matthew s. potter, lance f. bosart, and daniel keyser department of earth and atmospheric sciences

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the Inland Reintensification of Tropical Cyclone Danny (1997) within an Equatorward Jet-Entrance Region Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences University at Albany, SUNY, Albany, NY Support Provided By UCAR/NCEP Grant S1071092 NROW-XIII Thursday 3 November 2011

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A Multiscale Analysis of the Inland Reintensification of Tropical Cyclone Danny (1997) within an Equatorward Jet-Entrance Region. Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences University at Albany, SUNY, Albany, NY. NROW-XIII - PowerPoint PPT Presentation

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Page 1: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

A Multiscale Analysis of the Inland Reintensification of Tropical Cyclone Danny (1997) within an Equatorward

Jet-Entrance Region

Matthew S. Potter, Lance F. Bosart, and Daniel KeyserDepartment of Earth and Atmospheric Sciences

University at Albany, SUNY, Albany, NY

Support Provided By UCAR/NCEP Grant S1071092

NROW-XIIIThursday 3 November 2011

Page 2: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview

• Motivation and Objectives • Data and Methodology

• TC Danny (1997) Case Study

• TC Camille (1969) Case Study

• Concluding Remarks

Page 3: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Motivation

• Documentation of inland reintensifying tropical cyclones (TCs) is scarce:

–Bosart and Lackmann (1995): TC David (1979)

–Bassil and Morgan (2006): TC Danny (1997)

– Evans et al. (2011): TC Erin (2007)

Page 4: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Objectives

• Identify inland reintensifying TCs during a 61-yr time period (1950–2010)

• Investigate the physical mechanisms that enable a TC to reintensify inland

Page 5: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Data and Methodology

• Inland Reintensifying TCs (1950–2010)

– TCs which may have reintensified inland (“candidate cases”) were selected subjectively based on information gathered from • NHC best-track data• Archived surface charts from NCDC on microfilm• 2.5° NCEP–NCAR Reanalysis datasets

– Subjective criteria were employed to identify inland reintensifying TCs

Page 6: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

– Subjective criteria used to create a list of inland reintensifying TCs

• Minimum central MSLP decreased by 2 hPa and/or maximum sustained wind speed increased by 5 kt in a 6-h time period

• Central circulation (i.e., eye) of the TC remained inland throughout reintensification

• 500-hPa wind speed was less than or equal to 30 kt

• Vertically stacked, warm-core was maintained or enhanced during reintensification

Data and Methodology

Page 7: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

• TC Danny Case Study– Used 0.5° Climate Forecast System Reanalysis (CFSR)

datasets to produce maps and cross sections– Employed a potential vorticity perspective to help

elucidate the TC-jet interaction– Used WSR-88D radar data and satellite imagery

from Unidata–Wisconsin data stream to identify changes in precipitation structure

• TC Camille Case Study– Used 2.5° ECMWF 40-yr Reanalysis (ERA-40)

datasets to produce maps and cross sections

Data and Methodology

Page 8: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Inland Reintensifying TCs (1950–2010)

Cindy (1959) Danny (1997)

Cleo (1964) Helene (2000)

Agnes (1972) Allison (2001)

David (1979) Gaston (2004)

Diana (1984) Erin (2007)

• Every TC had an interaction with a upper-level jet except Erin (2007)

•TC Danny had the largest pressure fall (12 hPa) and wind speed increase (10 m s-1) inland compared to other TCs in the climatology

Page 9: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny

0000 UTC Locations

1800 UTC 24 July1000 hPa 40 kt

0000 UTC 19 July984 hPa 70 kt

0000 UTC 24 July1012 hPa 20 kt

960 mm of rain fell over Dauphin Island

Track where TC Danny reintensified inland

Page 10: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 11: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 12: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 13: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 14: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 15: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 16: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 17: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Danny250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 18: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Relatively Low Shear Environment Under Anticyclone

Page 19: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 20: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 21: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 22: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 23: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 24: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 25: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 26: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Cross Section and Dynamic Tropopause MapPV (shaded every 1 PVU), θ (solid black, every 5 K), and the wind component normal to the cross section (dotted green every 5 m s-1)

Potential temperature (shaded every 5 K), winds (barbs in kt), and 925–850-hPa layer-averaged relative vorticity (solid black every 0.5 × 10-4 s-1)

Page 27: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Radar and Satellite Imagery

KBMX Base Reflectivity 1813 UTC 22 July

GOES-8 Visible Image 1815 UTC 22 July

Page 28: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KBMX Base Reflectivity 0013 UTC 23 July

GOES-8 Visible Image 2315 UTC 22 July

Radar and Satellite Imagery

Page 29: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KFFC Base Reflectivity 0611 UTC 23 July

GOES-8 Infrared Image 0615 UTC 23 July

Radar and Satellite Imagery

Page 30: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KFFC Base Reflectivity 1218 UTC 23 July

GOES-8 Visible Image 1215 UTC 23 July

Radar and Satellite Imagery

Page 31: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KGSP Base Reflectivity 1823 UTC 23 July

GOES-8 Visible Image 1815 UTC 23 July

Radar and Satellite Imagery

Page 32: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KGSP Base Reflectivity 0015 UTC 24 July

GOES-8 Visible Image 2315 UTC 23 July

Radar and Satellite Imagery

Page 33: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KCAE Base Reflectivity 0617 UTC 24 July

GOES-8 Infrared Image 0615 UTC 24 July

Radar and Satellite Imagery

Page 34: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KAKQ Base Reflectivity 1318 UTC 24 July

GOES-8 Visible Image 1313 UTC 24 July

Radar and Satellite Imagery

Page 35: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

KAKQ Base Reflectivity 1814 UTC 24 July

GOES-8 Visible Image 1815 UTC 24 July

Radar and Satellite Imagery

Page 36: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Diabatic Outflow at 1800 UTC 24 July250-hPa wind speed (color shading in kt), 250-hPa potential vorticity (solid gray every 1 PVU), 250-hPa relative humidity (gray shading in %), 600–400-hPa layer-averaged ω (red every 4 × 10-3 hPa s-1, negative values only), 300–200 hPa layer-averaged irrotational wind (arrows, m s-1)

Diabatic outflow from convection around TC Danny strengthens jet

Page 37: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and FrontogenesisFrontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

5 cm/s

Page 38: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 39: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 40: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 41: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 42: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 43: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 44: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Frontogenesis

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 45: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Frontogenesis

Ageostrophic Circulation and Frontogenesis

5 cm/s

Frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every --5 × 10-3 hPa s-1), wind component normal to the cross section (solid brown, m s-1), and the ageostrophic wind component tangential to the cross section (arrows, m s-1)

Page 46: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Danny Remarks• Danny Case Study– The inland reintensification of TC Danny can be

attributed to:(1) Frontogenesis along the lower-tropospheric baroclinic

zone and the associated tropospheric-deep ascent beneath the equatorward entrance region of the upper-level jet

(2) Deep convection that provided a source of diabatic heating and reinforced the ascent near the storm center

(3) Upper-tropospheric PV reduction north of the storm center that strengthened the meridional PV gradient and the associated jet

(4) Lower-tropospheric vorticity growth in an environment that favored enhanced ascent near the storm center

Page 47: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Camille

0000 UTC Locations

0000 UTC 18 August909 hPa 165 kt

0000 UTC 20 August1005 hPa 25 kt

Severe Inland Flooding (153 fatalities)

690 mm of rain fell over West Nelson County

Page 48: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Camille250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 49: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Camille250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 50: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Overview of TC Camille250-hPa wind speed (shaded, m s-1), 1000–500-hPa thickness (dashed red, dam), and MSLP (solid black, hPa)

Page 51: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Frontogenesis and Moisture 925-hPa frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 1 K), mixing ratio (solid red every 1 g kg-1), and winds (barbs, m s-1)

Page 52: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Frontogenesis and Moisture 925-hPa frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 1 K), mixing ratio (solid red every 1 g kg-1), and winds (barbs, m s-1)

Page 53: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Frontogenesis and Moisture

Region of worst flooding

925-hPa frontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 1 K), mixing ratio (solid red every 1 g kg-1), and winds (barbs ,m s-1)

Page 54: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and FrontogenesisFrontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every 0.5 × 10-3 hPa s-1, negative values only), and the ageostrophic wind component tangential to the cross section (m s-1)

5 cm/s

Page 55: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and FrontogenesisFrontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every 0.5 × 10-3 hPa s-1, negative values only), and the ageostrophic wind component tangential to the cross section (m s-1)

5 cm/s

Frontogenesis

Page 56: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Ageostrophic Circulation and FrontogenesisFrontogenesis (shaded in K (100 km)-1 (3 h)-1), θ (solid black every 5 K), ω (dotted red every 0.5 × 10-3 hPa s-1, negative values only), and the ageostrophic wind component tangential to the cross section (m s-1)

5 cm/s

Frontogenesis

Page 57: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Camille Remarks

• Camille Case Study– The inland flooding associated with TC

Camille can be attributed to:(1) Moist, southerly flow that focused moisture

along a lower-tropospheric frontogenetical baroclinic zone over an area of complex terrain

(2) Tropospheric-deep ascent beneath the equatorward entrance region of an upper-level jet

Page 58: Matthew S. Potter, Lance F. Bosart, and Daniel Keyser Department of Earth and Atmospheric Sciences

Concluding Remarks• Differences between TC Camille and TC Danny– Inland reintensification only occurred with TC Danny– Inland flooding associated with TC Camille occurred in a

more favorable environment

• Similarities between TC Camille and TC Danny– Interaction with an equatorward entrance region of an

upper-level jet– Frontogenesis along a lower-tropospheric baroclinic zone