Outer Tropical Cyclone Rainbands Associated with Typhoon Matmo (2014)

Total Page:16

File Type:pdf, Size:1020Kb

Outer Tropical Cyclone Rainbands Associated with Typhoon Matmo (2014) JULY 2020 Y U E T A L . 2935 Outer Tropical Cyclone Rainbands Associated with Typhoon Matmo (2014) CHENG-KU YU,LIN-WEN CHENG,CHUN-CHIEH WU, AND CHIA-LUN TSAI Department of Atmospheric Sciences, National Taiwan University, Taipei, Taiwan (Manuscript received 18 February 2020, in final form 14 April 2020) ABSTRACT On 23 July 2014, a commercial aircraft (GE222) crashed near the Ma-Gong Airport on Penghu Island off the southwestern coast of Taiwan as it struggled to land in the stormy weather that was caused by the outer tropical cyclone rainbands (OTCRs) of Typhoon Matmo. This study aims to document the detailed aspects of airflow and precipitation of OTCRs through high-resolution radar and surface observations and to identify how these observed structures contribute to aviation weather hazards. Analyses indicate that the weather at the airport was significantly influenced by the passage of three OTCRs (R1, R2, and R3), and these rainbands share common characteristics of squall-line-like airflow and precipitation structures. As GE222 descended to approach the runway and flew immediately behind and roughly parallel to the leading edge of R3, the aircraft encountered the heaviest precipitation of the rainband and the prominent crosswind that was a manifestation of the rear-to-front flow generated locally by the rainband. The heavy rain–induced poor visibility and the occurrence of strong crosswinds were primary weather hazards affecting this flight event. Momentum budget analyses suggest that the frontward pressure gradient force provided by the near-surface, convectively gen- erated mesohigh played a major role in driving the low-level rear-to-front flow inside the band. The results from the present study imply that closely monitoring convective activities in the outer regions of tropical cyclones and their potential transformation into squall-line-like storms is crucial to complement the routine aviation alert of severe weather under the influence of tropical cyclones. 1. Introduction traffic and airport operation in areas where TCs pass by (Breslin 2016; Goodman and Small Griswold 2019). A The impact of weather on the operation and safety of mature TC is an approximately circular, strong cyclonic aviation is a worldwide issue (Humphreys 1930; WMO vortex, and its associated precipitation is typically 1989). Although the direct causes of accidents are most characterized by an organized, banded feature called commonly related to human error, weather is often a pri- ‘‘rainbands’’ or ‘‘spiral bands’’ (i.e., tropical cyclone mary contributing factor for aviation accidents (Helmreich rainbands, TCRs) (Senn and Hiser 1959; Willoughby 1997; Kulesa 2003). A number of weather phenomena, et al. 1984; Marks 2003; Yu and Chen 2011). It is well such as mountain waves and thunderstorms, have been recognized that the inner core, which is approximately shown to produce hazardous circumstances that may lead within 100–200 km or 2–3 times the radius of maximum to fatal aircraft accidents (Wurtele 1970; Fujita and Byers wind (RMW) from the TC center, is the most hazardous 1977; Wilson et al. 1984; Smith 1986; Haddad and Park region for TCs because it contains the most intense 2010; Keller et al. 2015). In particular, weather-induced swirling winds and eyewall convection (Anthes 1982; intense rainfall, high wind shear or strong downdrafts at Willoughby 1988; Rozoff et al. 2006; Wang 2009; Houze low altitudes near airports can significantly affect the air- 2010). Currently, both TC location and movement can craft takeoff/landing safety (Kessler 1985). The effective be monitored and predicted effectively by Doppler ra- documentation and prediction of aviation weather hazards dar and satellite observation systems and numerical are thus critically important for the prevention of aviation models. It is thus practically possible for meteorological accidents (Chun et al. 2017). forecasters to issue an appropriate, lead-time warning Tropical cyclones (TCs) are not only one of the most for the approach of hazardous, inner-core circulations of life-threatening and destructive natural phenomena on TCs. This weather alert usually allows aviation con- Earth but are also well known to strongly affect air trollers to direct aircraft to a safer space or hold air- planes on the ground over a sufficient time period Corresponding author: Cheng-Ku Yu, [email protected] beforehand (Goodman and Small Griswold 2019). DOI: 10.1175/MWR-D-20-0054.1 Ó 2020 American Meteorological Society. For information regarding reuse of this content and general copyright information, consult the AMS Copyright Policy (www.ametsoc.org/PUBSReuseLicenses). Unauthenticated | Downloaded 09/24/21 06:41 PM UTC 2936 MONTHLY WEATHER REVIEW VOLUME 148 In contrast to the inner core of TCs, both convective On 23 July 2014, a commercial aircraft (model: phenomena in the outer region of TCs and their po- ATR72–212A) with 2 pilots, 2 cabin crew, and 54 pas- tential impacts on aviation activities have not received sengers on board executed regular public transport service much attention. The outer vicinity of TCs exhibits (flight number GE222) from Kaohsiung (KH) International weaker swirling winds, and the moist convection in this Airport located in southern Taiwan to Ma-Gong (MG) region is not significantly filamented or constrained by Airport on Penghu Island off the southwestern coast of the inner-core vortex (Rozoff et al. 2006). However, the Taiwan (Fig. 1). The aircraft crashed near MG Airport outer region of TCs tends to possess larger convective as it struggled to land in the stormy weather caused by available potential energy (CAPE) and lower humidity the OTCRs of Typhoon Matmo (2014). Unfortunately, 4 than the inner-core environment (Frank 1977; Bogner flight crew and 44 passengers were killed in this airplane et al. 2000; Yu and Chen 2011; Molinari et al. 2012). accident. As noted in the investigation report of this These environmental conditions facilitate intense con- accident by the Taiwan Aviation Safety Council (TASC vection, making the structural characteristics of outer 2016), during the landing of the aircraft, meteorological TCRs (OTCRs) resemble severe thunderstorms such as conditions near MG Airport, including thunderstorm squall lines (Houze 2010; Eastin et al. 2012; Yu and activities, heavy rain and significant changes in visibility, Chen 2011; Yu and Tsai 2013; Tang et al. 2014; Moon wind direction and speed, were among the contributing and Nolan 2015). More recently, a comprehensive in- factors for the cause of the aircraft incident. The ob- vestigation of OTCRs by Yu et al. (2018, hereafter jective of this study is to use various available observa- YU18) analyzed a large set of 50 rainband cases tions to document the detailed aspects of the airflow and through dual-Doppler observations and identified a precipitation of OTCRs related to this accident and to frequent similarity (58%, 29 rainband cases) between identify how these mesoscale structural characteristics OTCRs and squall lines. These squall-line-like OTCRs contribute to the occurrence of hazardous weather are generally characterized by convective precipita- conditions that may impact aviation safety. Over the tion, an obvious convergence zone between the band- accident area, there is relatively good, persistent cov- relative rear-to-front flow and front-to-rear flow at low erage of temporal and spatial high-resolution measure- levels and a surface cold pool signature. The processes ments from two ground-based Doppler radars at Chi-Gu responsible for the initiation of OTCRs have been (CG) and MG Airport (see Fig. 1). These Doppler radar partially addressed in the literature. Limited research observations provide an unparalleled depiction of the evidence suggests that the origin of OTCRs is probably finescale rainband features of the OTCRs and their re- related to different scenarios and forcings, such as the lationship with the aerial incident. outer propagation of inner-core convective activities, the intensification of convectively generated cold pools 2. Data and the potential interaction of inner-core vortex cir- culation with its outer environmental flow (Willoughby As described in the Introduction section, the primary et al. 1984; Yu and Cheng 2014; Li et al. 2017; Yu et al. datasets used to document the detailed features of the 2019; Li et al. 2019). airflow and precipitation of Matmo’s OTCRs and their Unlike the inner-core, hazardous region with a connection to the occurrence of aviation weather haz- quasi-circular geometry that is well recognized and ards are provided by two ground-based Doppler radars can be appropriately located given a known TC cen- available in the surrounding area of the flight accident ter, our awareness and understanding of aviation (locations in Fig. 1). One is the S-band (10 cm) opera- weather hazards caused by OTCRs is relatively less tional Doppler radar of the Central Weather Bureau at adequate. In particular, the detailed aspects of OTCR- CG located at the coast of southwestern Taiwan, ap- produced severe weather conditions and how they af- proximately 65 km southeast of Penghu Island (Fig. 1a). fect aircraft safety have been neither described nor The other is the C-band (5 cm) operational Doppler elaborated in the literature. It should be noted that radar of the Weather Wing of the Chinese Air force at turbulence associated with OTCRs can lead to very MG Airport. As indicated in Fig. 1b, this radar site is rough flights, which are well recognized by pilots and located ;1 km immediately adjacent to the eastern flank scientists who flew into TCs (Chapter 10, Houze 2014). of the runway of MG Airport. MG Airport has a single Schaefer et al. (1992) noted that moderate turbulence runway oriented north-northeast to south-southwest, is frequently located in transverse waves emanating designated R20 and R02, respectively. The altitudes of from the OTCRs. It is possible that the impacts on the CG and MG radar sites are 38 and 48 m MSL, re- aviation for both the inner and outer regions of TCs spectively.
Recommended publications
  • Warm-Core Formation in Tropical Storm Humberto (2001)
    APRIL 2012 D O L L I N G A N D B A R N E S 1177 Warm-Core Formation in Tropical Storm Humberto (2001) KLAUS DOLLING AND GARY M. BARNES University of Hawaii at Manoa, Honolulu, Hawaii (Manuscript received 27 July 2011, in final form 18 October 2011) ABSTRACT At 0600 UTC 22 September 2001, Humberto was a tropical depression with a minimum central pressure of 1010 hPa. Twelve hours later, when the first global positioning system dropwindsondes (GPS sondes) were jettisoned, Humberto’s minimum central pressure was 1000 hPa and it had attained tropical storm strength. Thirty GPS sondes, radar from the WP-3D, and in situ aircraft measurements are utilized to observe ther- modynamic structures in Humberto and their relationship to stratiform and convective elements during the early stage of the formation of an eye. The analysis of Tropical Storm Humberto offers a new view of the pre-wind-induced surface heat exchange (pre-WISHE) stage of tropical cyclone evolution. Humberto contained a mesoscale convective vortex (MCV) similar to observations of other developing tropical systems. The MCV advects the exhaust from deep con- vection in the form of an anvil cyclonically over the low-level circulation center. On the trailing edge of the anvil an area of mesoscale descent induces dry adiabatic warming in the lower troposphere. The nascent warm core at low levels causes the initial drop in pressure at the surface and acts to cap the boundary layer (BL). As BL air flows into the nascent eye, the energy content increases until the energy is released from under the cap on the down shear side of the warm core in the form of vigorous cumulonimbi, which become the nascent eyewall.
    [Show full text]
  • Mesoscale Convective Complexes: an Overview by Harold Reynolds a Report Submitted in Conformity with the Requirements for the De
    Mesoscale Convective Complexes: An Overview By Harold Reynolds A report submitted in conformity with the requirements for the degree of Master of Science in the University of Toronto © Harold Reynolds 1990 Table of Contents 1. What is a Mesoscale Convective Complex?........................................................................................ 3 2. Why Study Mesoscale Convective Complexes?..................................................................................3 3. The Internal Structure and Life Cycle of an MCC...............................................................................4 3.1 Introduction.................................................................................................................................... 4 3.2 Genesis........................................................................................................................................... 5 3.3 Growth............................................................................................................................................6 3.4 Maturity and Decay........................................................................................................................ 7 3.5 Heat and Moisture Budgets............................................................................................................ 8 4. Precipitation......................................................................................................................................... 8 5. Mesoscale Warm-Core Vortices.......................................................................................................
    [Show full text]
  • Chapter 3 Mesoscale Processes and Severe Convective Weather
    CHAPTER 3 JOHNSON AND MAPES Chapter 3 Mesoscale Processes and Severe Convective Weather RICHARD H. JOHNSON Department of Atmospheric Science. Colorado State University, Fort Collins, Colorado BRIAN E. MAPES CIRESICDC, University of Colorado, Boulder, Colorado REVIEW PANEL: David B. Parsons (Chair), K. Emanuel, J. M. Fritsch, M. Weisman, D.-L. Zhang 3.1. Introduction tion, mesoscale phenomena occur on horizontal scales between ten and several hundred kilometers. This Severe convective weather events-tornadoes, hail­ range generally encompasses motions for which both storms, high winds, flash floods-are inherently mesoscale ageostrophic advections and Coriolis effects are im­ phenomena. While the large-scale flow establishes envi­ portant (Emanuel 1986). In general, we apply such a ronmental conditions favorable for severe weather, pro­ definition here; however, strict application is difficult cesses on the mesoscale initiate such storms, affect their since so many mesoscale phenomena are "multiscale." evolution, and influence their environment. A rich variety For example, a -100-km-Iong gust front can be less of mesocale processes are involved in severe weather, than -1 km across. The triggering of a storm by the ranging from environmental preconditioning to storm initi­ collision of gust fronts can actually occur on a ation to feedback of convection on the environment. In the -lOO-m scale (the microscale). Nevertheless, we will space available, it is not possible to treat all of these treat this overall process (and others similar to it) as processes in detail. Rather, we will introduce s~veral mesoscale since gust fronts are generally regarded as general classifications of mesoscale processes relatmg to mesoscale phenomena.
    [Show full text]
  • Synoptic Conditions Favorable for the Formation of the 15 July 1995 Southeastern Canada/Northeastern U.S
    SYNOPTIC CONDITIONS FAVORABLE FOR THE FORMATION OF THE 15 JULY 1995 SOUTHEASTERN CANADA/NORTHEASTERN U.S. DERECHO EVENT Mace L. Bentley Climatology Research Laboratory Department of Geography The University of Georgia Athens, Georgia Abstract On 15 July 1995, a derecho-producing mesoscale convective system inflicted considerable damage through southeastern Canada and the northeastern U.S. The synoptic-scale environ­ ment that precluded and persisted during this event is examined \ using swface and upper-air observations, satellite imagery v""--- and numerical model data. Evidence suggests that low-level ~~- - . -,.~ .... moisture inflow and forcing were major factors in initiating \ .-..... ~".... ". and sustaining this progressive warm season derecho event. : "?-.,. ~.:"... Favorable upper-level dynamics produced by jet streak induced Kingston. Ontario circulations were also found over the region. Products from ..------------.:t i the Eta model run initialized 12 hours prior to the event were ". used in the study to fill in between the 0000 UTC and 1200 UTC upper-air sounding times. Manipulation of these data sets was accomplished using GEMPAK 5.2.1. Calculation of 850 hPa moisture transport vectors andfrontogenesis were found to be particularly useful in determining the derecho producing mesoscale convective system's genesis and propagation regions. Future investiga­ tions of these systems should employ these techniques in order to assess their forecast applications. Fig. 1. Approximate track of the DMCS cloud shield on 15 July 1995. 1. Introduction In the early morning hours of 15 July 1995, a derecho­ producing mesoscale convective system (hereafter, DMCS) moved from southern Canada through the northeastern United States (Fig. 1). Widespread wind damage was reported through­ out the Northeast.
    [Show full text]
  • Some Basic Elements of Thunderstorm Forecasting
    (] NOAA TECHNICAL MEMORANDUM NWS CR-69 SOME BASIC ELEMENTS OF THUNDERSTORM FORECASTING Richard P. McNulty National Weather Service Forecast Office Topeka, Kansas May 1983 UNITED STATES I Nalion•l Oceanic and I National Weather DEPARTMENT OF COMMERCE Almospheric Adminislralion Service Malcolm Baldrige. Secretary John V. Byrne, Adm1mstrator Richard E. Hallgren. Director SOME BASIC ELEMENTS OF THUNDERSTORM FORECASTING 1. INTRODUCTION () Convective weather phenomena occupy a very important part of a Weather Service office's forecast and warning responsibilities. Severe thunderstorms require a critical response in the form of watches and warnings. (A severe thunderstorm by National Weather Service definition is one that produces wind gusts of 50 knots or greater, hail of 3/4 inch diameter or larger, and/or tornadoes.) Nevertheless, heavy thunderstorms, those just below severe in­ ·tensity or those producing copious rainfall, also require a certain degree of response in the form of statements and often staffing. (These include thunder­ storms producing hail of any size and/or wind gusts of 35 knots or greater, or storms producing sufficiently intense rainfall to possess a potential for flash flooding.) It must be realized that heavy thunderstorms can have as much or more impact on the public, and require as much action by a forecast office, as do severe thunderstorms. For the purpose of this paper the term "signi­ ficant convection" will refer to a combination of these two thunderstorm classes. · It is the premise of this paper that significant convection, whether heavy or severe, develops from similar atmospheric situations. For effective opera­ tions, forecasters at Weather Service offices should be familiar with those factors which produce significant convection.
    [Show full text]
  • Presentation
    14.4 INVESTIGATION OF MESOSCALE PRESSURE AND TEMPERATURE TRANSIENTS ASSOCIATED WITH BOW ECHOES Rebecca D. Adams∗ and Richard H. Johnson Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado 1. INTRODUCTION over the entire state, available over the past 13 years. For the purposes of this study, only the years 2002 Bow echoes have been an established part of the through 2005 were examined, to correspond with literature since a 1978 technical report by Fujita– available radar data. The diurnal cycle was then who not only coined the term, but also created a removed from the pressure observations; they were conceptual model showcasing the lifecycle of these also corrected to a constant height (356.5 m, av- systems. The bow echo’s association with severe erage height of all stations) using virtual tempera- winds has also been both well-studied and well- ture. In addition, a high-pass Lanczos filter (Duchon documented, from Fujita’s original work to the 1979) was run on the data to remove all the longer, present. However, very little work has focused on synoptic timescales. Following the definition pro- surface features, such as pressure and temperature, vided in the American Meteorological Society Glos- associated with these storms. While the arrange- sary (2000), the upper (longer) end of the meso- ment of these parameters as associated with squall timescale is the pendulum day, which for average lines has become highly recognizable (including the Oklahoma latitude is 41.2 hours in length. Thus, mesohigh, cold pool, and wake low; Johnson & the Lanczos filter was run to retain all features with Hamilton 1988, Loehrer & Johnson 1995), it is still a period shorter than this.
    [Show full text]
  • Downloaded 10/01/21 08:47 AM UTC 2062 JOURNAL of the ATMOSPHERIC SCIENCES VOLUME 57 Et Al
    1JULY 2000 BRYAN AND FRITSCH 2061 Diabatically Driven Discrete Propagation of Surface Fronts: A Numerical Analysis GEORGE H. BRYAN AND J. MICHAEL FRITSCH Department of Meteorology, The Pennsylvania State University, University Park, Pennsylvania (Manuscript received 2 July 1998, in ®nal form 30 August 1999) ABSTRACT Discrete frontal propagation has been identi®ed as a process whereby a surface front discontinuously moves forward, without evidence of frontal passage across a mesoscale region. Numerical simulations are employed to examine the upper-level evolution of a discrete frontal propagation event and to explore the processes that were responsible for the discrete movement. Model results indicate that a frontal pressure trough was not able to penetrate through a deep surface-based layer of cool air created by a precipitating convective system several hundred kilometers in advance of the front. Meanwhile, a new low-level baroclinic zone formed well ahead of the front along the southern side of the cool layer. As the midlevel front moved continuously over the cool layer, a new low-level front developed in the new baroclinic zone and the original low-level front dissipated. At the surface, the simulated front did not pass through the cool layer. Frontogenesis terms reveal that the prefrontal circulation that becomes the new frontal circulation initially forms directly from diabatic frontogenesis. Daytime heating in the prefrontal boundary layer and cooling from thunderstorms combine to create a thermal gradient and a mesoscale pressure perturbation. Winds turn in response to the altered pressure ®eld and form a convergent boundary, resulting in kinematic frontogenesis. The boundary subsequently undergoes rapid intensi®cation.
    [Show full text]
  • Manual on Low-Level Wind Shear
    Doc 9817 AN/449 Manual on Low-level Wind Shear Approved by the Secretary General and published under his authority First Edition — 2005 International Civil Aviation Organization Suzanne Doc 9817 AN/449 Manual on Low-level Wind Shear Approved by the Secretary General and published under his authority First Edition — 2005 International Civil Aviation Organization AMENDMENTS Amendments are announced in the supplements to the Catalogue of ICAO Publications; the Catalogue and its supplements are available on the ICAO website at www.icao.int. The space below is provided to keep a record of such amendments. RECORD OF AMENDMENTS AND CORRIGENDA AMENDMENTS CORRIGENDA No. Date Entered by No. Date Entered by 1 26/9/08 ICAO 1 17/11/05 ICAO 2 21/2/11 ICAO (iii) FOREWORD Since 1943, low-level wind shear has been cited in a number of aircraft accidents/incidents that together have contributed to over 1 400 fatalities worldwide. Increased awareness within the aviation community of the hazardous and insidious nature of low-level wind shear has been reflected in the fact that the ICAO Council has considered it to be one of the major technical problems facing aviation. Until the 1980s, lack of adequate operational remote-sensing equipment, the complexity of the subject, the wide range of scale of wind shear and its inherent unpredictability all conspired to hinder a complete solution to the problem which, in turn, limited the development of the necessary international Standards and Recommended Practices for the observing, reporting and forecasting of wind shear. In 1975 there were five jet transport aircraft accidents/incidents in which wind shear was cited, one of which resulted in major loss of life.1 The latter accident, which occurred at John F.
    [Show full text]
  • Storm Evolution and Transition Into a Bow Echo
    VOL. 58, NO.13 JOURNAL OF THE ATMOSPHERIC SCIENCES 1JULY 2001 Numerical Simulation of Tornadogenesis in a High-Precipitation Supercell. Part I: Storm Evolution and Transition into a Bow Echo CATHERINE A. FINLEY,* W. R. COTTON, AND R. A. PIELKE SR. Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado (Manuscript received 27 August 1998, in ®nal form 16 November 2000) ABSTRACT A nested grid primitive equation model (RAMS version 3b) was used to simulate a high-precipitation (HP) supercell, which produced two weak tornadoes. Six telescoping nested grids allowed atmospheric ¯ows ranging from the synoptic scale down to the tornadic scale to be represented in the simulation. All convection in the simulation was initiated with resolved vertical motion and subsequent condensation±latent heating from the model microphysics; no warm bubbles or cumulus parameterizations were used. Part I of this study focuses on the simulated storm evolution and its transition into a bow echo. The simulation initially produced a classic supercell that developed at the intersection between a stationary front and an out¯ow boundary. As the simulation progressed, additional storms developed and interacted with the main storm to produce a single supercell. This storm had many characteristics of an HP supercell and eventually evolved into a bow echo with a rotating comma-head structure. An analysis of the storm's transition into a bow echo revealed that the interaction between convective cells triggered a series of events that played a crucial role in the transition. The simulated storm structure and evolution differed signi®cantly from that of classic supercells produced by idealized simulations.
    [Show full text]
  • Some Meteorological Characteristics of Significant Tornado Events
    FEBRUARY 2002 NOTES AND CORRESPONDENCE 155 Some Meteorological Characteristics of Signi®cant Tornado Events Occurring in Proximity to Flash Flooding JOSEPH A. ROGASH NOAA/NWS/Weather Forecast Of®ce, El Paso, Texas JONATHAN RACY NOAA/NWS/Storm Prediction Center, Norman, Oklahoma 9 February 2001 and 5 September 2001 ABSTRACT A study was performed to determine meteorological aspects of environments in which thunderstorms produced both strong or violent tornadoes and ¯ash ¯oods within a limited temporal and spatial domain. It was found that the overwhelming majority of these episodes occurred in the spring and summer months and during the afternoon and evening hours. In most instances, at least some of the tornadoes were present when ¯ash ¯ooding was in progress. The ambient environment usually included an air mass that exhibited both relatively high convective instability and abundant lower-tropospheric moisture, including an average most-unstable CAPE of 3200 J kg21 and mean surface dewpoint and precipitable water values of 708F (218C) and 41 mm (1.6 in.), respectively. Storm-relative helicity magnitudes indicated that the vertical wind shear ranged from marginally to moderately favorable for supercell formation in all cases. Surface patterns for each episode were generally similar to patterns earlier studies determined to be frequently attendant with ¯ash ¯ooding, in which preexisting surface boundaries acted to focus deep convection. Most events also occurred east of an approaching and well- de®ned upper-tropospheric trough and in the left-front or right-rear quadrant of an upper-level jet streak in which upward vertical motion is usually present. 1. Introduction strong and violent tornadoes and excessive rain pose an exceptional hazard to both life and property, the ability Deep convection and associated weather phenomena to anticipate and identify such multiphenomena events remain a forecasting challenge for operational meteo- is critical to the mission of operational meteorologists.
    [Show full text]
  • Chapter 15, Part 1 What Are Thunderstorms? Ordinary
    Chapter 15, Part 1 Thunderstorms What are thunderstorms? • Thunderstorms are simply storms containing thunder and lightning. • Sometimes also gusty winds, heavy rain, or hail. • Categorized as – Ordinary – short lived, rarely produce strong winds or hail – Severe – high winds, flash floods, damaging hail, and even tornadoes Ordinary Thunderstorms • There are three stages of an ordinary thunderstorm: cumulus, mature, dissipating. 1 Cumulus Stage • Warm humid air rises, cools, and condenses into cumulus cloud(s) • Sometimes cloud evaporates in dry air, but then a new cloud grows higher. • Condensing water releases latent heat making cloud warmer than air around it. • Insufficient time for precipitation to form. • Updrafts keep water droplets and ice crystals suspended. Mature Thunderstorm • Entrainment – dryer colder air Anvil shape at drawn in. Sometimes rain drops stable region. evaporate further cooling air. • Creates downdraft. • Cell = updraft + downdraft. • Most storms several cells (~1hr). • Storm most intense with heavy rain and sometimes small hail. • Cold air at onset of precipitation. • Top reaching stable region leads to anvil shape. Picture of Mature Thunderstorm • Note anvil top. 2 Overshoot • Updrafts can be so strong than the cloud rises into the stable region of the atmosphere. Dissipating Stage • Updrafts weaken and downdrafts dominate. • Light precipitation, weaker winds. • Down drafts can feed other updrafts, creating multicell storms (common). • At end of storm surface temperature can be much cooler (10-20oF), but rain evaporating increases moisture. Dissipating Thunderstorm • Most of the lower half of cloud has evaporated leaving only cirrus anvil top. 3 A Multicell Storm • Middle cell is mature stage, right cell in cumulus stage, and left cell is almost mature.
    [Show full text]
  • Information to Users
    INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UMI films the text directly from the original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type of computer printer. The quality of this reproduction is dependent upon the quality of the copy submitled. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and improper alignment can adversely affect reproduction. In the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, beginning at the upper left-hand comer and continuing from left to right in equal sections with small overlaps. Photographs included in the original manuscript have been reproduced xerographically in this copy. Higher quality 6* x 9* black arxf white photographic prints are available for any photographs or illustrations appearing in this copy for an additional charge. Contact UMI directly to order. Bell & Howell Information and Learning 300 North Zfteb Road, Ann Arbor, Ml 48106-1346 USA UMI 800-521-0600 UNIVERSITY OF OKLAHOMA GRADUATE COLLEGE A PSEUDO-DUAL-DOPPLER ANALYSIS OF CYCLIC TORNADOGENESIS A Dissertation SUBMITTED TO THE GRADUATE FACULTY in partial fulfillment of the requirements for the degree of Doctor of Philosophy By DAVID C. DOWELL Norman, Oklahoma 2000 UMI Number 9956999 UMI UMI Microform9956999 Copyright 2000 by Bell & Howell Information and Learning Company.
    [Show full text]