Principal Rainband of Hurricane Katrina as observed in RAINEX Willoughby 1988 Anthony C. Didlake, Jr. 28th Conference on Hurricanes and Tropical Meteorology April 29, 2008 Barnes et al. 1983 Low-level radial inflow overturns inside of leaning reflectivity tower Downdraft within reflectivity tower continues as radial inflow Hurricane Katrina (2005) ELDORA radar • Sampling resolution ~0.4 km Similarities to Barnes et al. 1983 Hence and Houze 2008 Inner-edge downdraft What causes it? How often does it occur? What are the effects of it? Convective/stratiform classification Convective Similar to Steiner et al. 1995, TRMM satellite data classification Stratiform Weak echo No echo Rainband cross sections Radial cross sections at regular angular intervals • 0.375° 109 cross sections Cross section coordinates based on classification dBZ Two downdraft regimes Inner-edge downdrafts are slightly weaker and more localized Updrafts are strong and broad Vertical velocity (m/s) (plan view) dBZ Buoyant air parcel dBZ Conclusions Overturning updraft, low-level downdraft, inner-edge downdraft Inner-edge downdraft: • Convective scale feature, ~5 km • Creates sharp reflectivity gradient • Forced by rainband updrafts? Questions? Buoyancy pressure-gradient acceleration field H H Buoyant air parcel L L Idealized structure of a tropical cyclone downwind Primary and Secondary eyewalls Stationary Band Complex (SBC) • principal band • secondary band upwind Willoughby 1988 Autocorrelation along rainband D C B A Strong inner-edge downdrafts Low-level tangential wind max on inner-side of rainband References Willoughby, H.E., 1988: The dynamics of the tropical cyclone core. Aust. Met. Mag., 36, 183191. Barnes, G.M., E.J. Zipser, D. Jorgensen, and F. Marks, Jr., 1983: Mesoscale and convective structure of a hurricane rainband. J. Atmos. Sci., 40, 2125-2137. Hence, D.A. and R.A. Houze, Jr., 2008: Kinematic structure of convective-scale rainband features in Hurricanes Katrina and Rita (2005). J. Geophys. Res., accepted. “Strong” inner-edge downdrafts occur less frequently than “strong” updrafts Inner-edge downdrafts occur right along the reflectivity gradient Convective/stratiform classification Technique used in Steiner et al. 1995, Yuter and Houze 1997, Yuter et al. 2005 Algorithm separates convective regions from stratiform regions by comparing local reflectivity to background reflectivity Tuning of algorithm required to recognize convective regions; the rest is designated as stratiform Classification Algorithm Convective center if: • Z Zti • Z-Zbg Zcc(Zbg) Classified convective within R(Zbg) from convective center, remaining is classified stratiform (unless Z < Zwe) Zcc 1 Z bg Z cc a cos b 2 Zti = 45 dbZ Zwe = 20 dbZ R = 0.5+.23(Zbg-20) Rbg = 11 km a=9, b=45 Zbg Statistics of reflectivity data Yuter and Houze 1995 Beyond Barnes et al. (1983) x 10 -3 K1 - Deanna Hence Strong downdrafts where horizontal velocity decreases with height Tilting of vorticity tubes creates negative vertical vorticity Negative vertical vorticity is stretched in region of convergence and advected downward. It is confined to the lower layers by divergence at the ocean surface. Strong lower-level vertical vorticity is manifested in a local tangential wind maximum Future work Explore the roll of fluctuating updrafts and downdrafts in strength of storm circulation Compare dynamics with other convective regimes: eyewall, secondary eyewall, outer rainbands Analyze more ELDORA data volumes, N43 data, Rita rainbands Compare observations with model simulations, analyze evolution of rainbands altitude (km) Average tangential wind (m/s) distance (km) Aircraft and instruments NOAA P3 (N42, N43) Dropsondes and Doppler radar (dual-Doppler analysis) US Naval Research Laboratory P3 (NRL) ELDORA radar • Sampling resolution ~0.4 km Motivation for RAINEX How do interactions of environment, eyewalls, and rainbands in the mature storm… Max Wind Speed (knots) …lead to intensity changes like these? Intensity of Katrina (2005) 24 25 26 27 August 28 29
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