Supercell tornado environments

Slides:



Advertisements
Similar presentations
Tornado Workshop Langen, Germany, 25 February 2005 Contents 1. Basics –Parcel Theory –Perturbation pressure field –Updraft Rotation 2. Thunderstorm Classes.
Advertisements

The Analysis of Convective Storms
Some Applications of Indices to Forecasting
2005 National Severe Weather Workshop Paul Sirvatka April 20, 2004 Tornado Outbreak Nature Can Still Surprise… Paul L. Sirvatka Professor of Meteorology.
Synoptic/Meso-scale Comparison of Recent Historic Tornado Events Marc Kavinsky Senior Forecaster – Milwaukee/Sullivan WFO NWA 31 st Annual Meeting
ounding nalog etrieval ystem Ryan Jewell Storm Prediction Center Norman, OK SARS Sounding Analog Retrieval System.
Day 1 Severe Storms Forecasting Jim LaDue – WDTB 08 June, 2005.
Ounding nalog etrieval ystem Ryan Jewell Storm Prediction Center Norman, OK SARS Sounding Analog Retrieval System.
Outline  Introduction  CAPE Description  Parcel Choice  Fat vs Skinny  Other Forms  Conclusion.
Lesson 1 – Ingredients for severe thunderstorms
MesoscaleM. D. Eastin Deep Convection: Forecast Parameters.
The Impact of Gravity Wave/Undular Bore Dissipation on the June 22, 2003 Deshler and Aurora Nebraska Tornadic Supercells AARON W. JOHNSON NOAA/NWS Weather.
Characteristics of Isolated Convective Storms
1. 2 Presented by John P. Monteverdi Professor of Meteorology Department of Geosciences San Francisco State University Research completed as part of appointments.
My grandparents’ farm or so The farm NW of Sac City near Nemaha.
An Overview of Environmental Conditions and Forecast Implications of the 3 May 1999 Tornado Outbreak Richard L. Thompson and Roger Edwards Presentation.
Severe Convection and Mesoscale Convective Systems R. A. Houze Lecture, Summer School on Severe and Convective Weather, Nanjing, 11 July 2011.
More Thunderstorms. Today Homework in Wind shear More multicellular storms.
Meteorology 503 Meteorology 503 Tornadic Analysis Severe Weather Outbreak Dodge City, KS May 7, 2002 Julio C. Garcia! SFSU Julio C. Garcia! SFSU.
Lifting by cold pools (RKW theory) A&OS C115/C228.
6/26/2015 RUC Convective Parameters and Upscale Events in Southern Ontario Mike Leduc Environment Canada.
Kansas Tornadic Supercells May 7th, 2002 Austin Cross San Francisco State University Department of Geosciences Austin Cross San Francisco State University.
Synoptic, Thermodynamic, Shear Setting May 7, 2002 Tornadic Thunderstorm in Southwestern Kansas Michele Blazek May 15, 2005.
Characteristics of Isolated Convective Storms Meteorology 515/815 Spring 2006 Christopher Meherin.
Thunderstorms Conditions required: 1. Conditional instability 2. Trigger Mechanism (eg. front, sea-breeze front, mountains, localized zones of excess surface.
Corfidi, et al – convection where air parcels originate from a moist absolutely unstable layer above the PBL. Can produce severe hail, damaging.
Bow Echoes By Matthieu Desorcy.
© Craig Setzer and Al Pietrycha Supercell (mesocyclone) tornadoes: Supercell tornado environments Developed by Jon Davies – Private Meteorologist – Wichita,
1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part.
1 The Thermodynamic Diagram Adapted by K. Droegemeier for METR 1004 from Lectures Developed by Dr. Frank Gallagher III OU School of Meteorology.
Indices of Violent Tornado
A Study on the Environments Associated with Significant Tornadoes Occurring Within the Warm Sector versus Those Occurring Along Boundaries Jonathan Garner.
Observations of Near-Surface Thermodynamic and Wind Shear Profiles on Significant Tornado Days Observations of Near-Surface Thermodynamic and Wind Shear.
Composite Analysis of Environmental Conditions Favorable for Significant Tornadoes across Eastern Kansas Joshua M. Boustead, and Barbara E. Mayes NOAA/NWS.
Severe Convection and Mesoscale Convective Systems R. A. Houze Lecture, Indian Institute of Tropical Meteorology, Pune, 5 August 2010.
Soundings and Adiabatic Diagrams for Severe Weather Prediction and Analysis Continued.
The structure and evolution of vortex lines in supercell thunderstorms
Forecast Parameters. CAPE Convective Available Potential Energy – obviously, positive buoyancy is helpful for producing convection –100 mb mixed layer.
The Ingredients Based Tornado Parameter Matt Onderlinde.
Soundings and Adiabatic Diagrams for Severe Weather Prediction and Analysis.
Tropical Severe Local Storms Nicole Hartford. How do thunderstorms form?  Thunderstorms result from moist warm air that rises due to being less dense.
Summer Tornadoes – NWA 2015 Statistical Severe Convective Risk Assessment Model (SSCRAM) (Hart & Cohen, 2015) SPC Mesoanalysis Data Every hour from
Title card A Look at Environments Associated with Nighttime Supercell Tornadoes in the Central Plains Meteorologist Jon Davies Private © Dick McGowan &
The Analysis of Convective Storms. Thermodynamic Diagrams There are three desirable characteristics of atmospheric thermodynamic diagrams: The area enclosed.
Tornado Warning Skill as a Function of Environment National Weather Service Sub-Regional Workshop Binghamton, New York September 23, 2015 Yvette Richardson.
A Review of the March 28, 2007 Tornado Event Teresa Keck NWS North Platte, Nebraska Courtesy of Mike Hollingshead.
Christopher Nowotarski, Paul Markowski, Yvette Richardson
Principles of Convection. BACKGROUND When vertical shear is weak, the main influence on convective updrafts & downdrafts is bouyancy. As the vertical.
A Rare Severe Weather and Tornado Event in Central New York and Northeast Pennsylvania: July 8, 2014 Presented by Mike Evans 1.
The 22 May 2014 Duanesburg, NY, Tornadic Supercell Brian Tang, Matt Vaughan, Kristen Corbosiero, Ross Lazear, & Lance Bosart University at Albany, SUNY.
Kenneth R. Cook James Caruso Mickey McGuire National Weather Service, Wichita, KS.
Soundings and Adiabatic Diagrams for Severe Weather Prediction and Analysis Continued.
Cirrus anvil cumulonimbus T (skewed) LCL (Lifting Condensation Level) LFC (Level of Free Convection) EL (Equilibrium level) p overshooting CAPE Sounding.
Environmental Features Discriminating Between High Shear/Low CAPE Severe Convection and Null Events Keith Sherburn Matthew Parker North Carolina State.
Tornadoes – forecasting, dynamics and genesis Mteor 417 – Iowa State University – Week 12 Bill Gallus.
How to forecast the likelihood of thunderstorms!!!
Defining a Threat Area and Miller Techniques
Characteristics of Isolated Convective Storms
AOS 101 Severe Weather April 1/3.
SO441 Lesson 10: Tornadoes Week 15.
Convective: Part 2 Weather Systems – Fall 2017
Ingredients approach for severe weather
The Wind Hodograph METR 4433: Mesoscale Meteorology Spring 2013 Semester Adapted from Materials by Drs. Kelvin Droegemeier, Frank Gallagher III and Ming.
Forecast parameters, Tornadogensis, maintenance and decay
Neil Taylor1 and Bill Burrows2
Differences Between High Shear / Low CAPE Environments in the Northeast US Favoring Straight-Line Damaging Winds vs Tornadoes Michael E. Main, Ross A.
Tropical Cyclone Supercells and Tornadoes: Gaps in the Knowledge Base
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Lightning Potential Index (J/Kg) (Yair et al.2010,JGR)
Presentation transcript:

Supercell tornado environments Supercell (mesocyclone) tornadoes: © Craig Setzer and Al Pietrycha Developed by Jon Davies – Private Meteorologist – Wichita, Kansas

Basic environment ingredients for supercell tornadoes (from accepted research over the last 15 years) Basic environment ingredients for supercell tornadoes Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) (0-1 km) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights)

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) (0-1 km) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights) Sizable 0-3 km CAPE (relatively low LFC heights)? (Davies 2003)

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) (0-1 km) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights)

Need CAPE to generate an updraft for vertical stretching

Need low-level shear to generate horizontal vorticity (“spin”) ground 3 km 1 km

Tilting and stretching of horizontal vorticity: Low-level mesocyclones, possible tornadoes? Combinations of CAPE and low-level shear

Energy-Helicity Index from Johns, Davies, & Leftwich 1993 EHI = CAPE x SRH 160000 EHI = 2.0 F2+ tornadic storms Energy-Helicity Index

Energy-Helicity Index from Johns, Davies, & Leftwich 1993 Problems with EHI in this area of chart when SRH is large and CAPE is small EHI = CAPE x SRH 160000 EHI = 2.0 F2+ tornadic storms Energy-Helicity Index

Rasmussen (2003) 0-1 km EHI

CAPE-SRH combinations often don’t work well in these situations: Small CAPE – large SRH (many cool season cases) Cold core tornado situations (500 mb closed lows) Nonsupercell/nonmesocyclone tornadoes

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights)

Deep shear helps organize storms and strengthen updrafts This is important for most supercell tornadoes

from Davies and Johns 1993 30 kts 40 kts 50 kts F2+ tornadic storms

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights)

Low cloud bases (low LCL heights): clear slot/downdraft ( R F D ) updraft inflow low cloud bases & large humidity reduce cold pooling? downdraft not cold - contains buoyancy (Markowski et al. 2002)

From Craven and Brooks 2005 1500

Other environment characteristics that may have some relevance to tornadoes: Relatively low LFC heights? Sizable CAPE in low-levels (below 3 km)? (less work for low-level parcels of air to move upward and “stretch” in updrafts?)

(from 518 supercell cases using RUC profiles) F1 - F4 tornadoes by MLLFC range (from 518 supercell cases using RUC profiles) (Davies 2003)

Contrasting environments large CIN high LFC no CAPE0-3 low LCL This setting would probably be more favorable for tornadoes: small CIN low LFC large CAPE0-3 low LCL

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights) Sizable 0-3 km CAPE (relatively low LFC heights)?

Basic environment ingredients for supercell tornadoes: Instability (CAPE) Enhanced horizontal vorticity near ground (SRH) Deep-layer shear (0-6 km shear) Relatively low cloud bases? (low LCL heights) Sizable 0-3 km CAPE (relatively low LFC heights)? EHI S T P

Environment parameter values suggesting notable support for supercell tornadoes? 0-1 km MLEHI 2.0-3.0 or more? MLCAPE 500-1000 J kg-1 or more?* 0-1 km SRH 150-200 m2s-2 or more?* 0-6 km shear 30-35 kts or more?* MLLCL heights below 1200-1500 m?* 0-3 km MLCAPE 40-60 J kg-1 or more, MLLFC less than 2000-2500 m? Be careful using in small CAPE - large SRH settings! *in SPC’s STP parameter

Significant Tornado Parameter (updated - Thompson 2005): STP = MLCAPE/1500 x SRH0-1/150 x shear0-6/40 x (2000-LCL)/1500 x (200+CIN)/150 set to 1.5 if shear0-6 > 60 kts set to 0 if shear0-6 < 25 kts set to 1 if LCL < 1000 m set to 1 if CIN < -50 J/kg MLCAPE in J/kg; SRH in m2/s2; shear in kts; LCL in m; use lowest 100 mb mixed-layer lifted parcels

Environment parameters suggesting support for supercell tornadoes? Be careful using in small CAPE - large SRH settings! Use with caution… the atmosphere doesn’t recognize thresholds!!! 0-6 km shear < 30 kts 30 - 35 kts 36 - 44 kts 45+ kts 0-3 km CAPE < 20 J/kg 20-39 J/kg 40-59 J/kg 60+ J/kg (Surface boundaries can enhance and focus these parameters)

When using forecast fields of these ingredients: Look for areas of focus and convergence where storm development might be expected, and then assess how the parameter fields may affect that area. Fit the parameter fields with the surface pattern ! Don’t treat them as “magic numbers” or “bulls eyes” !

9 June 2005 Graham County KS tornado (w/Tim Samaras) 9 June 2005 – northwest Kansas: Strong supercell tornadoes (probe deployment attempt w/Tim Samaras) 8 May 2005 – central Kansas: nonsupercell/nonmesocyclone tornado

June 9, 2005

http://www.spc.noaa.gov

Storm relative helicity (SRH) http://www.spc.noaa.gov

Energy-helicity index (EHI) http://www.spc.noaa.gov

0-6 km shear http://www.spc.noaa.gov

LCL height http://www.spc.noaa.gov

LFC height http://www.spc.noaa.gov

(low-level instability) 0-3 km CAPE (low-level instability) http://www.spc.noaa.gov

MLCAPE 3780 J/kg 0-1 km SRH 140 m2/s2 0-1 km EHI 3.2 0-6 km shear 41 kts MLLCL 1290 m MLLFC 1610 m CAPE 0-3 km 90 J/kg STP 2.4

Significant Tornado Parameter (STP) All the basic environment ingredients that suggest support for supercell tornadoes came together in this area. http://www.spc.noaa.gov

1st tornadic storm develops

Tornado southwest of Hill City, KS ~ 4:25 pm CDT