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Convective Clouds Lecture Sequence Basic convective cloud types
Severe convection & mesoscale systems Tropical cloud population Convective feedbacks to large-scales Extreme convection Diurnal variability Clouds in tropical cyclones
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The tropical convective cloud population
Robert Houze University of Washington The midlevel inflow to the sf region is an imp part of the MCS circulation. Lecture, Summer School on Severe and Convective Weather, Nanjing, 11 July 2011
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The tropical convective cloud population
What do we know? How has technology contributed? What comes next? The midlevel inflow to the sf region is an imp part of the MCS circulation.
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Before Satellites
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Visual Observation Cumulonimbus Cumulus congestus Small cumulus
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Radiosonde data in the tropics
“Hot tower hypothesis” Riehl & Malkus 1958
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Convective parameterization
GCM grid
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Satellite Observations: an “inconvenient truth”
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Large cloud shields The IR pattern emphasizes the higher cloud tops, which largely determine the global precipitation (and hence latent heating) pattern.
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Satellite view of the tropical cloud population
Early 1970’s Satellite view of the tropical cloud population Explained satellite pictures Retained the hot tower notion Included smaller clouds
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The second “inconvenient truth”
Radars: The second “inconvenient truth”
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GATE 1974 40 ships. 12 a/c
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4 shipborne scanning digital C-band radars
1974 40 ships! 12 aircraft! 4 shipborne scanning digital C-band radars 40 ships. 12 a/c
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More Field Projects to Study Convection
BoB 1979 JASMINE 1999 EPIC TEPPS 1997 (Dashed: No sounding network) Ground, ship, & airborne cm radars
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Post-GATE view of the tropical cloud population
MESOSCALE CONVECTIVE SYSTEMS (MCSs) Hot Tower STRATIFORM RAIN GCM grid Houze et al. (1980)
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Heating and cooling processes in an MCS
Top heavy Houze 1982
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Simplified MCS Heating Profiles
Schumacher et al. 2004 Height (km) Deg K/day Convective Stratiform The blue curve is applied to the stratiform fraction of the precipitation at the given pixel. Go to next slide.
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MCS Net Heating Profiles
Height (km) Deg K/day 0% stratiform 40% stratiform 70% stratiform Schumacher et al. 2004 70% stratiform precipitation at a pixel yields the blue profile, which has a higher maximum than the 0% or 40 % stratiform profiles. Note also how the increased stratiform percentage yields a stronger vertical gradient of heating at upper levels and hence greater generation of potential vorticity. This shows how an increase in the stratiform rain fraction leads to a stronger circulation at upper levels.
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Precipitation Radar in Space
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The TRMM Satellite Ku-band Radar Low altitude, low inclination orbit
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Knowledge of global rainfall before satellites measured rain from space
Global water budget is formed from P, E, and runoff. Getting P accurate is very important to evaluating the residual P-E. The large max of P in the tropics is almost entirely the result of deep convection.
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Rainfall mapping revolutionized!
Satellites can map precipitation globally. ….This map is derived from a combination of IR, PMW, TRMM PR. Deeper clouds produce precipitation. ……Tropics mostly deep convection. ….. Midlatitudes partly convective, partly baroclinic. Combined satellite rainfall July 2000 TRMM plus passive microwave sensors + other
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TRMM Satellite Instrumentation
λ= 2 cm Important! PR measures 3D structure of radar echoes Wavelength—short for radar. Obtains data at high resolution in a 3D volume. Allows us to study vertical structure of echoes. Not trying to determine precip amounts. 92.5 minute orbit; approximately 16 orbits per day. Revisits specific locations times per 30 day period (dependent on latitude). Our data set consists of 1648 TRMM 2A23 & 2A25 rain containing orbit files from the monsoon season (June – September) in 2002 & 2003. The TRMM 2A25 data contains corrected TRMM reflectivity data in 250 m height bins. The TRMM 2A23 algorithm detects the presence of a bright band and categorizes precipitation as stratiform, convective or other (unclassified). Kummerow et al, 1998
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How tropical rain is distributed by cloud size and type
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2 Years of TRMM PR data Large Cbs MCSs Small isolated Cbs
Shallow isolated: Pixel separate from other rain certain areas withtop 1.5 km or more lower than climatological 0 deg C level. Schumacher & Houze 2003
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How do the environments of these regimes differ?
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TRMM PR Deep Convective TRMM PR Shallow, Isolated Convective
SST Climatology (July) July SST TRMM PR Shallow, Isolated Convective
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Traditional conceptual view of mean meridional distribution of tropical convection
Simpson 1992
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Stratocumulus Regime Moist layer a little deeper, but very dry aloft; no mechanism to remove the cap.
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Trade Wind Regime Moist layer a little deeper, but very dry aloft; no mechanism to remove the cap.
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Indo/Pacific Warm Pool
Marginally conditionally unstable through depth of troposphere. LCL low. Warm moist sfc air can get above LCL and have slight buoyancy to great heights, deep clouds, but relatively weak updrafts.
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“Trimodal” distribution Johnson et al
“Trimodal” distribution Johnson et al Evidence from TOGA COARE sounding data
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“Trimodal distribution”
Cu congestus Small Cb “Trimodal distribution” Suggested by TOGA COARE radiosonde data Johnson et al. 1999
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Cloud Radars
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“Trimodal” Distribution
X MANUS “Trimodal” Distribution Frequency of cloud-top height from 9 mm wavelength vertically pointing radar Histograms of cloud top height from MMCR for (a) day 20-08Z (b) night 8-20Z. Manus. Aug 1999-Oct 2000 35 GHZ, 9 mm wavelenght Hollars et al. 1999
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Cloud Radar in Space
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The A-Train Satellites show the complete MCS
MCSs previously studied in field projects—i.e. in local regions. Now they can be studied globally. Furthermore, the anvil clouds can be separated and studied separately. CloudSat CPR is 3mm wavelength MODS & AMSR-E are on Aqua Yuan and Houze 2010
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MCSs Over the Whole Tropics
(< km2) (> km2) Size of MCS is size of cold cloud top. To qualify as MCS, must have large cold cloud top, large rain area, and some heavy rain. This figure shows spatial distribution of active MCSs. Color of each point shows the number of active MCSs found within a circular area with radius of five degrees centered on that point. (a) Small separated MCSs (<12,000km2; i.e., the smallest 25%) in DJF, (b) large separated MCS (>40,000km2; i.e., the largest 25%) in DJF, (c) connected MCS in DJF, (d)-(f) same as (a)-(c) except for JJA. Yuan and Houze 2010
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Morphology of MCS anvils in different parts of the tropics
Data from CloudSat mm-Wavelength Cloud Profiling Radar Normalized by dimension of the MCS rain are Yuan and Houze 2010
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Internal structure of MCS anvils shown by CloudSat Cloud Profiling Radar
Africa Indian Ocean Yuan, Houze, and Heymsfield 2011
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Conceptual model of anvil microphysics
convective rain stratiform rain graupel snow WAVELENGTH: W-band, 3 mm wavelength THIN ANVILS: 1) LEADING—higher -- comes directly from convective updraft 2) TRAILING—occur at more levels -- moisten a deeper layer THICK ANVILS: 3) LEADING—stronger-larger particles -- graupel Cetrone and Houze 2011
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Five radars on a tiny island
Addu Atoll
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Non-precipitating Cumulus
Radar Supersite Approach Will document many aspects of the convective population HUMIDITY DUAL WAVELENGTH Water vapor * MM-WAVELENGTH Non-precipitating Cumulus Anvil cloud CM-WAVELENGTH Precipitation POLARIMETRY Microphysics DOPPLER Air motions
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Summary & Conclusions
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Timeline of progress Pre-satellite era Hot towers
Radars in field projects MCSs, convective and stratiform precipitation regions Precipitation radar in space Global patterns—convective, stratiform, shallow Cloud radars Ground based—trimodality of the population Satellite based—global distributions of MCSs, anvils, ... Dual wavelength Water vapor
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What we’ve learned Spectrum of convective cloud types and sizes covers a wide range of types and sizes of convective entities Mesoscale systems with stratiform rain Top-heavy heating profiles Multimodal size distributions Shallow isolated cells Structures of large anvil clouds Global variability of the population
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Where we are going How does convective population project onto larger-scale dynamics? Latent heating profiles Radiative heating profiles in anvils of MCSs Nonprecipitating convective clouds Relation between humidity field and cloud population evolution Role of clouds in MJO, ENSO, monsoon, & coupled equatorial waves
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This research was supported by
End This research was supported by NASA grants NNX07AD59G, NNX07AQ89G, NNX09AM73G, NNX10AH70G, NNX10AM28G, NSF grants, ATM , ATM , DOE grant DE-SC / ER-6
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Extra Slides
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Internal structure of “thick” anvils shown by CloudSat
Africa Indian Ocean Yuan, Houze, and Heymsfield 2011
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Internal structures of MCS anvils
Data from MCSs seen by ARM W-band radar in Niamey, Niger Height (km) WAVELENGTH: W-band, 3 mm wavelength THIN ANVILS: 1) LEADING—higher -- comes directly from convective updraft 2) TRAILING—occur at more levels -- moisten a deeper layer THICK ANVILS: 3) LEADING—stronger-larger particles -- graupel Cetrone & Houze 2011 and also Yuan et al CloudSat Reflectivity (dBZ)
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Internal structures of MCS anvils
Data from MCSs seen by ARM W-band radar in Niamey, Niger Height (km) WAVELENGTH: W-band, 3 mm wavelength THIN ANVILS: 1) LEADING—higher -- comes directly from convective updraft 2) TRAILING—occur at more levels -- moisten a deeper layer THICK ANVILS: 3) LEADING—stronger-larger particles -- graupel Cetrone & Houze 2011 and also Yuan et al CloudSat Reflectivity (dBZ)
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