The Characteristics and Structure of Extra-Tropical Cyclones in a Warmer Climate Victoria A
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Low Level Wind Shear: Invisible Enemy to Pilots
Low Level Wind Shear: Invisible Enemy To Pilots On the afternoon of August 2, 1985, a landmark aircraft accident occurred at the Dallas/Fort Worth (DFW) airport. The tragic accident, which killed 137 of the 163 passengers on board Delta Airlines Flight 191, was responsible for making “wind shear” a more commonly known weather phenomenon and implementing many new changes with regard to wind shear detection (Ref. 1). On that day, thunderstorms were in the area of approach to runway 17L at the DFW International Airport, with a thunderstorm rain shaft right in the path of final approach. The crew decided to proceed through the thunderstorm, which turned out to be a critical error. Shortly after entering the storm, turbulence increased and the L1011 aircraft encountered a 26 knot headwind. Just as suddenly, the wind switched to a 46 knot tailwind, resulting in a loss of 72 knots of airspeed. This much of an airspeed loss on final approach, when the jet was only 800 feet above the surface, was unrecoverable and the aircraft eventually crashed short of the runway (Ref. 1). The sudden change in wind speed and direction that the aircraft encountered is called wind shear. Wind shear can occur at many different levels of the atmosphere, however it is most dangerous at the low levels, as a sudden loss of airspeed and altitude can occur. Plenty of altitude is normally needed to recover from the stall produced by the abrupt change in wind speed and direction, which is why pilots need to be aware of the hazards and mitigation of low-level wind shear. -
Coping with the Long Term
Coping with the Long Term An Empirical Analysis of Time Perspectives, Time Orientations, and Temporal Uncertainty in Forestry Coping with the Long Term An Empirical Analysis of Time Perspectives, Time Orientations, and Temporal Uncertainty in Forestry Marjanke Alberttine Hoogstra Marjanke A. Hoogstra Coping with the Long Term An Empirical Analysis of Time Perspectives, Time Orientations, and Temporal Uncertainty in Forestry Marjanke Alberttine Hoogstra Promotoren: Prof. dr. H. (Heiner) Schanz Hoogleraar Märkte der Wald- und Holzwirtschaft Institut für Forst- und Umweltpolitik Albert-Ludwigs-Universität Freiburg, Duitsland Prof. dr. B.J.M (Bas) Arts Hoogleraar Bos- en Natuurbeleid Leerstoelgroep Bos- en Natuurbeleid Wageningen Universiteit, Nederland Promotiecommissie: Prof. dr. ir. G.M.J. Mohren (Wageningen Universiteit, Nederland) Prof. dr. G. Oesten (Albert-Ludwigs-Universität Freiburg, Duitsland) Dr. M. Pregernig (Universität für Bodenkultur Wien, Oostenrijk) Prof. dr. B.J. Thorsen (Københavns Universitet, Denemarken) Dit onderzoek is uitgevoerd binnen Mansholt Graduate School of Social Sciences Coping with the Long Term An Empirical Analysis of Time Perspectives, Time Orientations, and Temporal Uncertainty in Forestry Marjanke Alberttine Hoogstra Proefschrift ter verkrijging van de graad van doctor op gezag van de rector magnificus van Wageningen Universiteit, Prof. dr. M.J. Kropff, in het openbaar te verdedigen op dinsdag 16 december 2008 des middags te half twee in de Aula Hoogstra, M.A. [2008] Coping with the Long Term - An Empirical Analysis of Time Perspectives, Time Orientations, and Temporal Uncertainty in Forestry. PhD thesis Forest and Nature Conservation Policy Group, Wageningen University, Wageningen, the Netherlands. With references - with summary in Dutch and in English. ISBN 978-90-8585-242-1 The Road goes ever on and on Down from the door where it began. -
NWS Unified Surface Analysis Manual
Unified Surface Analysis Manual Weather Prediction Center Ocean Prediction Center National Hurricane Center Honolulu Forecast Office November 21, 2013 Table of Contents Chapter 1: Surface Analysis – Its History at the Analysis Centers…………….3 Chapter 2: Datasets available for creation of the Unified Analysis………...…..5 Chapter 3: The Unified Surface Analysis and related features.……….……….19 Chapter 4: Creation/Merging of the Unified Surface Analysis………….……..24 Chapter 5: Bibliography………………………………………………….…….30 Appendix A: Unified Graphics Legend showing Ocean Center symbols.….…33 2 Chapter 1: Surface Analysis – Its History at the Analysis Centers 1. INTRODUCTION Since 1942, surface analyses produced by several different offices within the U.S. Weather Bureau (USWB) and the National Oceanic and Atmospheric Administration’s (NOAA’s) National Weather Service (NWS) were generally based on the Norwegian Cyclone Model (Bjerknes 1919) over land, and in recent decades, the Shapiro-Keyser Model over the mid-latitudes of the ocean. The graphic below shows a typical evolution according to both models of cyclone development. Conceptual models of cyclone evolution showing lower-tropospheric (e.g., 850-hPa) geopotential height and fronts (top), and lower-tropospheric potential temperature (bottom). (a) Norwegian cyclone model: (I) incipient frontal cyclone, (II) and (III) narrowing warm sector, (IV) occlusion; (b) Shapiro–Keyser cyclone model: (I) incipient frontal cyclone, (II) frontal fracture, (III) frontal T-bone and bent-back front, (IV) frontal T-bone and warm seclusion. Panel (b) is adapted from Shapiro and Keyser (1990) , their FIG. 10.27 ) to enhance the zonal elongation of the cyclone and fronts and to reflect the continued existence of the frontal T-bone in stage IV. -
Effect of Intense Wind Shear Across the Inversion on Stratocumulus Clouds
GEOPHYSICAL RESEARCH LETTERS, VOL. 35, L15814, doi:10.1029/2008GL033865, 2008 Click Here for Full Article Effect of intense wind shear across the inversion on stratocumulus clouds Shouping Wang,1 Jean-Christophe Golaz,2 and Qing Wang3 Received 17 March 2008; revised 12 May 2008; accepted 9 July 2008; published 13 August 2008. [1] A large-eddy simulation model is used to examine the mental difference between the strongly sheared and the impact of the intense cross-inversion wind shear on the shear-free stratocumulus convection? stratocumulus cloud structure. The wind shear enhanced [3] A low-level jet near the top of the CTBL is frequently entrainment mixing effectively reduces the cloud water and observed off the California central coast during summer due thickens the inversion layer. It leads to a reduction of the to the topography and land-sea contrast [Strom et al., 2001; turbulence kinetic energy (TKE) production in the cloud Rahn and Parish, 2007]. Figures 1a–1c show soundings layer due to the weakened cloud-top radiative cooling and taken in an aircraft flight in the field experiment of the formation of a turbulent and cloud free sublayer within Development and Evolution of Coastal Stratocumulus the inversion. The thickness of the sublayer increases with the [Kalogiros and Wang, 2002]. The wind speed reaches enhanced wind shear intensity. Under the condition of a maximum 18 msÀ1 just below the base of the inversion; weaker inversion, the enhanced shear mixing within the decreases by 8 msÀ1 across the sharp inversion; and then inversion layer even lowers the cloud-top height and reduces reduces further but more gradually to 7 m sÀ1 at about 730 m. -
Geography 5942 Synoptic Meteorology: Severe Storm Forecasting Spring 2017
Geography 5942 Synoptic Meteorology: Severe Storm Forecasting Spring 2017 Instructor: Jeff Rogers, Prof. Emeritus Office: Derby 1048 e-mail: [email protected] Phone: 292-0148 Office Hours: Tu, Th 2:10-3:30p.m. Course Prerequisites: Geography 5941, Physics 1250 Class Meetings: Tu, Th, 3:55 – 5:15 p.m. in Db 0140 Access to course lecture materials: http://carmen.osu.edu. Suggested Textbook: Mesoscale Meteorology in Midlatitudes by Paul Markowski and YvetteRichardson. Order through websites such as Amazon, it has not been ordered for the OSU bookstores. Course Objectives: The aim of the course is to introduce students to the methods of analysis and techniques of forecasting thunderstorms and severe weather. The course is divided into five components: 1. Introductory overview of the climatology of severe weather and basic cloud physics, 2. The meteorological ingredients for severe weather and the forecasting of severe weather, 3. Weather radar and satellites as tools in severe weather analysis, 4. Convection and the characteristics and features of mesoscale storms, and 5. Practice in severe weather forecasting through a series of exercises and assignments. The initial course section focuses on the ingredients of, and synoptic setting in which, severe storms develop. The role of instability, moisture, low-level and upper-level synoptic scale uplift will be described as will means by which forecasters identify and categorize the importance of each of these. The subsequent segment of the course describes the ways in which weather radar and geostationary satellite imagery are used in the analysis and forecasting of severe weather. Some theory of radar and satellite imagery is covered but the emphasis is on the usage of these materials in preparing forecasts and in trying to understand the conditions that are ideal for severe weather development. -
EGU2014-6135, 2014 EGU General Assembly 2014 © Author(S) 2014
Geophysical Research Abstracts Vol. 16, EGU2014-6135, 2014 EGU General Assembly 2014 © Author(s) 2014. CC Attribution 3.0 License. Dynamic aspects of windstorm Kyrill (January 2007) Patrick Ludwig (1), Joaquim G. Pinto (1,2), Simona A. Hoepp (1), Andreas H. Fink (3), and Suzanne L. Gray (2) (1) Institute for Geophysics and Meteorology, University of Cologne, Cologne, Germany ([email protected]), (2) Department of Meteorology, University of Reading, Reading, United Kingdom, (3) Institute for Meteorology and Climate Research, Karlsruhe Institute of Technology (KIT), Karlsruhe, Germany Several dynamical and mesoscale aspects concerning severe windstorm Kyrill (January 2007) are analysed by results of high-resolution simulations with the regional climate model (RCM) COSMO-CLM. After explosive cyclogenesis south of Greenland takes place while crossing a very intense upper-level jet stream, Kyrill underwent secondary cyclogenesis over the North Atlantic Ocean just west of the British Isles. The secondary cyclogenesis (Kyrill II), was located on the occlusion front of the mature cyclone (Kyrill I), which is very unusual compared to typical frontal cyclogenesis generally occurring along the trailing cold fronts of existing cyclones. The mechanisms of secondary cyclogenesis are investigated based on moderate-resolution (0.0625◦ grid spacing) RCM simulations. The formation of Kyrill II along the occlusion front follows common mechanism for secondary cyclogenesis like breaking up of a local, low tropospheric PV strip along the front and diabatic heating with associated development of a vertical extended PV tower. Kyrill II propagated further towards Europe, and its development was favoured by a split jet structure aloft the surface cyclone, which maintained the deep core pressure (around 961 - 965 hPa) for at least 36 hours. -
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. -
Downloaded 10/05/21 02:25 PM UTC 3568 JOURNAL of the ATMOSPHERIC SCIENCES VOLUME 74
NOVEMBER 2017 B Ü ELER AND PFAHL 3567 Potential Vorticity Diagnostics to Quantify Effects of Latent Heating in Extratropical Cyclones. Part I: Methodology DOMINIK BÜELER AND STEPHAN PFAHL Institute for Atmospheric and Climate Science, ETH Zurich,€ Zurich, Switzerland (Manuscript received 9 February 2017, in final form 31 July 2017) ABSTRACT Extratropical cyclones develop because of baroclinic instability, but their intensification is often sub- stantially amplified by diabatic processes, most importantly, latent heating (LH) through cloud formation. Although this amplification is well understood for individual cyclones, there is still need for a systematic and quantitative investigation of how LH affects cyclone intensification in different, particularly warmer and moister, climates. For this purpose, the authors introduce a simple diagnostic to quantify the contribution of LH to cyclone intensification within the potential vorticity (PV) framework. The two leading terms in the PV tendency equation, diabatic PV modification and vertical advection, are used to derive a diagnostic equation to explicitly calculate the fraction of a cyclone’s positive lower-tropospheric PV anomaly caused by LH. The strength of this anomaly is strongly coupled to cyclone intensity and the associated impacts in terms of surface weather. To evaluate the performance of the diagnostic, sensitivity simulations of 12 Northern Hemisphere cyclones with artificially modified LH are carried out with a numerical weather prediction model. Based on these simulations, it is demonstrated that the PV diagnostic captures the mean sensitivity of the cyclones’ PV structure to LH as well as parts of the strong case-to-case variability. The simple and versatile PV diagnostic will be the basis for future climatological studies of LH effects on cyclone intensification. -
Severe Weather Forecasting Tip Sheet: WFO Louisville
Severe Weather Forecasting Tip Sheet: WFO Louisville Vertical Wind Shear & SRH Tornadic Supercells 0-6 km bulk shear > 40 kts – supercells Unstable warm sector air mass, with well-defined warm and cold fronts (i.e., strong extratropical cyclone) 0-6 km bulk shear 20-35 kts – organized multicells Strong mid and upper-level jet observed to dive southward into upper-level shortwave trough, then 0-6 km bulk shear < 10-20 kts – disorganized multicells rapidly exit the trough and cross into the warm sector air mass. 0-8 km bulk shear > 52 kts – long-lived supercells Pronounced upper-level divergence occurs on the nose and exit region of the jet. 0-3 km bulk shear > 30-40 kts – bowing thunderstorms A low-level jet forms in response to upper-level jet, which increases northward flux of moisture. SRH Intense northwest-southwest upper-level flow/strong southerly low-level flow creates a wind profile which 0-3 km SRH > 150 m2 s-2 = updraft rotation becomes more likely 2 -2 is very conducive for supercell development. Storms often exhibit rapid development along cold front, 0-3 km SRH > 300-400 m s = rotating updrafts and supercell development likely dryline, or pre-frontal convergence axis, and then move east into warm sector. BOTH 2 -2 Most intense tornadic supercells often occur in close proximity to where upper-level jet intersects low- 0-6 km shear < 35 kts with 0-3 km SRH > 150 m s – brief rotation but not persistent level jet, although tornadic supercells can occur north and south of upper jet as well. -
Severe Storm Xynthia Over Southwestern and Western Europe
Severe Storm Xynthia over southwestern and western Europe A severe storm named “Xynthia” affected Portugal, Spain, Switzerland, France, parts of south-east England, Belgium, the Netherlands, Luxembourg, Germany and Austria. Strong gusts on 27-28 February 2010 caused extended damage on traffic routes, electrical power outage, destruction due to flooding at the French Atlantic coast and more than 60 losses of lives. Most of the damage was in France and western Germany. The track of this storm and its rapid development were outstanding, but the magnitude of the gusts was comparable to other violent storms in the past. Synoptical development and weather conditions Xynthia arose from an initially shallow low pressure system which formed over the subtropical sea area south of the Azores Islands on Friday, 26 February 2010. The southward flow of colder air masses in the upper air caused the deepening of a broad trough over the central and eastern North Atlantic. A shortwave trough within this broader system and a high temperature difference between extremely warm air over Africa and colder air over the eastern Atlantic caused a strong cyclogenesis of Xynthia. On Saturday, February 27, the cyclone moved northeastwards over Portugal and the Bay of Biscay to the westernmost areas of France and intensified very rapidly to a core pressure of about 967 hPa around midnight which means a deepening of about 20 hPa within 24 hours (Fig. 1-3). During the following three days it began weakening and moved further northeastwards along the coastline of northern France and the North Sea, and then it crossed the southern Baltic Sea to southern Finland until March 3. -
Orkantief Sabine Löst Am 09./10. Februar 2020 Eine Schwere Sturmlage Über Europa Aus
Abteilung Klimaüberwachung Orkantief Sabine löst am 09./10. Februar 2020 eine schwere Sturmlage über Europa aus Autor(inn)en: Susanne Haeseler, Peter Bissolli, Jan Dassler, Volker Zins, Andrea Kreis Stand: 13.02.2020 Zusammenfassung Orkantief SABINE (in Westeuropa CIARA und in Norwegen ELSA benannt) löste am 9./10. Februar 2020 deutschlandweit Sturmböen bis Orkanstärke (12 Bft) aus. Die höchste Böe meldete der Feldberg im Schwarzwald am 10. Januar mit 49,1 m/s bzw. 177 km/h. Der Kern des Orkantiefs zog vom Atlantik kommend über Schottland nach Norwegen, wobei der Kerndruck zeitweise unter 945 hPa lag. Zwischen Nord- und Südeuropa bestanden Luftdruckunterschiede von etwa 80 hPa. Das dadurch generierte Sturmfeld erfasste weite Teile West-, Mittel- und Nordeuropas. In Deutschland war der Sturm, der sich von der Nordsee in Richtung Alpen ausweitete, von teils kräftigen Schauern und Gewittern begleitet. An der Nordsee gab es vom 10. bis 12. Januar mehrere teils schwere Sturmfluten (Abb. 1 und 4). Die extreme Sturmlage war schon Tage vorher angekündigt und es wurde von Tätigkeiten im Freien sowie Reisen während dieser Zeit abgeraten. Sport- und Musikveranstaltungen wurden vorsichtshalber abgesagt. Am 9./10. Februar stellte die Bahn in Deutschland den Verkehr zeitweise ein. Flüge und Fährverbindungen fielen aus. Viele Schulen und Kindergärten blieben am 10. Februar geschlossen. Der Sturm ließ in den betroffenen Ländern Bäume umstürzen und deckte Hausdächer ab. Auf den Britischen Inseln kam es zu Überschwemmungen. In einigen Regionen (auch in Deutschland) gab es Stromausfälle. Abbildung 1: Sturmflut am Weststrand von Norderney. Die Wellen laufen bis auf die Promenade, die als Küstenschutz dient, herauf. -
Synoptic Meteorology
Lecture Notes on Synoptic Meteorology For Integrated Meteorological Training Course By Dr. Prakash Khare Scientist E India Meteorological Department Meteorological Training Institute Pashan,Pune-8 186 IMTC SYLLABUS OF SYNOPTIC METEOROLOGY (FOR DIRECT RECRUITED S.A’S OF IMD) Theory (25 Periods) ❖ Scales of weather systems; Network of Observatories; Surface, upper air; special observations (satellite, radar, aircraft etc.); analysis of fields of meteorological elements on synoptic charts; Vertical time / cross sections and their analysis. ❖ Wind and pressure analysis: Isobars on level surface and contours on constant pressure surface. Isotherms, thickness field; examples of geostrophic, gradient and thermal winds: slope of pressure system, streamline and Isotachs analysis. ❖ Western disturbance and its structure and associated weather, Waves in mid-latitude westerlies. ❖ Thunderstorm and severe local storm, synoptic conditions favourable for thunderstorm, concepts of triggering mechanism, conditional instability; Norwesters, dust storm, hail storm. Squall, tornado, microburst/cloudburst, landslide. ❖ Indian summer monsoon; S.W. Monsoon onset: semi permanent systems, Active and break monsoon, Monsoon depressions: MTC; Offshore troughs/vortices. Influence of extra tropical troughs and typhoons in northwest Pacific; withdrawal of S.W. Monsoon, Northeast monsoon, ❖ Tropical Cyclone: Life cycle, vertical and horizontal structure of TC, Its movement and intensification. Weather associated with TC. Easterly wave and its structure and associated weather. ❖ Jet Streams – WMO definition of Jet stream, different jet streams around the globe, Jet streams and weather ❖ Meso-scale meteorology, sea and land breezes, mountain/valley winds, mountain wave. ❖ Short range weather forecasting (Elementary ideas only); persistence, climatology and steering methods, movement and development of synoptic scale systems; Analogue techniques- prediction of individual weather elements, visibility, surface and upper level winds, convective phenomena.