Precipitation as a driver of cloud droplet concentration variability along 20°S Photograph: Tony Clarke, VOCALS REx flight RF07 Robert Wood University.

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Presentation transcript:

Precipitation as a driver of cloud droplet concentration variability along 20°S Photograph: Tony Clarke, VOCALS REx flight RF07 Robert Wood University of Washington Dave Leon and Jeff Snider, University of Wyoming Robert Wood University of Washington Dave Leon and Jeff Snider, University of Wyoming

Radiative impact of cloud droplet concentration variations George and Wood, Atmos. Chem. Phys., 2010 albedo enhancement (fractional) Satellite-derived cloud droplet concentration N d low level wind How do we explain this pattern?

Aerosol (D>0.1  m) vs cloud droplet concentration (VOCALS, SE Pacific) 1:1 line see also... Twomey and Warner (1967) Martin et al. (1994)

Use method of Boers and Mitchell (1996), applied by Bennartz (2007) Screen to remove heterogeneous clouds by insisting on CF liq >0.6 in daily L3 MODIS-estimated mean cloud droplet concentration N d

Prevalence of drizzle from low clouds Leon et al., J. Geophys. Res. (2008) Drizzle occurrence = fraction of low clouds (1-4 km tops) for which Z max > -15 dBZ DAY NIGHT

Simple CCN budget in the MBL Model accounts for: Entrainment Surface production (sea-salt) Coalescence scavenging Dry deposition Model does not account for: New particle formation – significance still too uncertain to include Advection – more later  0

Production terms in CCN budget FT Aerosol concentration MBL depth Entrainment rate Wind speed at 10 m Sea-salt parameterization-dependent constant We use Clarke et al. (J. Geophys. Res., 2007) at 0.4% supersaturation to represent an upper limit

Loss terms in CCN budget: (1) Coalescence scavenging Precip. rate at cloud base MBL depth Constant cloud thickness Wood, J. Geophys. Res., 2006 Comparison against results from stochastic collection equation (SCE) applied to observed size distribution

Steady state (equilibrium) CCN concentration

VariableSourceDetails N FT Weber and McMurry (1996) & VOCALS in-situ observations (next slide) cm -3 active at 0.4% SS in remote FT DERA-40 Reanalysisdivergent regions in monthly mean U 10 Quikscat/Reanalysis- P CB CloudSat VOCALS (WCR and in-situ) PRECIP-2C-COLUMN, Haynes et al. (2009) & Z-based retrieval hMODISLWP, adiabatic assumption zizi CALIPSO or MODIS or COSMIC MODIS T top, CALIPSO z top, COSMIC hydrolapse Observable constraints from VOCALS and A-Train

Free tropospheric CCN source S = 0.9% S = 0.25% Data from VOCALS (Jeff Snider) Continentally- influenced FT Remote “background” FT Weber and McMurry (FT, Hawaii) S=0.9%

Self-preserving aerosol size distributions after Friedlander, explored by Raes: Raes et al., J. Geophys. Res. (1995) Fixed supersaturation: 0.8% 0.4% 0.2% Variable supersat. 0.3  0.2% Kaufman and Tanre (Nature 1994)

Precipitation over the VOCALS region CloudSat Attenuation and Z-R methods VOCALS Wyoming Cloud Radar and in-situ cloud probes Very little drizzle near coast Significant drizzle at 85 o W WCR data courtesy Dave Leon

Predicted and observed N d, VOCALS Model increase in N d toward coast is related to reduced drizzle and explains the majority of the observed increase Very close to the coast (<5 o ) an additional CCN source is required Even at the heart of the Sc sheet (80 o W) coalescence scavenging halves the N d Results insensitive to sea-salt flux parameterization o S

Mean precipitation rate (CloudSat, 2C-PRECIP-COLUMN, Stratocumulus regions)

Predicted and observed N d Monthly climatological means ( for MODIS, for CloudSat) Derive mean for locations where there are >3 months for which there is: (1) positive large scale div. (2) mean cloud top height <4 km (3) MODIS liquid cloud fraction > 0.4 Use 2C-PRECIP-COLUMN and Z-R where 2C-PRECIP- COLUMN missing

Reduction of N d from precipitation sink % Precipitation from midlatitude low clouds reduces N d by a factor of 5 In coastal subtropical Sc regions, precip sink is weak

But what controls precipitation? Precipitation rates P CB scale approximately with LWP 1.5 and N d -1 (e.g. Pawlowska and Brenguier 2003, Comstock et al. 2004, VanZanten et al. 2005) LWP 1.5 increases by a factor of  2.2 from 72.5 o W to 82.5 o W, while N d decreases by a factor of 2.5 (Bretherton et al. 2010)  LWP and N d influence the zonal gradient in precipitation rate along 20 o S in approximately equal measure  significant positive feedback on N d through aerosol-driven precipitation suppression; N d   P CB   N d  But see Chris Terai’s poster on precipitation susceptibility

Conclusions Simple CCN budget model, constrained with VOCALS observations predicts observed gradients in cloud droplet concentrations with some skill. FT aerosol significant possible source west of 75 o W. Significant fraction of the variability in N d across regions of extensive low clouds (from remote to coastal regions) is likely related to precipitation sinks rather than source variability. Implications for VOCALS Hypothesis H1c : – The small effective radii measured from space over the SEP are primarily controlled by anthropogenic, rather than natural, aerosol production, and entrainment of polluted air from the lower free-troposphere is an important source of cloud condensation nuclei (CCN) It may be difficult to separate the chicken from the egg in correlative studies suggesting inverse dependence of precipitation rate on cloud droplet concentration. Implications for Hypothesis H1a: – Variability in the physicochemical properties of aerosols has a measurable impact upon the formation of drizzle in stratocumulus clouds over the SEP.

Sea-salt source strength compared with entrainment from FT

Precipitation closure from Brenguier and Wood (2009) Precipitation rate dependent upon: cloud macrophysical properties (e.g. thickness, LWP); microphysical properties (e.g. droplet conc., CCN) precipitation rate at cloud base [mm/day]

A proposal A limited area perturbation experiment to critically test hypotheses related to aerosol indirect effects Cost  $30M

Precipitation susceptibility Construct from Feingold and Siebert (2009) can be used to examine aerosol influences on precipitation in both models and observations S = -(dlnR CB /dlnN a ) LWP,h Data from stratocumulus over the SE Pacific, Terai and Wood (Geophys. Res. Lett., 2011) S decreases strongly with cloud thickness Consistent with increasing importance of accretion in thicker clouds Consistent with results from A-Train (Kubar et al. 2009, Wood et al. 2009)

Effect of variable supersaturation Kaufman and Tanre 1994 Constant  Variable 

Range of observed and modeled CCN/droplet concentration in Baker and Charlson “drizzlepause” region where loss rates from drizzle are maximal Baker and Charlson source rates Baker and Charlson, Nature (1990)

Timescales to relax for N Entrainment: Surface:  sfc  Precip: z i /(hKP CB ) = 8x10^5/(3*2.25) = 1 day for P CB =1 mm day -1  dep  z i /w dep - typically 30 days

Can dry deposition compete with coalescence scavenging? w dep = to 0.03 cm s -1 (Georgi 1988) K = 2.25 m 2 kg -1 (Wood 2006) For P CB = > 0.1 mm day -1 and h = 300 m = 3 to 30 For precip rates > 0.1 mm day -1, coalescence scavenging dominates

Examine MODIS Nd imagery – fingerprinting of entrainment sources vs MBL sources.

Cloud droplet concentrations in marine stratiform low cloud over ocean Latham et al., Phil. Trans. Roy. Soc. (2011) The view from MODIS....how can we explain this distribution? N d [cm -3 ]

Baker and Charlson model CCN/cloud droplet concentration budget with sources (specified) and sinks due to drizzle (for weak source, i.e. low CCN conc.) and aerosol coagulation (strong source, i.e. high CCN conc.) Stable regimes generated at point A (drizzle) and B (coagulation) Observed marine CCN/N d values actually fall in unstable regime! Baker and Charlson, Nature (1990) observations CCN concentration [cm -3 ] CCN loss rate [cm -3 day -1 ]

Baker and Charlson model Stable region A exists because CCN loss rates due to drizzle increase strongly with CCN concentration – In the real world this is probably not the case, and loss rates are  constant with CCN conc. However, the idea of a simple CCN budget model is alluring Baker and Charlson, Nature (1990) observations CCN concentration [cm -3 ] CCN loss rate [cm -3 day -1 ]

Mean precipitation rate (2C-PRECIP-COLUMN)

Sea-spray flux parameterizations Courtesy of Ernie Lewis, Brookhaven National Laboratory u 10 =8 m s -1

MODIS-estimated cloud droplet concentration N d, VOCALS Regional Experiment Data from Oct-Nov 2008 Sampling along 20 o S across strong microphysical gradient

Conceptual model of background FT aerosol Clarke et al. (J. Geophys. Res. 1998)

Tomlinson et al., J. Geophys. Res. (2007) Observed MBL aerosol dry size distributions (SE Pacific) 0.08  m 0.06

Predicted and observed N d - histograms Minimum values imposed in GCMs

Loss terms in CCN budget: (2) Dry deposition Deposition velocity w dep = to 0.03 cm s -1 (Georgi 1988) K = 2.25 m 2 kg -1 (Wood 2006) For P CB = > 0.1 mm day -1 and h = 300 m = 3 to 30 For precip rates > 0.1 mm day -1, coalescence scavenging dominates

Precipitation over the VOCALS region CloudSat Attenuation and Z-R methods VOCALS Wyoming Cloud Radar and in-situ cloud probes Very little drizzle near coast Significant drizzle at 85 o W WCR data courtesy Dave Leon