PICTURE of the MONTH Some Frequently Overlooked Severe
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American Meteorological Society Revised Manuscript Click Here to Download Manuscript (Non-Latex): JAMC-D-14-0252 Revision3.Docx
AMERICAN METEOROLOGICAL SOCIETY Journal of Applied Meteorology and Climatology EARLY ONLINE RELEASE This is a preliminary PDF of the author-produced manuscript that has been peer-reviewed and accepted for publication. Since it is being posted so soon after acceptance, it has not yet been copyedited, formatted, or processed by AMS Publications. This preliminary version of the manuscript may be downloaded, distributed, and cited, but please be aware that there will be visual differences and possibly some content differences between this version and the final published version. The DOI for this manuscript is doi: 10.1175/JAMC-D-14-0252.1 The final published version of this manuscript will replace the preliminary version at the above DOI once it is available. If you would like to cite this EOR in a separate work, please use the following full citation: Wang, Y., and B. Geerts, 2015: Vertical-plane dual-Doppler radar observations of cumulus toroidal circulations. J. Appl. Meteor. Climatol. doi:10.1175/JAMC-D-14- 0252.1, in press. © 2015 American Meteorological Society Revised manuscript Click here to download Manuscript (non-LaTeX): JAMC-D-14-0252_revision3.docx Vertical-plane dual-Doppler radar observations of cumulus toroidal circulations Yonggang Wang1, and Bart Geerts University of Wyoming Submitted to J. Appl. Meteor. Climat. October 2014 Revised version submitted in May 2015 1 Corresponding author address: Yonggang Wang, Department of Atmospheric Science, University of Wyoming, Laramie WY 82071, USA; email: [email protected] 1 Profiling dual-Doppler radar observations of cumulus toroidal circulations 2 3 Abstract 4 5 6 High-resolution vertical-plane dual-Doppler velocity data, collected by an airborne profiling 7 cloud radar in transects across non-precipitating orographic cumulus clouds, are used to examine 8 vortical circulations near cloud top. -
The Lagrange Torando During Vortex2. Part Ii: Photogrammetry Analysis of the Tornado Combined with Dual-Doppler Radar Data
6.3 THE LAGRANGE TORANDO DURING VORTEX2. PART II: PHOTOGRAMMETRY ANALYSIS OF THE TORNADO COMBINED WITH DUAL-DOPPLER RADAR DATA Nolan T. Atkins*, Roger M. Wakimoto#, Anthony McGee*, Rachel Ducharme*, and Joshua Wurman+ *Lyndon State College #National Center for Atmospheric Research +Center for Severe Weather Research Lyndonville, VT 05851 Boulder, CO 80305 Boulder, CO 80305 1. INTRODUCTION studies, however, that have related the velocity and reflectivity features observed in the radar data to Over the years, mobile ground-based and air- the visual characteristics of the condensation fun- borne Doppler radars have collected high-resolu- nel, debris cloud, and attendant surface damage tion data within the hook region of supercell (e.g., Bluestein et al. 1993, 1197, 204, 2007a&b; thunderstorms (e.g., Bluestein et al. 1993, 1997, Wakimoto et al. 2003; Rasmussen and Straka 2004, 2007a&b; Wurman and Gill 2000; Alexander 2007). and Wurman 2005; Wurman et al. 2007b&c). This paper is the second in a series that pre- These studies have revealed details of the low- sents analyses of a tornado that formed near level winds in and around tornadoes along with LaGrange, WY on 5 June 2009 during the Verifica- radar reflectivity features such as weak echo holes tion on the Origins of Rotation in Tornadoes Exper- and multiple high-reflectivity rings. There are few iment (VORTEX 2). VORTEX 2 (Wurman et al. 5 June, 2009 KCYS 88D 2002 UTC 2102 UTC 2202 UTC dBZ - 0.5° 100 Chugwater 100 50 75 Chugwater 75 330° 25 Goshen Co. 25 km 300° 50 Goshen Co. 25 60° KCYS 30° 30° 50 80 270° 10 25 40 55 dBZ 70 -45 -30 -15 0 15 30 45 ms-1 Fig. -
Skip Talbot Photography by Jennifer Brindley
STORM SPOTTING Skip Talbot SECRETS Photography by Jennifer Brindley Ubl and others Topics • Supercell Visualization • Radar Presentation • Structure Identification • Storm Properties • Walk Through Disclaimers • Attend spotter training • Your safety is more important than spotting, photos, video, or tornado reports Supercell Visualization Lemon and Doswell 1979 Supercell Visualization Supercell Visualization Photo: Chris Gullikson Supercell Visualization Photo: Chris Gullikson Anvil Anvil Backshear Mammatus Cumulonimbus Flanking Line Cloud Base Striations Precipitation Wall Cloud Precipitation-free Base Supercell Visualization Radar Presentation Classic Hook Echo Radar Presentation Android / iOS Android Windows GrLevel3 / GrLevel2 Radar Presentation Classic Hook Echo Radar Presentation Radar Presentation Radar Presentation Radar Presentation Storm Spotting Zoo • Bear’s Cage • Whale’s Mouth • Beaver Tail • Horseshoe • Ghost Train Base (Updraft Base) (Rain Free Base or RFB) Base (Updraft Base) (Rain Free Base or RFB) Base (Updraft Base) (Rain Free Base or RFB) Base (Updraft Base) (Rain Free Base or RFB) Base (Updraft Base) (Rain Free Base or RFB) Base (Updraft Base) (Rain Free Base or RFB) Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe Horseshoe - Cyclical supercell with multiple tornadoes HorseshoeHorseshoe HorseshoeHorseshoe Horseshoe Horseshoe – Anticyclonic Funnel Horseshoe Horseshoe – Anticyclonic Funnel Horseshoe - No Wall Cloud Horseshoe - No Wall Cloud -
Mid-Latitude Dynamics and Atmospheric Rivers Session: Theory, Structure, Processes 1 Jason M
Mid-Latitude Dynamics and Atmospheric Rivers Session: Theory, Structure, Processes 1 Jason M. Cordeira Wednesday, 10 August 2016 Plymouth State University, CW3E/Scripps Contribution from: Heini Werni Peter Knippertz Harold Sodemann Andreas Stohl Francina Dominguez Huancui Hu 2016 International Atmospheric Rivers Conference 8–11 August 2016 Scripps Institution of Oceanography Objective and Outline Objective • What components of midlatitude circulation support formation and structure of atmospheric rivers? Outline • Part 1: ARs, midlatitude storm track, and cyclogenesis • Part 2: ARs, tropical moisture exports, and warm conveyor belt Objective and Outline Objective • What components of midlatitude circulation support formation and structure of atmospheric rivers? Outline • Part 1: ARs, midlatitude storm track, and cyclogenesis • Part 2: ARs, tropical moisture exports, and warm conveyor belt Mimic TPW (SSEC/Wisconsin) • Global water vapor distribution is concentrated at lower latitudes owing to warmer temperatures • Observations illustrate poleward extrusions of water vapor along “tropospheric rivers” or “atmospheric rivers” Zhu and Newell (MWR-1998) • >90% of meridional water vapor transports occurs along ARs • ARs part of midlatitude cyclones and move with storm track Climatology of Water Vapor Transport Global mean IVT 150 kg m−1 s−1 • ECMWF ERA Interim Reanalysis • Oct–Mar 99/00 to 08/09 (i.e., ten winters) • IVT calculated for isobaric layers between 1000 and 100 hPa Tropical–Extratropical Interactions Waugh and Fanutso (2003-JAS) Knippertz -
Äikesega) Kaasnevad Ohtlikud Ilmanähtused
TALLINNA TEHNIKAÜLIKOOL Eesti Mereakadeemia Merenduskeskus Veeteede lektoraat Raldo Täll RÜNKSAJUPILVEDEGA KAASNEVAD OHTLIKUD ILMANÄHTUSED LÄÄNEMEREL Lõputöö Juhendajad: Jüri Kamenik Lia Pahapill Tallinn 2016 SISUKORD SISUKORD ................................................................................................................................ 2 SÕNASTIK ................................................................................................................................ 4 SISSEJUHATUS ........................................................................................................................ 6 1. RÜNKSAJUPILVED JA ÄIKE ............................................................................................. 8 1.1. Äikese tekkimine ja areng ............................................................................................. 10 1.1.1. Äikese arengustaadiumid ........................................................................................ 11 1.2. Äikeste klassifikatsioon ................................................................................................. 14 1.2.1. Sünoptilise olukorra põhine liigitus ........................................................................ 14 1.2.2. Äikese seos tsüklonitega ......................................................................................... 15 1.2.3. Organiseerumispõhine liigitus ................................................................................ 16 2. RÜNKSAJUPILVEDEGA (ÄIKESEGA) KAASNEVAD OHTLIKUD ILMANÄHTUSED -
ESSENTIALS of METEOROLOGY (7Th Ed.) GLOSSARY
ESSENTIALS OF METEOROLOGY (7th ed.) GLOSSARY Chapter 1 Aerosols Tiny suspended solid particles (dust, smoke, etc.) or liquid droplets that enter the atmosphere from either natural or human (anthropogenic) sources, such as the burning of fossil fuels. Sulfur-containing fossil fuels, such as coal, produce sulfate aerosols. Air density The ratio of the mass of a substance to the volume occupied by it. Air density is usually expressed as g/cm3 or kg/m3. Also See Density. Air pressure The pressure exerted by the mass of air above a given point, usually expressed in millibars (mb), inches of (atmospheric mercury (Hg) or in hectopascals (hPa). pressure) Atmosphere The envelope of gases that surround a planet and are held to it by the planet's gravitational attraction. The earth's atmosphere is mainly nitrogen and oxygen. Carbon dioxide (CO2) A colorless, odorless gas whose concentration is about 0.039 percent (390 ppm) in a volume of air near sea level. It is a selective absorber of infrared radiation and, consequently, it is important in the earth's atmospheric greenhouse effect. Solid CO2 is called dry ice. Climate The accumulation of daily and seasonal weather events over a long period of time. Front The transition zone between two distinct air masses. Hurricane A tropical cyclone having winds in excess of 64 knots (74 mi/hr). Ionosphere An electrified region of the upper atmosphere where fairly large concentrations of ions and free electrons exist. Lapse rate The rate at which an atmospheric variable (usually temperature) decreases with height. (See Environmental lapse rate.) Mesosphere The atmospheric layer between the stratosphere and the thermosphere. -
Quasi-Linear Convective System Mesovorticies and Tornadoes
Quasi-Linear Convective System Mesovorticies and Tornadoes RYAN ALLISS & MATT HOFFMAN Meteorology Program, Iowa State University, Ames ABSTRACT Quasi-linear convective system are a common occurance in the spring and summer months and with them come the risk of them producing mesovorticies. These mesovorticies are small and compact and can cause isolated and concentrated areas of damage from high winds and in some cases can produce weak tornadoes. This paper analyzes how and when QLCSs and mesovorticies develop, how to identify a mesovortex using various tools from radar, and finally a look at how common is it for a QLCS to put spawn a tornado across the United States. 1. Introduction Quasi-linear convective systems, or squall lines, are a line of thunderstorms that are Supercells have always been most feared oriented linearly. Sometimes, these lines of when it has come to tornadoes and as they intense thunderstorms can feature a bowed out should be. However, quasi-linear convective systems can also cause tornadoes. Squall lines and bow echoes are also known to cause tornadoes as well as other forms of severe weather such as high winds, hail, and microbursts. These are powerful systems that can travel for hours and hundreds of miles, but the worst part is tornadoes in QLCSs are hard to forecast and can be highly dangerous for the public. Often times the supercells within the QLCS cause tornadoes to become rain wrapped, which are tornadoes that are surrounded by rain making them hard to see with the naked eye. This is why understanding QLCSs and how they can produce mesovortices that are capable of producing tornadoes is essential to forecasting these tornadic events that can be highly dangerous. -
Session 8.Pdf
MARTIN SETVÁK [email protected] CZECH HYDROMETEOROLOGICAL INSTITUTE ČESKÝ HYDROMETEOROLOGICKÝ ÚSTAV http://www.chmi.cz http://www.setvak.cz Anticipated benefits of improved temporal and spatial resolution (with focus on deep convective clouds) EUMeTrain Event Week on MTG-I Satellite, 7 – 11 November 2016 Martin Setvák version: 2016-11-11 Introduction The most significant impact of improved spatial resolution and shorter scan interval: observations (detection, monitoring, nowcasting, …) and studies of short-lived and small scale features or phenomena e.g. fires, valley fog, shallow convection, and tops of deep convective clouds (storms) – namely their overshooting tops Martin Setvák Introduction The most significant impact of improved spatial resolution and shorter scan interval: observations (detection, monitoring, nowcasting, …) and studies of short-lived and small scale features or phenomena e.g. fires, valley fog, shallow convection, and tops of deep convective clouds (storms) – namely their overshooting tops geometrical properties and characteristics (visible and near-IR bands), cloud microphysics, cloud-top brightness temperature (BT) Martin Setvák Overshooting tops definition and appearance OVERSHOOTING TOP (anvil dome, penetrating top): A domelike protrusion above a cumulonimbus anvil, representing the intrusion of an updraft through its equilibrium level (level of neutral buoyancy). It is usually a transient feature because the rising parcel's momentum acquired during its buoyant ascent carries it past the point where it is -
Storm Spotting – Solidifying the Basics PROFESSOR PAUL SIRVATKA COLLEGE of DUPAGE METEOROLOGY Focus on Anticipating and Spotting
Storm Spotting – Solidifying the Basics PROFESSOR PAUL SIRVATKA COLLEGE OF DUPAGE METEOROLOGY HTTP://WEATHER.COD.EDU Focus on Anticipating and Spotting • What do you look for? • What will you actually see? • Can you identify what is going on with the storm? Is Gilbert married? Hmmmmm….rumor has it….. Its all about the updraft! Not that easy! • Various types of storms and storm structures. • A tornado is a “big sucky • Obscuration of important thing” and underneath the features make spotting updraft is where it forms. difficult. • So find the updraft! • The closer you are to a storm the more difficult it becomes to make these identifications. Conceptual models Reality is much harder. Basic Conceptual Model Sometimes its easy! North Central Illinois, 2-28-17 (Courtesy of Matt Piechota) Other times, not so much. Reality usually is far more complicated than our perfect pictures Rain Free Base Dusty Outflow More like reality SCUD Scattered Cumulus Under Deck Sigh...wall clouds! • Wall clouds help spotters identify where the updraft of a storm is • Wall clouds may or may not be present with tornadic storms • Wall clouds may be seen with any storm with an updraft • Wall clouds may or may not be rotating • Wall clouds may or may not result in tornadoes • Wall clouds should not be reported unless there is strong and easily observable rotation noted • When a clear slot is observed, a well written or transmitted report should say as much Characteristics of a Tornadic Wall Cloud • Surface-based inflow • Rapid vertical motion (scud-sucking) • Persistent • Persistent rotation Clear Slot • The key, however, is the development of a clear slot Prof. -
Rear-Inflow Structure in Severe and Non-Severe Bow-Echoes Observed by Airborne Doppler Radar During Bamex
J5J.3 REAR-INFLOW STRUCTURE IN SEVERE AND NON-SEVERE BOW-ECHOES OBSERVED BY AIRBORNE DOPPLER RADAR DURING BAMEX David P. Jorgensen* NOAA/National Severe Storms Laboratory Norman, Oklahoma Hanne V. Murphey and Roger M. Wakimoto University of California, Los Angeles Los Angeles, California 1. INTRODUCTION Bow-echoes have been of scientific and operational interest since Fujita (1978) showed their structure in relation to surface wind damage. The Bow-Echo and Mesoscale Convective Vortex Experiment (BAMEX) focused on bow-echoes, using highly mobile platforms, in the Midwest U.S. The field exercise ran during the late spring/early summer of 2003 from a main base of operations at MidAmerica Airport near St. Louis, MO. BAMEX has two principal foci: 1) improve understanding and improve prediction of bow echoes, principally those which produce damaging surface winds and last at least 4 hours and (2) document the mesoscale processes which produce long lived mesoscale convective vortices (MCVs). More information concerning the science objectives and the observational strategies of BAMEX are contained in the scientific overview document: Fig. 1. Composite National Weather Service WSR-88D http://www.mmm.ucar.edu/bamex/science.html. A base reflectivity at 0540 UTC 10 June 2003. WSR-88D radars are indicated by the stars, profilers by the flags, more complete description of the BAMEX IOPs, solid black lines are state boundaries, light brown lines including data set availability, can be found on the are county boundaries, blue lines are interstate University Corporation for Atmospheric highways. Flight tracks for the two turbo prop aircraft are Research/Joint Office for Science Support red lines (NRL P-3) and magenta lines (NOAA P-3). -
Hurricane Sea Surface Inflow Angle and an Observation-Based
NOVEMBER 2012 Z H A N G A N D U H L H O R N 3587 Hurricane Sea Surface Inflow Angle and an Observation-Based Parametric Model JUN A. ZHANG Rosenstiel School of Marine and Atmospheric Science, University of Miami, and NOAA/AOML/Hurricane Research Division, Miami, Florida ERIC W. UHLHORN NOAA/AOML/Hurricane Research Division, Miami, Florida (Manuscript received 22 November 2011, in final form 2 May 2012) ABSTRACT This study presents an analysis of near-surface (10 m) inflow angles using wind vector data from over 1600 quality-controlled global positioning system dropwindsondes deployed by aircraft on 187 flights into 18 hurricanes. The mean inflow angle in hurricanes is found to be 222.6862.28 (95% confidence). Composite analysis results indicate little dependence of storm-relative axisymmetric inflow angle on local surface wind speed, and a weak but statistically significant dependence on the radial distance from the storm center. A small, but statistically significant dependence of the axisymmetric inflow angle on storm intensity is also found, especially well outside the eyewall. By compositing observations according to radial and azimuthal location relative to storm motion direction, significant inflow angle asymmetries are found to depend on storm motion speed, although a large amount of unexplained variability remains. Generally, the largest storm- 2 relative inflow angles (,2508) are found in the fastest-moving storms (.8ms 1) at large radii (.8 times the radius of maximum wind) in the right-front storm quadrant, while the smallest inflow angles (.2108) are found in the fastest-moving storms in the left-rear quadrant. -
On the Dynamics of Tropical Cyclone Structural Changes
Quart. J. R. Met. SOC. (1984), 110, pp. 723-745 551.515.21 On the dynamics of tropical cyclone structural changes By GREG. J. HOLLAND. and ROBERT T. MERRILL Department of Atmospheric Science, Colorado State University (Received 16 March 1983; revised 17 January 1%) SUMMARY Tropical cyclone structural change is separated into three modes: intensity, strength and size. The possible physical mechanisms behind these three modes are examined using observations .in the Australiadsouth-west Pacific region and an axisymmetric diagnostic model. We propose that, though dependent on moist convection and other internal processes, the ultimate intensity, strength or sue of a cyclone is regulated by interactions with its environment. Possible mechanisms whereby these interactions occur are described. 1. INTRODUCTION Most of the work on tropical cyclone development in past years has been concerned with ‘genesis’ and ‘intensification’, even though no precise definition exists for either term. The result has been confusion in interpreting some aspects of cyclone structural changes, and the neglect of other aspects altogether. More precise and comprehensive interpretations are possible if we separate tropical cyclone structural changes into three modes: intensity, strength, and size (Merrill and Gray 1983). These are illustrated in Fig. 1 as changes from an initial tangential wind profile. ‘Intensity’ is defined by the maximum wind, or by the central pressure if no maximum wind data are available, and has received the most attention in the literature. ‘Strength’ is defined by the average relative angular momentum of the low-level inner circulation (inside 300 km radius). ‘Size’ is defined by the axisymmetric extent of gale force winds, or by the radius of the outermost closed isobar.