Sungsu Park, Christopher S. Bretherton, Phil J. Rasch

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Sungsu Park, Christopher S. Bretherton, Phil J. Rasch Progress on U.W. PBL and Macrophysics reformulations Interactions among cloud, radiation, and PBL turbulence CCSM Meeting, NCAR June. 17. 2008 Sungsu Park, Christopher S. Bretherton, Phil J. Rasch Dept. of Atmospheric Sciences, Univ. of Washington, Seattle NCAR Thanks to Cecile Hanny, Rich Neale

Outline Inconsistency between cloud fraction and in-cloud LWC Offline computation of stratiform macrophysics Introduction of a new macrophysics scheme UW PBL + UW ShCu + RK Microphysics + PBR Macrophysics UW PBL + UW ShCu + MG Microphysics + PBR Macrophysics

Inconsistency between stratus fraction and in-stratus LWC

Interplay among various processes in stratocumulus Large-Scale Subsidence Ocean Entrainment Moistening Cooling Cloud-top LW cooling In-cloud SW warming Aerosol Drying Warming Drizzle & Evaporative cooling Cumulus Advective cooling Advective drying Surface moisture flux Surface heat flux

Interplay among various processes in stratocumulus Entrainment Cloud-top LW cooling Aerosol Problem in stratiform macrophysics → Distortion of interaction between LW radiative cooling and inversion strength → Too shallow PBL and many other related problems Problem of droplet activation in MG stratiform microphysics ? → Too strong SW CRF → Too strong aerosol indirect effect in current CAM ? Ocean

CAMUW = CAM35 + UW PBL + UW ShCu PBL top OWSN (30N,140W). Yr 0. Sep. 26th CAMUW = CAM35 + UW PBL + UW ShCu Ambiguous Layer Cooling & Moistening due to entrainment Too large in-cloud LWC 4 [ g kg-1 ] !!! PBL top

[ K hr-1 ] CAM Nature -1.2 -4.9 ~ -4.0 ~ 0 Ambiguous L. Isothermal, cloud in the PBL top layer is a black body, transparent clear air [ K hr-1 ] CAM Nature Ambiguous L. -1.2 -4.9 PBL Top L. ~ -4.0 ~ 0 Ambiguous Layer PBL Top Layer θNATURE θCAM

→ What caused inconsistency between cloud fraction and in-cloud LWC ? As a result, current CAM suffers from → Strong inversion at the PBL top → Too weak entrainment → Too shallow, cold, moist PBL Too much (less) subtropical stratocumulus in downstream (upstream) Suppression of nocturnal deepening of PBL Too strong ENSO amplitude due to too weak SST damping by weak upward LHF Summary Inconsistency between cloud fraction and in-cloud LWC can exert large Influences on global climate system through complex feedbacks among cloud, radiation, and moist turbulence → What caused inconsistency between cloud fraction and in-cloud LWC ?

What caused inconsistency between cloud fraction and in-cloud LWC What caused inconsistency between cloud fraction and in-cloud LWC ? → Stratiform Macrophysics Scheme Isolate stratiform macrophysics from the CAM and perform off-line computation Force the ambiguous layer at p = 900 [hPa], T = 280 [K], qv = 6.84 [g kg-1], ql = 0.16 [g kg-1], a = 0.6, ∆p = 20 [hPa] with various external forcings of temperature (AT) and water vapor (Aqv) Neglect cumulus, cloud ice, and precipitation Examine ∆a vs ∆ql,cloud Test for CAM30, CAM35, Equilibrium CAM35, and Triangular PDF with a half width of total specific humidity = 0.1*qs(T,p)

How stratiform net condensation rate Q is computed in CAM Equilibrium CAM35 a0, Ω0 a0, Ω0 a0, Ω1 a1, Ω1 a1, Ω1 a : stratus fraction Ω = T, qv, ql, qi Equilibrium stratus fraction (a1) and state variables (Ω1) are used for computing Q at the next time step

II I III IV

II I III IV

II I III IV

Too small cloud fraction Too large in-cloud LWC Too small cloud fraction

II I III IV Too weak LW cooling Equilibrium CAM35 produces consistent cloud fraction and in-cloud LWC. → Realistic LW cooling rate and reasonable response of moist turbulence within PBL

A New Stratiform Macrophysics Scheme Uses equilibrium cloud fraction and equilibrium state variables for computing Q Formulation based on conservative scalars Consistent with the assumption of uniform T within the grid Incorporation of fusion heat in computing Q Treatment of ice and mixed-phase clouds Explicit treatment of cumulus cloud Cumulus and stratus are non-overlapped in each layer and have their own in-cloud LWC and cloud fraction

Cu Cu Stratus Stratus Original Macrophysics New Macrophysics Overlap In-cumulus CWC = In-stratus CWC Non-overlap In-cumulus CWC ≠ In-stratus CWC

A New Stratiform Macrophysics Scheme Uses equilibrium cloud fraction and equilibrium state variables for computing Q Formulation based on conservative scalars Consistent with the assumption of uniform T within the grid Incorporation of fusion heat in computing Q Treatment of ice and mixed-phase clouds Explicit treatment of cumulus cloud Cumulus and stratus are non-overlapped in each layer and have their own in-cloud LWC and cloud fraction Has the following functionalities: Stratus fraction formula based on either RH or triangular PDF (CAMstfrac) For PDF-based cloud, Uclr → 1 as ast → 1 consistent with the real world Specify in-cloud CWC (LWC+IWC) of newly formed or dissipated stratus from zero (cc=0) to the CWC of pre-existing stratus (cc=1) Force in-stratus CWC to be bounded by externally-specified limiting values (qcst_min>0, qcst_max>0) by performing pseudo condensation-evaporation in each layer. Natural removal of ‘empty’ (a>0, ql,cloud=0) and ‘dense’(a=0, ql,cloud>0) cloud Potential replacement of Vavrus polar cloud fix Explicit or implicit computation of Q by choosing different iteration number (niter) Potential to allow super-saturation within the stratus in any phases

CAMUW + RK Micro + New Macro 5 years AMIP runs using version CAM3_5_42 Several refinements are made to UW PBL and UW shallow convection Increase turbulent master length scale in the convective regime Refined computation of TKE at the entrainment interfaces Maximum cumulus updraft core fractional area of 10 % instead of 5 % Refined identification of penetrative entrainment zone Cumulus fraction and in-cumulus CWC are not included in computing radiation and grid-mean CWC. Switches in the macrophysics scheme CAMstfrac = RH cloud, cc = 1, niter = 3, qcst_min = 0.01, qcst_max = 3 [ g kg-1 ]

JJA LCA. Old Macro ΔPBLH. New - Old LCA. Observation LCA. New Macro The center of stratocumulus is shifted downstream compared to the observation PBL deepens in the stratocumulus deck LCA. Observation LCA. New Macro JJA Now, the center of stratocumulus is located at the correct spot ΔLCA. Old – Obs. ΔLCA. New – Old.

CAMUW + MG Micro + New Macro Condensation (Q) into cloud liquid [Qw= (1-f)*Q] and cloud ice [Qi= f*Q ] are explicitly treated within the macrophysics scheme by setting f = qi,cloud/(ql,cloud+qi,cloud) Bergeron-Findeisen process within the MG microphysics scheme is treated as a separate process independent of Q In the MG microphysics, droplet activation occurs only when Q > 0 instead of when ‘ql,cloud, qi,cloud > 0’ only one time at each time step, that is, mtime = 1 instead of mtime = ∆t / to where to is a mixing time scale of aerosol within cloud

ql,cloud > 0 Provide 2 CCN Q > 0 Provide 2 CCN Stratus Original Before Droplet Activation After Droplet Activation Stratus ql,cloud > 0 Original MG Micro. Provide 2 CCN Droplet Q > 0 Modified MG Micro. Provide 2 CCN

CAMUW + MG Micro + New Macro Condensation (Q) into cloud liquid [Qw= (1-f)*Q] and cloud ice [Qi= f*Q ] are explicitly treated within the macrophysics scheme by setting f = qi,cloud/(ql,cloud+qi,cloud) Bergeron-Findeisen process within the MG microphysics scheme is treated as a separate process independent of Q In the MG microphysics, droplet activation occurs only when Q > 0 instead of when ‘ql,cloud, qi,cloud > 0’ only one time at each time step, that is, mtime = 1 instead of mtime = ∆t / to where to is a mixing time scale of aerosol within cloud Cumulus fraction and in-cumulus CWC are explicitly included in computation of radiation and grid-mean CWC with appropriate tunings (dp1 = 0.03, co = 0.02) Switches in the macrophysics scheme CAMstfrac = RH cloud, cc = 0, niter = 3, qcst_min = 0.01, qcst_max = 3 [g/kg]

LWP. Annual Mean New Macro ΔLWP. New – Old Old Macro Increase of LWP in the trade cumulus & deep convection regimes due to explicit treatment of in-cumulus LWC

SWCF. Annual Mean Huge improvement of SWCF Old Macro New Macro CERES Observation ΔSWCF. New – Old Huge improvement of SWCF Enhanced SWCF in the trade due to explicit contribution of Cu CWC to radiation

→ Increase of in-cloud IWC in the storm track Δ In-cloud LWP. New - Old Δ In-cloud IWP. New - Old ‘Qi= f*Q’ + ‘Forcing in-stratus CWC to be bounded by two limiting values’ → Increase of in-cloud IWC in the storm track

UW PBL + UW ShCu + MG Micro + New Macro RESTOM [ W m-2 ] SWCF LWCF at 60oS. DJF TGCLDLWP [ g m-2 ] PRECT [ mm day-1 ] PREH2O [ mm ] LHFLX Base0 -6.3 -63.3 32.6 -170 105 2.91 26.5 85.1 Enhance entrainment1 (a2l = 30 ← 15) -4.5 -61.4 32.4 -163 100 Zero-CWC of newly formed stratus2 -7.4 -64.2 32.3 -168 90 2.99 26.3 87.5 Cloud drop activation only when Q > 03 -1.7 -56.2 30.1 -147 2.96 26.2 86.4 Increase activation time scale of CCN4 ( mtime = 1 ← 1.5 ) -5.4 -62.0 32.2 101 2.92 85.5 Enhance conversion of deep Cu LWC to precip.5 ( co = 0.02 ← 0.01 ) -4.9 -61.7 32.1 97 26.4 85.4 Reduce deep Cu fraction6 ( dp1 = 0.03 ← 0.05 ) -5.6 -62.7 85.3 Neglect Cu contribution in computing radiation -2.6 -58.8 32.0 -157 85 26.6 85.2 0+1(a2l=20)+2+3+4+5 0.3 -51.7 27.9 -140 75 3.07 25.8 89.8 Observation -48.6~-54.2 ( CERES, ERBE ) 27.2 ~30.4 -148 ( CERES ) 78 ~ 113 ( NVAP, MODIS ) 2.61 ( GPCP ) 25.0 ( ERA40 ) 82.4

Climate Bias Index (CBI) Summary of Global Model Performance Variable CAM30 rms error CAM3.5 ( Revise ZM deep conv. ) UW PBL UW ShCu RK Micro ZE Macro UW PBL* UW ShCu* MG Micro MG Micro* PBR Macro SLP 3.5 hPa 0.82 0.86 0.88 0.85 Surface wind stress 0.05 N m-2 0.81 0.76 0.84 Zonal wind at 300 hPa 4.5 m s-1 0.77 0.80 0.73 0.74 Surface rainfall 1.7 mm day-1 0.93 0.92 0.99 Air temperature at 2m 3.5 K 0.94 0.95 0.91 SWCF 22.8 W m-2 1.02 1.14 LWCF 11.7 W m-2 0.97 T 2.1 K RH 11.0 % 0.78 0.79 Climate Bias Index (CBI)

Conclusion We developed a new stratiform macrophysics scheme which ensures consistency between cloud fraction and in-cloud LWC by using equilibrium variables for computing Q, removes many conceptual and mathematical inconsistencies in CAM’s cloud system model by using conservative scalars in computing Q, taking into account of fusion heat, treating cumulus (CWC as well as fraction) separately from stratus, mimicking a PDF-approach in computing stratus fraction and in-stratus CWC, forcing in-stratus CWC to be bounded by two limiting values, allowing the possibility of super-saturation within stratus MG microphysics is modified, so that droplet activation occurs only when Q > 0 instead of whenever stratus exists → substantially reduced the bias of SWCF → may help to reduce too strong aerosol indirect effect (-2.3 → -1.1 Wm-2) ? Overall, our new macrophysics scheme deepens PBL in the stratocumulus deck and increases LWP in the trade cumulus regime, resulting in improved skill scores of SWCF and T. However, simulation of precipitation and surface wind stress is worsen due to enhancement of already strong hydrological cycle. Future and on-going works: Find a tuning set to weaken hydrological cycle Analysis of diurnal cycle and ENSO amplitude

Stochastic Ocean Mixed Layer Model [Frankignoul and Hasselman 1977; Deser et al. 2003; Park et al. 2006] Downward surface heat flux anomaly SST anomaly is amplified Positive feedback PBL turbulence, convective deflation stratocumulus, anvil cirrus water vapor, aerosol