q^2, ! divided by dz (not dz*h(i,j)) (m/s) ! tcd(mx,my,nz) : Countergradient diffusion term for Theta_l ! (K/s) ! qcd(mx,my,nz) : Countergradient diffusion term for Q_w ! (kg/kg s) ! pd?(mx,my,nz) : Half of the production terms ! ! Only tcd and qcd are defined at the center of the grid boxes ! ! # DO NOT forget that tcd and qcd are added on the right-hand side ! of the equations for Theta_l and Q_w, respectively. ! ! Work arrays: see subroutine mym_initialize and level2 ! ! # dtl, dqw, dtv, gm and gh are allowed to share storage units with ! dfm, dfh, dfq, tcd and qcd, respectively, for saving memory. ! SUBROUTINE mym_turbulence ( kts,kte,& 1 & levflag, & & dz, zw, & & u, v, thl, ql, qw, & & qke, tsq, qsq, cov, & & vt, vq,& & rmo, flt, flq, & !JOE-BouLac/PBLH test & zi,theta,& !JOE-end & El,& & Dfm, Dfh, Dfq, Tcd, Qcd, Pdk, Pdt, Pdq, Pdc & !JOE-TKE BUDGET & ,qWT1D,qSHEAR1D,qBUOY1D,qDISS1D, & & bl_mynn_tkebudget & !JOE-end &) !------------------------------------------------------------------- ! INTEGER, INTENT(IN) :: kts,kte INTEGER, INTENT(IN) :: levflag REAL, DIMENSION(kts:kte), INTENT(in) :: dz REAL, DIMENSION(kts:kte+1), INTENT(in) :: zw REAL, INTENT(in) :: rmo,flt,flq REAL, DIMENSION(kts:kte), INTENT(in) :: u,v,thl,qw,& &ql,vt,vq,qke,tsq,qsq,cov REAL, DIMENSION(kts:kte), INTENT(out) :: dfm,dfh,dfq,& &pdk,pdt,pdq,pdc,tcd,qcd,el !JOE-TKE BUDGET REAL, DIMENSION(kts:kte), INTENT(inout) :: & qWT1D,qSHEAR1D,qBUOY1D,qDISS1D REAL :: q3sq_old,dlsq1,qWTP_old,qWTP_new REAL :: dudz,dvdz,dTdz,& upwp,vpwp,Tpwp INTEGER, INTENT(in) :: bl_mynn_tkebudget !JOE-end REAL, DIMENSION(kts:kte) :: qkw,dtl,dqw,dtv,gm,gh,sm,sh INTEGER :: k ! REAL :: cc2,cc3,e1c,e2c,e3c,e4c,e5c REAL :: e6c,dzk,afk,abk,vtt,vqq,& &cw25,clow,cupp,gamt,gamq,smd,gamv,elq,elh !JOE-added for BouLac/PBLH test REAL :: zi REAL, DIMENSION(kts:kte), INTENT(in) :: theta !JOE-end !JOE-Canuto/Kitamura mod REAL :: a2den, duz, ri !JOE-end DOUBLE PRECISION q2sq, t2sq, r2sq, c2sq, elsq, gmel, ghel DOUBLE PRECISION q3sq, t3sq, r3sq, c3sq, dlsq, qdiv DOUBLE PRECISION e1, e2, e3, e4, enum, eden, wden ! ! tv0 = 0.61*tref ! gtr = 9.81/tref ! ! cc2 = 1.0-c2 ! cc3 = 1.0-c3 ! e1c = 3.0*a2*b2*cc3 ! e2c = 9.0*a1*a2*cc2 ! e3c = 9.0*a2*a2*cc2*( 1.0-c5 ) ! e4c = 12.0*a1*a2*cc2 ! e5c = 6.0*a1*a1 ! CALL mym_level2 (kts,kte,& & dz, & & u, v, thl, qw, & & ql, vt, vq, & & dtl, dqw, dtv, gm, gh, sm, sh ) ! CALL mym_length (kts,kte, & & dz, zw, & & rmo, flt, flq, & & vt, vq, & & qke, & & dtv, & & el, & !JOE BouLac/PBLH test & zi,theta,& !JOE-end & qkw) ! DO k = kts+1,kte dzk = 0.5 *( dz(k)+dz(k-1) ) afk = dz(k)/( dz(k)+dz(k-1) ) abk = 1.0 -afk elsq = el (k)**2 q2sq = b1*elsq*( sm(k)*gm(k)+sh(k)*gh(k) ) q3sq = qkw(k)**2 !JOE-Canuto/Kitamura mod duz = ( u(k)-u(k-1) )**2 +( v(k)-v(k-1) )**2 duz = duz /dzk**2 ! ** Gradient Richardson number ** ri = -gh(k)/MAX( duz, 1.0e-10 ) IF (CKmod .eq. 1) THEN a2den = 1. + MAX(ri,0.0) ELSE a2den = 1. + 0.0 ENDIF !JOE-end ! ! Modified: Dec/22/2005, from here, (dlsq -> elsq) gmel = gm (k)*elsq ghel = gh (k)*elsq ! Modified: Dec/22/2005, up to here ! ! ** Since qkw is set to more than 0.0, q3sq > 0.0. ** IF ( q3sq .LT. q2sq ) THEN qdiv = SQRT( q3sq/q2sq ) sm(k) = sm(k) * qdiv sh(k) = sh(k) * qdiv ! !JOE-Canuto/Kitamura mod ! e1 = q3sq - e1c*ghel * qdiv**2 ! e2 = q3sq - e2c*ghel * qdiv**2 ! e3 = e1 + e3c*ghel * qdiv**2 ! e4 = e1 - e4c*ghel * qdiv**2 e1 = q3sq - e1c*ghel/a2den * qdiv**2 e2 = q3sq - e2c*ghel/a2den * qdiv**2 e3 = e1 + e3c*ghel/(a2den**2) * qdiv**2 e4 = e1 - e4c*ghel/a2den * qdiv**2 !JOE-end eden = e2*e4 + e3*e5c*gmel * qdiv**2 eden = MAX( eden, 1.0d-20 ) ELSE !JOE-Canuto/Kitamura mod ! e1 = q3sq - e1c*ghel ! e2 = q3sq - e2c*ghel ! e3 = e1 + e3c*ghel ! e4 = e1 - e4c*ghel e1 = q3sq - e1c*ghel/a2den e2 = q3sq - e2c*ghel/a2den e3 = e1 + e3c*ghel/(a2den**2) e4 = e1 - e4c*ghel/a2den !JOE-end eden = e2*e4 + e3*e5c*gmel eden = MAX( eden, 1.0d-20 ) ! qdiv = 1.0 sm(k) = q3sq*a1*( e3-3.0*c1*e4 )/eden !JOE-Canuto/Kitamura mod ! sh(k) = q3sq*a2*( e2+3.0*c1*e5c*gmel )/eden sh(k) = q3sq*(a2/a2den)*( e2+3.0*c1*e5c*gmel )/eden !JOE-end END IF ! ! ** Level 3 : start ** IF ( levflag .EQ. 3 ) THEN t2sq = qdiv*b2*elsq*sh(k)*dtl(k)**2 r2sq = qdiv*b2*elsq*sh(k)*dqw(k)**2 c2sq = qdiv*b2*elsq*sh(k)*dtl(k)*dqw(k) t3sq = MAX( tsq(k)*abk+tsq(k-1)*afk, 0.0 ) r3sq = MAX( qsq(k)*abk+qsq(k-1)*afk, 0.0 ) c3sq = cov(k)*abk+cov(k-1)*afk ! ! Modified: Dec/22/2005, from here c3sq = SIGN( MIN( ABS(c3sq), SQRT(t3sq*r3sq) ), c3sq ) ! vtt = 1.0 +vt(k)*abk +vt(k-1)*afk vqq = tv0 +vq(k)*abk +vq(k-1)*afk t2sq = vtt*t2sq +vqq*c2sq r2sq = vtt*c2sq +vqq*r2sq c2sq = MAX( vtt*t2sq+vqq*r2sq, 0.0d0 ) t3sq = vtt*t3sq +vqq*c3sq r3sq = vtt*c3sq +vqq*r3sq c3sq = MAX( vtt*t3sq+vqq*r3sq, 0.0d0 ) ! cw25 = e1*( e2 + 3.0*c1*e5c*gmel*qdiv**2 )/( 3.0*eden ) ! ! ** Limitation on q, instead of L/q ** dlsq = elsq IF ( q3sq/dlsq .LT. -gh(k) ) q3sq = -dlsq*gh(k) ! ! ** Limitation on c3sq (0.12 =< cw =< 0.76) ** !JOE-Canuto/Kitamura mod ! e2 = q3sq - e2c*ghel * qdiv**2 ! e3 = q3sq + e3c*ghel * qdiv**2 ! e4 = q3sq - e4c*ghel * qdiv**2 e2 = q3sq - e2c*ghel/a2den * qdiv**2 e3 = q3sq + e3c*ghel/(a2den**2) * qdiv**2 e4 = q3sq - e4c*ghel/a2den * qdiv**2 !JOE-end eden = e2*e4 + e3 *e5c*gmel * qdiv**2 ! !JOE-Canuto/Kitamura mod ! wden = cc3*gtr**2 * dlsq**2/elsq * qdiv**2 & ! & *( e2*e4c - e3c*e5c*gmel * qdiv**2 ) wden = cc3*gtr**2 * dlsq**2/elsq * qdiv**2 & & *( e2*e4c/a2den - e3c*e5c*gmel/(a2den**2) * qdiv**2 ) !JOE-end ! IF ( wden .NE. 0.0 ) THEN clow = q3sq*( 0.12-cw25 )*eden/wden cupp = q3sq*( 0.76-cw25 )*eden/wden ! IF ( wden .GT. 0.0 ) THEN c3sq = MIN( MAX( c3sq, c2sq+clow ), c2sq+cupp ) ELSE c3sq = MAX( MIN( c3sq, c2sq+clow ), c2sq+cupp ) END IF END IF ! e1 = e2 + e5c*gmel * qdiv**2 eden = MAX( eden, 1.0d-20 ) ! Modified: Dec/22/2005, up to here ! !JOE-Canuto/Kitamura mod ! e6c = 3.0*a2*cc3*gtr * dlsq/elsq e6c = 3.0*(a2/a2den)*cc3*gtr * dlsq/elsq !JOE-end ! ! ** for Gamma_theta ** !! enum = qdiv*e6c*( t3sq-t2sq ) IF ( t2sq .GE. 0.0 ) THEN enum = MAX( qdiv*e6c*( t3sq-t2sq ), 0.0d0 ) ELSE enum = MIN( qdiv*e6c*( t3sq-t2sq ), 0.0d0 ) ENDIF gamt =-e1 *enum /eden ! ! ** for Gamma_q ** !! enum = qdiv*e6c*( r3sq-r2sq ) IF ( r2sq .GE. 0.0 ) THEN enum = MAX( qdiv*e6c*( r3sq-r2sq ), 0.0d0 ) ELSE enum = MIN( qdiv*e6c*( r3sq-r2sq ), 0.0d0 ) ENDIF gamq =-e1 *enum /eden ! ! ** for Sm' and Sh'd(Theta_V)/dz ** !! enum = qdiv*e6c*( c3sq-c2sq ) enum = MAX( qdiv*e6c*( c3sq-c2sq ), 0.0d0) !JOE-Canuto/Kitamura mod ! smd = dlsq*enum*gtr/eden * qdiv**2 * (e3c+e4c)*a1/a2 smd = dlsq*enum*gtr/eden * qdiv**2 * (e3c/(a2den**2) + e4c/a2den)*a1/(a2/a2den) !JOE-end gamv = e1 *enum*gtr/eden ! sm(k) = sm(k) +smd ! ! ** For elh (see below), qdiv at Level 3 is reset to 1.0. ** qdiv = 1.0 ! ** Level 3 : end ** ! ELSE ! ** At Level 2.5, qdiv is not reset. ** gamt = 0.0 gamq = 0.0 gamv = 0.0 END IF ! elq = el(k)*qkw(k) elh = elq*qdiv ! pdk(k) = elq*( sm(k)*gm (k) & & +sh(k)*gh (k)+gamv ) pdt(k) = elh*( sh(k)*dtl(k)+gamt )*dtl(k) pdq(k) = elh*( sh(k)*dqw(k)+gamq )*dqw(k) pdc(k) = elh*( sh(k)*dtl(k)+gamt )& &*dqw(k)*0.5 & &+elh*( sh(k)*dqw(k)+gamq )*dtl(k)*0.5 ! tcd(k) = elq*gamt qcd(k) = elq*gamq ! dfm(k) = elq*sm (k) / dzk dfh(k) = elq*sh (k) / dzk ! Modified: Dec/22/2005, from here ! ** In sub.mym_predict, dfq for the TKE and scalar variance ** ! ** are set to 3.0*dfm and 1.0*dfm, respectively. (Sqfac) ** dfq(k) = dfm(k) ! Modified: Dec/22/2005, up to here IF ( bl_mynn_tkebudget == 1) THEN !TKE BUDGET dudz = ( u(k)-u(k-1) )/dzk dvdz = ( v(k)-v(k-1) )/dzk dTdz = ( thl(k)-thl(k-1) )/dzk upwp = -elq*sm(k)*dudz vpwp = -elq*sm(k)*dvdz Tpwp = -elq*sh(k)*dTdz Tpwp = SIGN(MAX(ABS(Tpwp),1.E-6),Tpwp) IF ( k .EQ. kts+1 ) THEN qWT1D(kts)=0. q3sq_old =0. qWTP_old =0. !** Limitation on q, instead of L/q ** dlsq1 = MAX(el(kts)**2,1.0) IF ( q3sq_old/dlsq1 .LT. -gh(k) ) q3sq_old = -dlsq1*gh(k) ENDIF !!!Vertical Transport Term qWTP_new = elq*Sqfac*sm(k)*(q3sq - q3sq_old)/dzk qWT1D(k) = 0.5*(qWTP_new - qWTP_old)/dzk qWTP_old = elq*Sqfac*sm(k)*(q3sq - q3sq_old)/dzk q3sq_old = q3sq !!!Shear Term !!!qSHEAR1D(k)=-(upwp*dudz + vpwp*dvdz) qSHEAR1D(k) = elq*sm(k)*gm(k) !!!Buoyancy Term !!!qBUOY1D(k)=g*Tpwp/thl(k) !qBUOY1D(k)= elq*(sh(k)*gh(k) + gamv) qBUOY1D(k) = elq*(sh(k)*(-dTdz*g/thl(k)) + gamv) !!!Dissipation Term qDISS1D(k) = (q3sq**(3./2.))/(b1*MAX(el(k),1.)) ENDIF END DO ! dfm(kts) = 0.0 dfh(kts) = 0.0 dfq(kts) = 0.0 tcd(kts) = 0.0 qcd(kts) = 0.0 tcd(kte) = 0.0 qcd(kte) = 0.0 ! DO k = kts,kte-1 dzk = dz(k) tcd(k) = ( tcd(k+1)-tcd(k) )/( dzk ) qcd(k) = ( qcd(k+1)-qcd(k) )/( dzk ) END DO ! IF ( bl_mynn_tkebudget == 1) THEN !JOE-TKE BUDGET qWT1D(kts)=0. qSHEAR1D(kts)=qSHEAR1D(kts+1) qBUOY1D(kts)=qBUOY1D(kts+1) qDISS1D(kts)=qDISS1D(kts+1) ENDIF RETURN END SUBROUTINE mym_turbulence ! ================================================================== ! SUBROUTINE mym_predict: ! ! Input variables: see subroutine mym_initialize and turbulence ! qke(mx,my,nz) : qke at (n)th time level ! tsq, ...cov : ditto ! ! Output variables: ! qke(mx,my,nz) : qke at (n+1)th time level ! tsq, ...cov : ditto ! ! Work arrays: ! qkw(mx,my,nz) : q at the center of the grid boxes (m/s) ! bp (mx,my,nz) : = 1/2*F, see below ! rp (mx,my,nz) : = P-1/2*F*Q, see below ! ! # The equation for a turbulent quantity Q can be expressed as ! dQ/dt + Ah + Av = Dh + Dv + P - F*Q, (1) ! where A is the advection, D the diffusion, P the production, ! F*Q the dissipation and h and v denote horizontal and vertical, ! respectively. If Q is q^2, F is 2q/B_1L. ! Using the Crank-Nicholson scheme for Av, Dv and F*Q, a finite ! difference equation is written as ! Q{n+1} - Q{n} = dt *( Dh{n} - Ah{n} + P{n} ) ! + dt/2*( Dv{n} - Av{n} - F*Q{n} ) ! + dt/2*( Dv{n+1} - Av{n+1} - F*Q{n+1} ), (2) ! where n denotes the time level. ! When the advection and diffusion terms are discretized as ! dt/2*( Dv - Av ) = a(k)Q(k+1) - b(k)Q(k) + c(k)Q(k-1), (3) ! Eq.(2) can be rewritten as ! - a(k)Q(k+1) + [ 1 + b(k) + dt/2*F ]Q(k) - c(k)Q(k-1) ! = Q{n} + dt *( Dh{n} - Ah{n} + P{n} ) ! + dt/2*( Dv{n} - Av{n} - F*Q{n} ), (4) ! where Q on the left-hand side is at (n+1)th time level. ! ! In this subroutine, a(k), b(k) and c(k) are obtained from ! subprogram coefvu and are passed to subprogram tinteg via ! common. 1/2*F and P-1/2*F*Q are stored in bp and rp, ! respectively. Subprogram tinteg solves Eq.(4). ! ! Modify this subroutine according to your numerical integration ! scheme (program). ! !------------------------------------------------------------------- SUBROUTINE mym_predict (kts,kte,& 1 & levflag, & & delt,& & dz, & & ust, flt, flq, pmz, phh, & & el, dfq, & & pdk, pdt, pdq, pdc,& & qke, tsq, qsq, cov & &) !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte INTEGER, INTENT(IN) :: levflag REAL, INTENT(IN) :: delt REAL, DIMENSION(kts:kte), INTENT(IN) :: dz, dfq,el REAL, DIMENSION(kts:kte), INTENT(INOUT) :: pdk, pdt, pdq, pdc REAL, INTENT(IN) :: flt, flq, ust, pmz, phh REAL, DIMENSION(kts:kte), INTENT(INOUT) :: qke,tsq, qsq, cov INTEGER :: k,nz REAL, DIMENSION(kts:kte) :: qkw, bp, rp, df3q REAL :: vkz,pdk1,phm,pdt1,pdq1,pdc1,b1l,b2l REAL, DIMENSION(kts:kte) :: dtz REAL, DIMENSION(1:kte-kts+1) :: a,b,c,d nz=kte-kts+1 ! ** Strictly, vkz*h(i,j) -> vk*( 0.5*dz(1)*h(i,j)+z0 ) ** vkz = vk*0.5*dz(kts) ! ! Modified: Dec/22/2005, from here ! ** dfq for the TKE is 3.0*dfm. ** ! CALL coefvu ( dfq, 3.0 ) ! make change here ! Modified: Dec/22/2005, up to here ! DO k = kts,kte !! qke(k) = MAX(qke(k), 0.0) qkw(k) = SQRT( MAX( qke(k), 0.0 ) ) !df3q(k)=3.*dfq(k) df3q(k)=Sqfac*dfq(k) dtz(k)=delt/dz(k) END DO ! pdk1 = 2.0*ust**3*pmz/( vkz ) phm = 2.0/ust *phh/( vkz ) pdt1 = phm*flt**2 pdq1 = phm*flq**2 pdc1 = phm*flt*flq ! ! ** pdk(i,j,1)+pdk(i,j,2) corresponds to pdk1. ** pdk(kts) = pdk1 -pdk(kts+1) !! pdt(kts) = pdt1 -pdt(kts+1) !! pdq(kts) = pdq1 -pdq(kts+1) !! pdc(kts) = pdc1 -pdc(kts+1) pdt(kts) = pdt(kts+1) pdq(kts) = pdq(kts+1) pdc(kts) = pdc(kts+1) ! ! ** Prediction of twice the turbulent kinetic energy ** !! DO k = kts+1,kte-1 DO k = kts,kte-1 b1l = b1*0.5*( el(k+1)+el(k) ) bp(k) = 2.*qkw(k) / b1l rp(k) = pdk(k+1) + pdk(k) END DO !! a(1)=0. !! b(1)=1. !! c(1)=-1. !! d(1)=0. ! Since df3q(kts)=0.0, a(1)=0.0 and b(1)=1.+dtz(k)*df3q(k+1)+bp(k)*delt. DO k=kts,kte-1 a(k-kts+1)=-dtz(k)*df3q(k) b(k-kts+1)=1.+dtz(k)*(df3q(k)+df3q(k+1))+bp(k)*delt c(k-kts+1)=-dtz(k)*df3q(k+1) d(k-kts+1)=rp(k)*delt + qke(k) ENDDO !! DO k=kts+1,kte-1 !! a(k-kts+1)=-dtz(k)*df3q(k) !! b(k-kts+1)=1.+dtz(k)*(df3q(k)+df3q(k+1)) !! c(k-kts+1)=-dtz(k)*df3q(k+1) !! d(k-kts+1)=rp(k)*delt + qke(k) - qke(k)*bp(k)*delt !! ENDDO a(nz)=-1. !0. b(nz)=1. c(nz)=0. d(nz)=0. CALL tridiag(nz,a,b,c,d) DO k=kts,kte qke(k)=d(k-kts+1) ENDDO IF ( levflag .EQ. 3 ) THEN ! ! Modified: Dec/22/2005, from here ! ** dfq for the scalar variance is 1.0*dfm. ** ! CALL coefvu ( dfq, 1.0 ) make change here ! Modified: Dec/22/2005, up to here ! ! ** Prediction of the temperature variance ** !! DO k = kts+1,kte-1 DO k = kts,kte-1 b2l = b2*0.5*( el(k+1)+el(k) ) bp(k) = 2.*qkw(k) / b2l rp(k) = pdt(k+1) + pdt(k) END DO !zero gradient for tsq at bottom and top !! a(1)=0. !! b(1)=1. !! c(1)=-1. !! d(1)=0. ! Since dfq(kts)=0.0, a(1)=0.0 and b(1)=1.+dtz(k)*dfq(k+1)+bp(k)*delt. DO k=kts,kte-1 a(k-kts+1)=-dtz(k)*dfq(k) b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1))+bp(k)*delt c(k-kts+1)=-dtz(k)*dfq(k+1) d(k-kts+1)=rp(k)*delt + tsq(k) ENDDO !! DO k=kts+1,kte-1 !! a(k-kts+1)=-dtz(k)*dfq(k) !! b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1)) !! c(k-kts+1)=-dtz(k)*dfq(k+1) !! d(k-kts+1)=rp(k)*delt + tsq(k) - tsq(k)*bp(k)*delt !! ENDDO a(nz)=-1. !0. b(nz)=1. c(nz)=0. d(nz)=0. CALL tridiag(nz,a,b,c,d) DO k=kts,kte tsq(k)=d(k-kts+1) ENDDO ! ** Prediction of the moisture variance ** !! DO k = kts+1,kte-1 DO k = kts,kte-1 b2l = b2*0.5*( el(k+1)+el(k) ) bp(k) = 2.*qkw(k) / b2l rp(k) = pdq(k+1) +pdq(k) END DO !zero gradient for qsq at bottom and top !! a(1)=0. !! b(1)=1. !! c(1)=-1. !! d(1)=0. ! Since dfq(kts)=0.0, a(1)=0.0 and b(1)=1.+dtz(k)*dfq(k+1)+bp(k)*delt. DO k=kts,kte-1 a(k-kts+1)=-dtz(k)*dfq(k) b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1))+bp(k)*delt c(k-kts+1)=-dtz(k)*dfq(k+1) d(k-kts+1)=rp(k)*delt + qsq(k) ENDDO !! DO k=kts+1,kte-1 !! a(k-kts+1)=-dtz(k)*dfq(k) !! b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1)) !! c(k-kts+1)=-dtz(k)*dfq(k+1) !! d(k-kts+1)=rp(k)*delt + qsq(k) -qsq(k)*bp(k)*delt !! ENDDO a(nz)=-1. !0. b(nz)=1. c(nz)=0. d(nz)=0. CALL tridiag(nz,a,b,c,d) DO k=kts,kte qsq(k)=d(k-kts+1) ENDDO ! ** Prediction of the temperature-moisture covariance ** !! DO k = kts+1,kte-1 DO k = kts,kte-1 b2l = b2*0.5*( el(k+1)+el(k) ) bp(k) = 2.*qkw(k) / b2l rp(k) = pdc(k+1) + pdc(k) END DO !zero gradient for tqcov at bottom and top !! a(1)=0. !! b(1)=1. !! c(1)=-1. !! d(1)=0. ! Since dfq(kts)=0.0, a(1)=0.0 and b(1)=1.+dtz(k)*dfq(k+1)+bp(k)*delt. DO k=kts,kte-1 a(k-kts+1)=-dtz(k)*dfq(k) b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1))+bp(k)*delt c(k-kts+1)=-dtz(k)*dfq(k+1) d(k-kts+1)=rp(k)*delt + cov(k) ENDDO !! DO k=kts+1,kte-1 !! a(k-kts+1)=-dtz(k)*dfq(k) !! b(k-kts+1)=1.+dtz(k)*(dfq(k)+dfq(k+1)) !! c(k-kts+1)=-dtz(k)*dfq(k+1) !! d(k-kts+1)=rp(k)*delt + cov(k) - cov(k)*bp(k)*delt !! ENDDO a(nz)=-1. !0. b(nz)=1. c(nz)=0. d(nz)=0. CALL tridiag(nz,a,b,c,d) DO k=kts,kte cov(k)=d(k-kts+1) ENDDO ELSE !! DO k = kts+1,kte-1 DO k = kts,kte-1 IF ( qkw(k) .LE. 0.0 ) THEN b2l = 0.0 ELSE b2l = b2*0.25*( el(k+1)+el(k) )/qkw(k) END IF ! tsq(k) = b2l*( pdt(k+1)+pdt(k) ) qsq(k) = b2l*( pdq(k+1)+pdq(k) ) cov(k) = b2l*( pdc(k+1)+pdc(k) ) END DO !! tsq(kts)=tsq(kts+1) !! qsq(kts)=qsq(kts+1) !! cov(kts)=cov(kts+1) tsq(kte)=tsq(kte-1) qsq(kte)=qsq(kte-1) cov(kte)=cov(kte-1) END IF END SUBROUTINE mym_predict ! ================================================================== ! SUBROUTINE mym_condensation: ! ! Input variables: see subroutine mym_initialize and turbulence ! pi (mx,my,nz) : Perturbation of the Exner function (J/kg K) ! defined on the walls of the grid boxes ! This is usually computed by integrating ! d(pi)/dz = h*g*tv/tref**2 ! from the upper boundary, where tv is the ! virtual potential temperature minus tref. ! ! Output variables: see subroutine mym_initialize ! cld(mx,my,nz) : Cloud fraction ! ! Work arrays: ! qmq(mx,my,nz) : Q_w-Q_{sl}, where Q_{sl} is the saturation ! specific humidity at T=Tl ! alp(mx,my,nz) : Functions in the condensation process ! bet(mx,my,nz) : ditto ! sgm(mx,my,nz) : Combined standard deviation sigma_s ! multiplied by 2/alp ! ! # qmq, alp, bet and sgm are allowed to share storage units with ! any four of other work arrays for saving memory. ! ! # Results are sensitive particularly to values of cp and rd. ! Set these values to those adopted by you. ! !------------------------------------------------------------------- SUBROUTINE mym_condensation (kts,kte, & 2 & dz, & & thl, qw, & & p,exner, & & tsq, qsq, cov, & & Vt, Vq) !------------------------------------------------------------------- INTEGER, INTENT(IN) :: kts,kte REAL, DIMENSION(kts:kte), INTENT(IN) :: dz REAL, DIMENSION(kts:kte), INTENT(IN) :: p,exner, thl, qw, & &tsq, qsq, cov REAL, DIMENSION(kts:kte), INTENT(OUT) :: vt,vq REAL, DIMENSION(kts:kte) :: qmq,alp,bet,sgm,ql,cld DOUBLE PRECISION :: t3sq, r3sq, c3sq ! REAL :: p2a,t,esl,qsl,dqsl,q1,cld0,eq1,qll,& &q2p,pt,rac,qt INTEGER :: i,j,k REAL :: erf ! Note: kte needs to be larger than kts, i.e., kte >= kts+1. DO k = kts,kte-1 p2a = exner(k) t = thl(k)*p2a !x if ( ct .gt. 0.0 ) then ! a = 17.27 ! b = 237.3 !x else !x a = 21.87 !x b = 265.5 !x end if ! ! ** 3.8 = 0.622*6.11 (hPa) ** esl=svp11*EXP(svp2*(t-svpt0)/(t-svp3)) qsl=ep_2*esl/(p(k)-ep_3*esl) ! qsl = 3.8*EXP( a*ct/( b+ct ) ) / ( 1000.0*p2a**rk ) dqsl = qsl*ep_2*ev/( rd*t**2 ) ! qmq(k) = qw(k) -qsl alp(k) = 1.0/( 1.0+dqsl*xlvcp ) bet(k) = dqsl*p2a ! t3sq = MAX( tsq(k), 0.0 ) r3sq = MAX( qsq(k), 0.0 ) c3sq = cov(k) c3sq = SIGN( MIN( ABS(c3sq), SQRT(t3sq*r3sq) ), c3sq ) ! r3sq = r3sq +bet(k)**2*t3sq -2.0*bet(k)*c3sq sgm(k) = SQRT( MAX( r3sq, 1.0d-10 ) ) END DO ! DO k = kts,kte-1 q1 = qmq(k) / sgm(k) cld0 = 0.5*( 1.0+erf( q1*rr2 ) ) ! q1=0. ! cld0=0. eq1 = rrp*EXP( -0.5*q1*q1 ) qll = MAX( cld0*q1 + eq1, 0.0 ) cld(k) = cld0 ql (k) = alp(k)*sgm(k)*qll ! q2p = xlvcp/exner( k ) pt = thl(k) +q2p*ql(k) qt = 1.0 +p608*qw(k) -(1.+p608)*ql(k) rac = alp(k)*( cld0-qll*eq1 )*( q2p*qt-(1.+p608)*pt ) ! vt (k) = qt-1.0 -rac*bet(k) vq (k) = p608*pt-tv0 +rac END DO ! cld(kte) = cld(kte-1) ql(kte) = ql(kte-1) vt(kte) = vt(kte-1) vq(kte) = vq(kte-1) RETURN END SUBROUTINE mym_condensation ! ================================================================== SUBROUTINE mynn_tendencies(kts,kte,& 1,6 &levflag,grav_settling,& &delt,& &dz,& &u,v,th,qv,qc,p,exner,& &thl,sqv,sqc,sqw,& &ust,flt,flq,wspd,qcg,& &tsq,qsq,cov,& &tcd,qcd,& &dfm,dfh,dfq,& &Du,Dv,Dth,Dqv,Dqc) !------------------------------------------------------------------- INTEGER, INTENT(in) :: kts,kte INTEGER, INTENT(in) :: grav_settling,levflag !! grav_settling = 1 for gravitational settling of droplets !! grav_settling = 0 otherwise ! thl - liquid water potential temperature ! qw - total water ! dfm,dfh,dfq - as above ! flt - surface flux of thl ! flq - surface flux of qw REAL, DIMENSION(kts:kte), INTENT(in) :: u,v,th,qv,qc,p,exner,& &dfm,dfh,dfq,dz,tsq,qsq,cov,tcd,qcd REAL, DIMENSION(kts:kte), INTENT(inout) :: thl,sqw,sqv,sqc REAL, DIMENSION(kts:kte), INTENT(out) :: du,dv,dth,dqv,dqc REAL, INTENT(IN) :: delt,ust,flt,flq,wspd,qcg ! REAL, INTENT(IN) :: delt,ust,flt,flq,qcg,& ! &gradu_top,gradv_top,gradth_top,gradqv_top !local vars REAL, DIMENSION(kts:kte) :: dtz,vt,vq REAL, DIMENSION(1:kte-kts+1) :: a,b,c,d REAL :: rhs,gfluxm,gfluxp,dztop INTEGER :: k,kk,nz nz=kte-kts+1 dztop=.5*(dz(kte)+dz(kte-1)) DO k=kts,kte dtz(k)=delt/dz(k) ENDDO !! u k=kts a(1)=0. b(1)=1.+dtz(k)*(dfm(k+1)+ust**2/wspd) c(1)=-dtz(k)*dfm(k+1) d(1)=u(k) !! a(1)=0. !! b(1)=1.+dtz(k)*dfm(k+1) !! c(1)=-dtz(k)*dfm(k+1) !! d(1)=u(k)*(1.-ust**2/wspd*dtz(k)) DO k=kts+1,kte-1 kk=k-kts+1 a(kk)=-dtz(k)*dfm(k) b(kk)=1.+dtz(k)*(dfm(k)+dfm(k+1)) c(kk)=-dtz(k)*dfm(k+1) d(kk)=u(k) ENDDO !! no flux at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=0. !! specified gradient at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=gradu_top*dztop !! prescribed value a(nz)=0 b(nz)=1. c(nz)=0. d(nz)=u(kte) CALL tridiag(nz,a,b,c,d) DO k=kts,kte du(k)=(d(k-kts+1)-u(k))/delt ENDDO !! v k=kts a(1)=0. b(1)=1.+dtz(k)*(dfm(k+1)+ust**2/wspd) c(1)=-dtz(k)*dfm(k+1) d(1)=v(k) !! a(1)=0. !! b(1)=1.+dtz(k)*dfm(k+1) !! c(1)=-dtz(k)*dfm(k+1) !! d(1)=v(k)*(1.-ust**2/wspd*dtz(k)) DO k=kts+1,kte-1 kk=k-kts+1 a(kk)=-dtz(k)*dfm(k) b(kk)=1.+dtz(k)*(dfm(k)+dfm(k+1)) c(kk)=-dtz(k)*dfm(k+1) d(kk)=v(k) ENDDO !! no flux at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=0. !! specified gradient at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=gradv_top*dztop !! prescribed value a(nz)=0 b(nz)=1. c(nz)=0. d(nz)=v(kte) CALL tridiag(nz,a,b,c,d) DO k=kts,kte dv(k)=(d(k-kts+1)-v(k))/delt ENDDO !! thl k=kts a(1)=0. b(1)=1.+dtz(k)*dfh(k+1) c(1)=-dtz(k)*dfh(k+1) ! if qcg not used then assume constant flux in the surface layer IF (qcg < qcgmin) THEN IF (sqc(k) > qcgmin) THEN gfluxm=grav_settling*gno*sqc(k)**gpw ELSE gfluxm=0. ENDIF ELSE gfluxm=grav_settling*gno*(qcg/(1.+qcg))**gpw ENDIF IF (.5*(sqc(k+1)+sqc(k)) > qcgmin) THEN gfluxp=grav_settling*gno*(.5*(sqc(k+1)+sqc(k)))**gpw ELSE gfluxp=0. ENDIF rhs=-xlvcp/exner(k)& &*( & &(gfluxp - gfluxm)/dz(k)& & ) + tcd(k) d(1)=thl(k)+dtz(k)*flt+rhs*delt DO k=kts+1,kte-1 kk=k-kts+1 a(kk)=-dtz(k)*dfh(k) b(kk)=1.+dtz(k)*(dfh(k)+dfh(k+1)) c(kk)=-dtz(k)*dfh(k+1) IF (.5*(sqc(k+1)+sqc(k)) > qcgmin) THEN gfluxp=grav_settling*gno*(.5*(sqc(k+1)+sqc(k)))**gpw ELSE gfluxp=0. ENDIF IF (.5*(sqc(k-1)+sqc(k)) > qcgmin) THEN gfluxm=grav_settling*gno*(.5*(sqc(k-1)+sqc(k)))**gpw ELSE gfluxm=0. ENDIF rhs=-xlvcp/exner(k)& &*( & &(gfluxp - gfluxm)/dz(k)& & ) + tcd(k) d(kk)=thl(k)+rhs*delt ENDDO !! no flux at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=0. !! specified gradient at the top !assume gradthl_top=gradth_top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=gradth_top*dztop !! prescribed value a(nz)=0. b(nz)=1. c(nz)=0. d(nz)=thl(kte) CALL tridiag(nz,a,b,c,d) DO k=kts,kte thl(k)=d(k-kts+1) ENDDO !! total water k=kts a(1)=0. b(1)=1.+dtz(k)*dfh(k+1) c(1)=-dtz(k)*dfh(k+1) IF (qcg < qcgmin) THEN IF (sqc(k) > qcgmin) THEN gfluxm=grav_settling*gno*sqc(k)**gpw ELSE gfluxm=0. ENDIF ELSE gfluxm=grav_settling*gno*(qcg/(1.+qcg))**gpw ENDIF IF (.5*(sqc(k+1)+sqc(k)) > qcgmin) THEN gfluxp=grav_settling*gno*(.5*(sqc(k+1)+sqc(k)))**gpw ELSE gfluxp=0. ENDIF rhs=& &( & &(gfluxp - gfluxm)/dz(k)& & ) + qcd(k) d(1)=sqw(k)+dtz(k)*flq+rhs*delt DO k=kts+1,kte-1 kk=k-kts+1 a(kk)=-dtz(k)*dfh(k) b(kk)=1.+dtz(k)*(dfh(k)+dfh(k+1)) c(kk)=-dtz(k)*dfh(k+1) IF (.5*(sqc(k+1)+sqc(k)) > qcgmin) THEN gfluxp=grav_settling*gno*(.5*(sqc(k+1)+sqc(k)))**gpw ELSE gfluxp=0. ENDIF IF (.5*(sqc(k-1)+sqc(k)) > qcgmin) THEN gfluxm=grav_settling*gno*(.5*(sqc(k-1)+sqc(k)))**gpw ELSE gfluxm=0. ENDIF rhs=& &( & &(gfluxp - gfluxm)/dz(k)& & ) + qcd(k) d(kk)=sqw(k) + rhs*delt ENDDO !! no flux at the top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=0. !! specified gradient at the top !assume gradqw_top=gradqv_top ! a(nz)=-1. ! b(nz)=1. ! c(nz)=0. ! d(nz)=gradqv_top*dztop !! prescribed value a(nz)=0. b(nz)=1. c(nz)=0. d(nz)=sqw(kte) CALL tridiag(nz,a,b,c,d) !convert to mixing ratios for wrf DO k=kts,kte sqw(k)=d(k-kts+1) sqv(k)=sqw(k)-sqc(k) Dqv(k)=(sqv(k)/(1.-sqv(k))-qv(k))/delt ! Dqc(k)=(sqc(k)/(1.-sqc(k))-qc(k))/delt Dqc(k)=0. Dth(k)=(thl(k)+xlvcp/exner(k)*sqc(k)-th(k))/delt ENDDO END SUBROUTINE mynn_tendencies ! ================================================================== SUBROUTINE retrieve_exchange_coeffs(kts,kte,& 1 &dfm,dfh,dfq,dz,& &K_m,K_h,K_q) !------------------------------------------------------------------- INTEGER , INTENT(in) :: kts,kte REAL, DIMENSION(KtS:KtE), INTENT(in) :: dz,dfm,dfh,dfq REAL, DIMENSION(KtS:KtE), INTENT(out) :: & &K_m, K_h, K_q INTEGER :: k REAL :: dzk K_m(kts)=0. K_h(kts)=0. K_q(kts)=0. DO k=kts+1,kte dzk = 0.5 *( dz(k)+dz(k-1) ) K_m(k)=dfm(k)*dzk K_h(k)=dfh(k)*dzk K_q(k)=dfq(k)*dzk ENDDO END SUBROUTINE retrieve_exchange_coeffs ! ================================================================== SUBROUTINE tridiag(n,a,b,c,d) 8,2 !! to solve system of linear eqs on tridiagonal matrix n times n !! after Peaceman and Rachford, 1955 !! a,b,c,d - are vectors of order n !! a,b,c - are coefficients on the LHS !! d - is initially RHS on the output becomes a solution vector !------------------------------------------------------------------- INTEGER, INTENT(in):: n REAL, DIMENSION(n), INTENT(in) :: a,b REAL, DIMENSION(n), INTENT(inout) :: c,d INTEGER :: i REAL :: p REAL, DIMENSION(n) :: q c(n)=0. q(1)=-c(1)/b(1) d(1)=d(1)/b(1) DO i=2,n p=1./(b(i)+a(i)*q(i-1)) q(i)=-c(i)*p d(i)=(d(i)-a(i)*d(i-1))*p ENDDO DO i=n-1,1,-1 d(i)=d(i)+q(i)*d(i+1) ENDDO END SUBROUTINE tridiag ! ================================================================== SUBROUTINE mynn_bl_driver(& 1,8 &initflag,& &grav_settling,& &delt,& &dz,& &u,v,th,qv,qc,& &p,exner,rho,& &xland,ts,qsfc,qcg,ps,& &ust,ch,hfx,qfx,rmol,wspd,& &Qke,& !ACF for QKE advection &qke_adv,bl_mynn_tkeadvect,& !ACF-end &Tsq,Qsq,Cov,& &Du,Dv,Dth,& &Dqv,Dqc,& ! &K_m,K_h,K_q& &K_h,k_m,& &Pblh& !JOE-added for extra ouput &,el_mynn& !JOE-end !JOE-TKE BUDGET &,dqke,qWT,qSHEAR,qBUOY,qDISS & &,bl_mynn_tkebudget & !JOE-end &,IDS,IDE,JDS,JDE,KDS,KDE & &,IMS,IME,JMS,JME,KMS,KME & &,ITS,ITE,JTS,JTE,KTS,KTE) !------------------------------------------------------------------- INTEGER, INTENT(in) :: initflag INTEGER, INTENT(in) :: grav_settling INTEGER, INTENT(in) :: bl_mynn_tkebudget !ACF for QKE advection LOGICAL, INTENT(IN) :: bl_mynn_tkeadvect !ACF-end INTEGER,INTENT(IN) :: & & IDS,IDE,JDS,JDE,KDS,KDE & &,IMS,IME,JMS,JME,KMS,KME & &,ITS,ITE,JTS,JTE,KTS,KTE ! initflag > 0 for TRUE ! else for FALSE ! levflag : <>3; Level 2.5 ! = 3; Level 3 ! grav_settling = 1 when gravitational settling accounted for ! grav_settling = 0 when gravitational settling NOT accounted for REAL, INTENT(in) :: delt REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), INTENT(in) :: dz,& &u,v,th,qv,qc,p,exner,rho REAL, DIMENSION(IMS:IME,JMS:JME), INTENT(in) :: xland,ust,& &ch,rmol,ts,qsfc,qcg,ps,hfx,qfx, wspd REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), INTENT(inout) :: & &Qke,Tsq,Qsq,Cov, & !ACF for QKE advection &qke_adv !ACF-end REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), INTENT(out) :: & &Du,Dv,Dth,Dqv,Dqc REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), INTENT(out) :: & &K_h,K_m REAL, DIMENSION(IMS:IME,JMS:JME), INTENT(inout) :: & &Pblh REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), INTENT(inout) :: & &el_mynn !JOE-TKE BUDGET REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME), & INTENT(inout) :: & qWT,qSHEAR,qBUOY,qDISS,dqke !JOE-end !local vars INTEGER :: ITF,JTF,KTF INTEGER :: i,j,k REAL, DIMENSION(KMS:KME) :: thl,sqv,sqc,sqw,& &El, Dfm, Dfh, Dfq, Tcd, Qcd, Pdk, Pdt, Pdq, Pdc, Vt, Vq REAL, DIMENSION(IMS:IME,KMS:KME,JMS:JME) :: K_q REAL, DIMENSION(KMS:KME+1) :: zw REAL :: cpm,sqcg,flt,flq,pmz,phh,exnerg,zet REAL, DIMENSION(KMS:KME) :: thetav INTEGER, SAVE :: levflag JTF=MIN0(JTE,JDE-1) ITF=MIN0(ITE,IDE-1) KTF=MIN0(KTE,KDE-1) levflag=mynn_level IF (initflag > 0) THEN DO j=JTS,JTF DO i=ITS,ITF DO k=KTS,KTF sqv(k)=qv(i,k,j)/(1.+qv(i,k,j)) thl(k)=th(i,k,j) thetav(k)=th(i,k,j)*(1.+0.61*sqv(k)) IF (k==kts) THEN zw(k)=0. ELSE zw(k)=zw(k-1)+dz(i,k-1,j) ENDIF k_m(i,k,j)=0. k_h(i,k,j)=0. k_q(i,k,j)=0. el_mynn(i,k,j)=0. IF ( bl_mynn_tkebudget == 1) THEN !TKE BUDGET VARIABLES qWT(i,k,j)=0. qSHEAR(i,k,j)=0. qBUOY(i,k,j)=0. qDISS(i,k,j)=0. dqke(i,k,j)=0. ENDIF ENDDO zw(ktf+1)=zw(ktf)+dz(i,ktf,j) CALL GET_PBLH(KTS,KTE,PBLH(i,j),thetav(kts:kte),& & Qke(i,kts:kte,j),zw(kts:kte+1),dz(i,kts:kte,j),xland(i,j)) CALL mym_initialize ( kts,kte,& &dz(i,kts:kte,j), zw(kts:kte+1), & &u(i,kts:kte,j), v(i,kts:kte,j), & &thl(kts:kte), sqv(kts:kte),& !JOE-BouLac mod &PBLH(i,j),th(i,kts:kte,j),& !JOE-end &ust(i,j), rmol(i,j),& &Qke(i,kts:kte,j), Tsq(i,kts:kte,j), & &Qsq(i,kts:kte,j), Cov(i,kts:kte,j)) !ACF,JOE- initialize qke_adv array if using advection IF (bl_mynn_tkeadvect) THEN DO k=KTS,KTF qke_adv(i,k,j)=qke(i,k,j) ENDDO ENDIF !ACF,JOE-end ENDDO ENDDO ENDIF ! end initflag !ACF copy qke_adv array into qke if using advection IF (bl_mynn_tkeadvect) THEN qke=qke_adv ENDIF !ACF-end DO j=JTS,JTF DO i=ITS,ITF DO k=KTS,KTF !JOE-TKE BUDGET IF ( bl_mynn_tkebudget == 1) THEN dqke(i,k,j)=qke(i,k,j) END IF sqv(k)=qv(i,k,j)/(1.+qv(i,k,j)) sqc(k)=qc(i,k,j)/(1.+qc(i,k,j)) sqw(k)=sqv(k)+sqc(k) thl(k)=th(i,k,j)-xlvcp/exner(i,k,j)*sqc(k) thetav(k)=th(i,k,j)*(1.+0.61*sqv(k)) IF (k==kts) THEN zw(k)=0. ELSE zw(k)=zw(k-1)+dz(i,k-1,j) ENDIF ENDDO zw(ktf+1)=zw(ktf)+dz(i,ktf,j) CALL GET_PBLH(KTS,KTE,PBLH(i,j),thetav(kts:kte),& Qke(i,kts:kte,j),zw(kts:kte+1),dz(i,kts:kte,j),xland(i,j)) sqcg=qcg(i,j)/(1.+qcg(i,j)) cpm=cp*(1.+0.8*qv(i,kts,j)) ! The exchange coefficient for cloud water is assumed to be the same as ! that for heat. CH is multiplied by WSPD. See module_sf_mynn.F exnerg=(ps(i,j)/p1000mb)**rcp flt = hfx(i,j)/( rho(i,kts,j)*cpm ) & +xlvcp*ch(i,j)*(sqc(kts)/exner(i,kts,j)-sqcg/exnerg) flq = qfx(i,j)/ rho(i,kts,j) & -ch(i,j)*(sqc(kts) -sqcg ) !!!!! zet = 0.5*dz(i,kts,j)*rmol(i,j) if ( zet >= 0.0 ) then pmz = 1.0 + (cphm_st-1.0) * zet phh = 1.0 + cphh_st * zet else pmz = 1.0/ (1.0-cphm_unst*zet)**0.25 - zet phh = 1.0/SQRT(1.0-cphh_unst*zet) end if !!!!! CALL mym_condensation ( kts,kte,& &dz(i,kts:kte,j), & &thl(kts:kte), sqw(kts:kte), & &p(i,kts:kte,j),exner(i,kts:kte,j), & &tsq(i,kts:kte,j), qsq(i,kts:kte,j), cov(i,kts:kte,j), & &Vt(kts:kte), Vq(kts:kte)) CALL mym_turbulence ( kts,kte,& &levflag, & &dz(i,kts:kte,j), zw(kts:kte+1), & &u(i,kts:kte,j), v(i,kts:kte,j), thl(kts:kte),& &sqc(kts:kte), sqw(kts:kte), & &qke(i,kts:kte,j), tsq(i,kts:kte,j), & &qsq(i,kts:kte,j), cov(i,kts:kte,j), & &vt(kts:kte), vq(kts:kte),& &rmol(i,j), flt, flq, & !JOE-BouLac mod &PBLH(i,j),th(i,kts:kte,j),& !JOE-end &el_mynn(i,kts:kte,j), & &Dfm(kts:kte),Dfh(kts:kte),Dfq(kts:kte), & &Tcd(kts:kte),Qcd(kts:kte),Pdk(kts:kte), & &Pdt(kts:kte),Pdq(kts:kte),Pdc(kts:kte) & !JOE-TKE BUDGET &,qWT(i,kts:kte,j),qSHEAR(i,kts:kte,j),& &qBUOY(i,kts:kte,j),qDISS(i,kts:kte,j),& &bl_mynn_tkebudget & !JOE-end &) CALL mym_predict (kts,kte,& &levflag, & &delt,& &dz(i,kts:kte,j), & &ust(i,j), flt, flq, pmz, phh, & &el_mynn(i,kts:kte,j), dfq(kts:kte), pdk(kts:kte), & &pdt(kts:kte), pdq(kts:kte), pdc(kts:kte),& &Qke(i,kts:kte,j), Tsq(i,kts:kte,j), & &Qsq(i,kts:kte,j), Cov(i,kts:kte,j)) CALL mynn_tendencies(kts,kte,& &levflag,grav_settling,& &delt,& &dz(i,kts:kte,j),& &u(i,kts:kte,j),v(i,kts:kte,j),& &th(i,kts:kte,j),qv(i,kts:kte,j),qc(i,kts:kte,j),& &p(i,kts:kte,j),exner(i,kts:kte,j),& &thl(kts:kte),sqv(kts:kte),sqc(kts:kte),sqw(kts:kte),& &ust(i,j),flt,flq,wspd(i,j),qcg(i,j),& &tsq(i,kts:kte,j),qsq(i,kts:kte,j),cov(i,kts:kte,j),& &tcd(kts:kte),qcd(kts:kte),& &dfm(kts:kte),dfh(kts:kte),dfq(kts:kte),& &Du(i,kts:kte,j),Dv(i,kts:kte,j),Dth(i,kts:kte,j),& &Dqv(i,kts:kte,j),Dqc(i,kts:kte,j)) CALL retrieve_exchange_coeffs(kts,kte,& &dfm(kts:kte),dfh(kts:kte),dfq(kts:kte),dz(i,kts:kte,j),& &K_m(i,kts:kte,j),K_h(i,kts:kte,j),K_q(i,kts:kte,j)) !JOE-TKE BUDGET IF ( bl_mynn_tkebudget == 1) THEN DO k=KTS,KTF dqke(i,k,j) = (qke(i,k,j)-dqke(i,k,j))*0.5 !qke->tke qWT(i,k,j) = qWT(i,k,j)*delt qSHEAR(i,k,j)= qSHEAR(i,k,j)*delt qBUOY(i,k,j) = qBUOY(i,k,j)*delt qDISS(i,k,j) = qDISS(i,k,j)*delt ENDDO ENDIF !JOE-end ENDDO ENDDO !ACF copy qke into qke_adv if using advection IF (bl_mynn_tkeadvect) THEN qke_adv=qke ENDIF !ACF-end END SUBROUTINE mynn_bl_driver ! ================================================================== SUBROUTINE mynn_bl_init_driver(& 1 &Du,Dv,Dth,& &Dqv,Dqc& &,RESTART,ALLOWED_TO_READ,LEVEL& &,IDS,IDE,JDS,JDE,KDS,KDE & &,IMS,IME,JMS,JME,KMS,KME & &,ITS,ITE,JTS,JTE,KTS,KTE) !--------------------------------------------------------------- LOGICAL,INTENT(IN) :: ALLOWED_TO_READ,RESTART INTEGER,INTENT(IN) :: LEVEL INTEGER,INTENT(IN) :: IDS,IDE,JDS,JDE,KDS,KDE, & & IMS,IME,JMS,JME,KMS,KME, & & ITS,ITE,JTS,JTE,KTS,KTE REAL,DIMENSION(IMS:IME,KMS:KME,JMS:JME),INTENT(OUT) :: & &Du,Dv,Dth,Dqv,Dqc INTEGER :: I,J,K,ITF,JTF,KTF JTF=MIN0(JTE,JDE-1) KTF=MIN0(KTE,KDE-1) ITF=MIN0(ITE,IDE-1) IF(.NOT.RESTART)THEN DO J=JTS,JTF DO K=KTS,KTF DO I=ITS,ITF Du(i,k,j)=0. Dv(i,k,j)=0. Dth(i,k,j)=0. Dqv(i,k,j)=0. Dqc(i,k,j)=0. ENDDO ENDDO ENDDO ENDIF mynn_level=level END SUBROUTINE mynn_bl_init_driver ! ================================================================== SUBROUTINE GET_PBLH(KTS,KTE,zi,thetav1D,qke1D,zw1D,dz1D,landsea) 2 !--------------------------------------------------------------- ! NOTES ON THE PBLH FORMULATION ! !The 1.5-theta-increase method defines PBL heights as the level at !which the potential temperature first exceeds the minimum potential !temperature within the boundary layer by 1.5 K. When applied to !observed temperatures, this method has been shown to produce PBL- !height estimates that are unbiased relative to profiler-based !estimates (Nielsen-Gammon et al. 2008). However, their study did not !include LLJs. Banta and Pichugina (2008) show that a TKE-based !threshold is a good estimate of the PBL height in LLJs. Therefore, !a hybrid definition is implemented that uses both methods, weighting !the TKE-method more during stable conditions (PBLH < 400 m). !A variable tke threshold (TKEeps) is used since no hard-wired !value could be found to work best in all conditions. !--------------------------------------------------------------- INTEGER,INTENT(IN) :: KTS,KTE REAL, INTENT(OUT) :: zi REAL, INTENT(IN) :: landsea REAL, DIMENSION(KTS:KTE), INTENT(IN) :: thetav1D, qke1D, dz1D REAL, DIMENSION(KTS:KTE+1), INTENT(IN) :: zw1D !LOCAL VARS REAL :: PBLH_TKE,qtke,qtkem1,wt,maxqke,TKEeps,minthv REAL :: delt_thv !delta theta-v; dependent on land/sea point REAL, PARAMETER :: sbl_lim = 200. !typical scale of stable BL (m). REAL, PARAMETER :: sbl_damp = 400. !transition length for blending (m). INTEGER :: I,J,K,kthv,ktke !FIND MAX TKE AND MIN THETAV IN THE LOWEST 500 M k = kts+1 kthv = 1 ktke = 1 maxqke = 0. minthv = 9.E9 DO WHILE (zw1D(k) .LE. 500.) qtke =MAX(Qke1D(k),0.) ! maximum QKE IF (maxqke < qtke) then maxqke = qtke ktke = k ENDIF IF (minthv > thetav1D(k)) then minthv = thetav1D(k) kthv = k ENDIF k = k+1 ENDDO !TKEeps = maxtke/20. = maxqke/40. TKEeps = maxqke/40. TKEeps = MAX(TKEeps,0.025) !FIND THETAV-BASED PBLH (BEST FOR DAYTIME). zi=0. k = kthv+1 IF((landsea-1.5).GE.0)THEN ! WATER delt_thv = 0.75 ELSE ! LAND delt_thv = 1.5 ENDIF zi=0. k = kthv+1 DO WHILE (zi .EQ. 0.) IF (thetav1D(k) .GE. (minthv + delt_thv))THEN zi = zw1D(k) - dz1D(k-1)* & & MIN((thetav1D(k)-(minthv + delt_thv))/MAX(thetav1D(k)-thetav1D(k-1),1E-6),1.0) ENDIF k = k+1 IF (k .EQ. kte-1) zi = zw1D(kts+1) !EXIT SAFEGUARD ENDDO !print*,"IN GET_PBLH:",thsfc,zi !FOR STABLE BOUNDARY LAYERS, USE TKE METHOD TO COMPLEMENT THE !THETAV-BASED DEFINITION (WHEN THE THETA-V BASED PBLH IS BELOW ~0.5 KM). !THE TANH WEIGHTING FUNCTION WILL MAKE THE TKE-BASED DEFINITION NEGLIGIBLE !WHEN THE THETA-V-BASED DEFINITION IS ABOVE ~1 KM. PBLH_TKE=0. k = ktke+1 DO WHILE (PBLH_TKE .EQ. 0.) !QKE CAN BE NEGATIVE (IF CKmod == 0)... MAKE TKE NON-NEGATIVE. qtke =MAX(Qke1D(k)/2.,0.) ! maximum TKE qtkem1=MAX(Qke1D(k-1)/2.,0.) IF (qtke .LE. TKEeps) THEN PBLH_TKE = zw1D(k) - dz1D(k-1)* & & MIN((TKEeps-qtke)/MAX(qtkem1-qtke, 1E-6), 1.0) !IN CASE OF NEAR ZERO TKE, SET PBLH = LOWEST LEVEL. PBLH_TKE = MAX(PBLH_TKE,zw1D(kts+1)) !print *,"PBLH_TKE:",i,j,PBLH_TKE, Qke1D(k)/2., zw1D(kts+1) ENDIF k = k+1 IF (k .EQ. kte-1) PBLH_TKE = zw1D(kts+1) !EXIT SAFEGUARD ENDDO !With TKE advection turned on, the TKE-based PBLH can be very large !in grid points with convective precipitation (> 8 km!), !so an artificial limit is imposed to not let PBLH_TKE exceed 4km. !This has no impact on 98-99% of the domain, but is the simplest patch !that adequately addresses these extremely large PBLHs. PBLH_TKE = MIN(PBLH_TKE,4000.) !BLEND THE TWO PBLH TYPES HERE: wt=.5*TANH((zi - sbl_lim)/sbl_damp) + .5 zi=PBLH_TKE*(1.-wt) + zi*wt END SUBROUTINE GET_PBLH ! ================================================================== END MODULE module_bl_mynn