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Tropical squall lines as convectively coupled gravity waves: Why do most systems travel westward?. Stefan Tulich 1 and George Kiladis 2 1 CIRES, University of Colorado, Boulder CO, USA 2 NOAA ESRL, Boulder CO, USA Funding: NSF ATM-0806553. Objectives.
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Tropical squall lines as convectively coupled gravity waves: Why do most systems travel westward? Stefan Tulich1 and George Kiladis2 1CIRES, University of Colorado, Boulder CO, USA 2NOAA ESRL, Boulder CO, USA Funding: NSF ATM-0806553
Objectives Provide evidence that many tropical “squall line systems” are part of a broad family of disturbances that arise through coupling between convection and tropospheric gravity waves Start to address the question of why most of these wave disturbances move westward
Outline Brief historical review of tropical squall lines - how did we come to know about them; current state of knowledge Analysis of observational data - provide evidence to support the idea Explicit simulations of convection on an equatorial beta-plane - test hypothesis about what causes westward bias Conclusions and future work
Historical Review of Tropical Squall Lines If one goes back to the earliest papers by leading authors, they’ll be pointed to two even earlier papers on west African squall lines
West African “Disturbance Lines” Hamilton and Archibald (1945; QJRMS; No previous articles referenced!) Eldridge (1957; QJRMS; 2 articles referenced)
West African “Disturbance Lines” Hamilton and Archibald (1945; QJRMS; No previous articles referenced!) Eldridge (1957; QJRMS; 2 articles referenced) 25 deg / 45 hr = 17 m/s
The Thunderstorm Project (1947; USA) Newton (1950; J. Meteor.) “Structure and mechanisms of the prefrontal squall line”
The Thunderstorm Project (1947; USA) Newton (1950; J. Meteor.) “Structure and mechanisms of the prefrontal squall line”
The Line Islands Exp. (1967 Cntrl. Pac.) Zipser (1969; J. Appl. Meteor.) “The role of organized unsaturated downdrafts in the structure and decay of an equatorial disturbance” 15 m/s
The Line Islands Exp. (1967 Cntrl. Pac.) Zipser (1969; J. Appl. Meteor.) “The role of organized unsaturated downdrafts in the structure and decay of an equatorial disturbance”
GATE (1974; Eastern Atlantic) Several squall lines sampled as they passed across the IFA Barnes and Sieckman (1984; MWR) “The environment of fast- and slow-moving tropical mesoscale convective cloud lines”
GATE (1974; Eastern Atlantic) A number of squall lines sampled as they passed across the IFA Barnes and Sieckman (1984; MWR) “The environment of fast- and slow-moving tropical mesoscale convective cloud lines” Vn > 7 m/s Vn < 3 m/s
TOGA-COARE (1992; Eq. west Pac.) Similar to GATE but satellite data more accessible Linear MCS-scale bands dominate total rainfall Numerous fast-moving “2-day waves” were sampled
TOGA-COARE (1992; Eq. west Pac.) 2-day wave composite evolution Haertel and Johnson (1998)
TOGA-COARE (1992; Eq. west Pac.) 2-day wave composite evolution ~ 1500 km Haertel and Johnson (1998)
TOGA-COARE (1992; Eq. west Pac.) 2-day wave composite evolution 16 m/s Haertel and Johnson (1998)
TOGA-COARE (1992; Eq. west Pac.) 2-day wave vertical cloud evolution Takayabu et al. (1996)
TOGA-COARE (1992; Eq. west Pac.) 2-day wave vertical cloud evolution Are 2-day waves just large-scale squall lines? Takayabu et al. (1996)
TOGA-COARE (1992; Eq. west Pac.) 2-day wave vertical cloud evolution Are 2-day waves just large-scale squall lines? Or are squall-lines mini- versions of 2-day waves? Takayabu et al. (1996)
Observational Analysis Goal: Advance the idea that many tropical squall line systems are part of a broader family of convectively coupled gravity wave disturbances Strategy: Space-time spectral (Fourier) analysis of high-resolution satellite data
Space-time spectral analysis: Previous work Power Spectrum of OLR (symmetric component) 1.25 days 3 days 96 days -15 15 WestwardEastward Wheeler and Kiladis (1999)
Space-time spectral analysis: Previous work Power Spectrum of OLR (symmetric component) Wheeler and Kiladis (1999)
Space-time spectral analysis: Previous work Power Spectrum of OLR (symmetric component) Westward inertia-gravity waves (1.3-2.5 day) Kelvin waves (3-10 day) Eq. Rossby waves (6-50 day) Wheeler and Kiladis (1999)
Spectral Analysis of TRMM TRMM 3B42 Rainfall Product 1) Global from 50N-50S 2) 0.25 deg. resolution in space 3) 3-hourly in time (1999-present) TRMM TMI CPC Global Merged IR
Spectral Analysis of TRMM TRMM 3B42 Rainfall Product 1) Global from 50N-50S 2) 0.25 deg. resolution in space 3) 3-hourly in time (1999-present)
TRMM rainfall spectrum 96 days 3 days 1.7 days
Looking at smaller scales 96 days 12 hrs 1 day -80 80
Looking at smaller scales 96 days 12 hrs 1 day Sharp diurnal peak -80 80
Looking at smaller scales hn ~ 20-40 m 96 days 12 hrs 1 day Sharp diurnal peak -80 80
Looking at smaller scales cn ~ 14-20 m/s 96 days 12 hrs 1 day Sharp diurnal peak -80 80
Looking at even smaller scales 6 hrs 12 hrs 96 days
Looking at even smaller scales 6 hrs 12 hrs 96 days ~ 6-hr periods & ~ 400-km wavelengths
Where are these signals most active? 6 hrs 12 hrs 96 days “WIG” filter window
Hovmollers of rainfall over N. Africa (7.5-12.5N) 2005 2006 2007
Hovmollers of rain over N. Africa (7.5-12.5N) 2005 2006 2007
How do these systems relate to objectively identified squall lines? AMMA 2006 Field Experiment (ROP: July 5 – Sept 27)
Analysis of Niamey Radar Data Rickenbach et al. (2009; JGR) “Radar-observed squall line propagation…”
Linear convective bands during TOGA COARE? Rickenbach and Rutledge (1998)
Linear convective bands during TOGA COARE? Rickenbach and Rutledge (1998)
What is the typical evolution of these disturbances? Strategy: Lagged linear regression of WIG-filtered rainfall to construct statistical composites
Location of base point Base point (2E, 10N)
Composite WIG rain evolution (2E,10N) Note: data averaged between 7.5-12.5 N