THE DVORAK TROPICAL CYCLONE INTENSITY ESTIMATION TECHNIQUE a Satellite-Based Method That Has Endured for Over 30 Years
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
UNDERSTANDING the GENESIS of HURRICANE VINCE THROUGH the SURFACE PRESSURE TENDENCY EQUATION Kwan-Yin Kong City College of New York 1 1
9B.4 UNDERSTANDING THE GENESIS OF HURRICANE VINCE THROUGH THE SURFACE PRESSURE TENDENCY EQUATION Kwan-yin Kong City College of New York 1 1. INTRODUCTION 20°W Hurricane Vince was one of the many extraordinary hurricanes that formed in the record-breaking 2005 Atlantic hurricane season. Unlike Katrina, Rita, and Wilma, Vince was remarkable not because of intensity, nor the destruction it inflicted, but because of its defiance to our current understandings of hurricane formation. Vince formed in early October of 2005 in the far North Atlantic Ocean and acquired characteristics of a hurricane southeast of the Azores, an area previously unknown to hurricane formation. Figure 1 shows a visible image taken at 14:10 UTC on 9 October 2005 when Vince was near its peak intensity. There is little doubt that a hurricane with an eye surrounded by convection is located near 34°N, 19°W. A buoy located under the northern eyewall of the hurricane indicated a sea-surface temperature (SST) of 22.9°C, far below what is considered to be the 30°N minimum value of 26°C for hurricane formation (see insert of Fig. 3f). In March of 2004, a first-documented hurricane in the South Atlantic Ocean also formed over SST below this Figure 1 Color visible image taken at 14:10 UTC 9 October 2005 by Aqua. 26°C threshold off the coast of Brazil. In addition, cyclones in the Mediterranean and polar lows in sub-arctic seas had been synoptic flow serves to “steer” the forward motion of observed to acquire hurricane characteristics. -
Extended Abstract
THE REASONS FOR A REANALYSIS OF THE 1. The reanalysis with the satellite data after the TYPHOONS INTENSITY IN THE WESTERN reconnaissances era since August 1987 NORTH PACIFIC The most significant case was Typhoon Sally in September 1996 which was moving west-north-west 1 1 Karl Hoarau , Ludovic Chalonge and Jean-Paul when it was located east-north-east of the Philippines 2 Hoarau (ATCR, 1996). JTWC estimated the maximum intensity at 72 m/s on 7 th September at 1800Z while the RSMC 1. Introduction of Tokyo gave a sustained surface wind of 41 m/s at the same time and 44 m/s at 0000Z on 8 th (JMA, 1996). 41 At the time where a recent article (Webster and al., m/s and 44 m/s over 10 minutes match respectively 2005) claimed that the number of intense tropical with T 5.2 and T 5.5 in the Dvorak’scale used by cyclones have significantly increased since 1975, it was Tokyo. As JTWC used the sustained winds over 1 very urgent to have a view as objective as possible on minute and that 72 m/s represents T 7.0 in the 1984 the quality of the best track data. We chose the western Dvorak’scale, this means that there was a difference of North Pacific because this basin is the more active, it almost 2 T-numbers at 1800Z on 7 th and 1.5 T-number has the greatest number of cyclones at the at 0000Z on 8th. The 72 m/s estimated by JTWC have hurricane/typhoon's intensity (at least 33 m/s) and the been primarily based on the Objective Dvorak more important number of cyclones with a sustained Technique (ODT) tested with the typhoons displaying wind at or over 60 m/s (at least Category 4 of Saffir- an eye in the western North Pacific between 1995 and Simpson). -
1 a Hyperactive End to the Atlantic Hurricane Season: October–November 2020
1 A Hyperactive End to the Atlantic Hurricane Season: October–November 2020 2 3 Philip J. Klotzbach* 4 Department of Atmospheric Science 5 Colorado State University 6 Fort Collins CO 80523 7 8 Kimberly M. Wood# 9 Department of Geosciences 10 Mississippi State University 11 Mississippi State MS 39762 12 13 Michael M. Bell 14 Department of Atmospheric Science 15 Colorado State University 16 Fort Collins CO 80523 17 1 18 Eric S. Blake 19 National Hurricane Center 1 Early Online Release: This preliminary version has been accepted for publication in Bulletin of the American Meteorological Society, may be fully cited, and has been assigned DOI 10.1175/BAMS-D-20-0312.1. The final typeset copyedited article will replace the EOR at the above DOI when it is published. © 2021 American Meteorological Society Unauthenticated | Downloaded 09/26/21 05:03 AM UTC 20 National Oceanic and Atmospheric Administration 21 Miami FL 33165 22 23 Steven G. Bowen 24 Aon 25 Chicago IL 60601 26 27 Louis-Philippe Caron 28 Ouranos 29 Montreal Canada H3A 1B9 30 31 Barcelona Supercomputing Center 32 Barcelona Spain 08034 33 34 Jennifer M. Collins 35 School of Geosciences 36 University of South Florida 37 Tampa FL 33620 38 2 Unauthenticated | Downloaded 09/26/21 05:03 AM UTC Accepted for publication in Bulletin of the American Meteorological Society. DOI 10.1175/BAMS-D-20-0312.1. 39 Ethan J. Gibney 40 UCAR/Cooperative Programs for the Advancement of Earth System Science 41 San Diego, CA 92127 42 43 Carl J. Schreck III 44 North Carolina Institute for Climate Studies, Cooperative Institute for Satellite Earth System 45 Studies (CISESS) 46 North Carolina State University 47 Asheville NC 28801 48 49 Ryan E. -
REVIEW the Extratropical Transition of Tropical Cyclones. Part I
VOLUME 145 MONTHLY WEATHER REVIEW NOVEMBER 2017 REVIEW The Extratropical Transition of Tropical Cyclones. Part I: Cyclone Evolution and Direct Impacts a b c d CLARK EVANS, KIMBERLY M. WOOD, SIM D. ABERSON, HEATHER M. ARCHAMBAULT, e f f g SHAWN M. MILRAD, LANCE F. BOSART, KRISTEN L. CORBOSIERO, CHRISTOPHER A. DAVIS, h i j k JOÃO R. DIAS PINTO, JAMES DOYLE, CHRIS FOGARTY, THOMAS J. GALARNEAU JR., l m n o p CHRISTIAN M. GRAMS, KYLE S. GRIFFIN, JOHN GYAKUM, ROBERT E. HART, NAOKO KITABATAKE, q r s t HILKE S. LENTINK, RON MCTAGGART-COWAN, WILLIAM PERRIE, JULIAN F. D. QUINTING, i u v s w CAROLYN A. REYNOLDS, MICHAEL RIEMER, ELIZABETH A. RITCHIE, YUJUAN SUN, AND FUQING ZHANG a University of Wisconsin–Milwaukee, Milwaukee, Wisconsin b Mississippi State University, Mississippi State, Mississippi c NOAA/Atlantic Oceanographic and Meteorological Laboratory/Hurricane Research Division, Miami, Florida d NOAA/Climate Program Office, Silver Spring, Maryland e Embry-Riddle Aeronautical University, Daytona Beach, Florida f University at Albany, State University of New York, Albany, New York g National Center for Atmospheric Research, Boulder, Colorado h University of São Paulo, São Paulo, Brazil i Naval Research Laboratory, Monterey, California j Canadian Hurricane Center, Dartmouth, Nova Scotia, Canada k The University of Arizona, Tucson, Arizona l Institute for Atmospheric and Climate Science, ETH Zurich, Zurich, Switzerland m RiskPulse, Madison, Wisconsin n McGill University, Montreal, Quebec, Canada o Florida State University, Tallahassee, Florida p -
HURRICANE IRMA (AL112017) 30 August–12 September 2017
NATIONAL HURRICANE CENTER TROPICAL CYCLONE REPORT HURRICANE IRMA (AL112017) 30 August–12 September 2017 John P. Cangialosi, Andrew S. Latto, and Robbie Berg National Hurricane Center 1 24 September 2021 VIIRS SATELLITE IMAGE OF HURRICANE IRMA WHEN IT WAS AT ITS PEAK INTENSITY AND MADE LANDFALL ON BARBUDA AT 0535 UTC 6 SEPTEMBER. Irma was a long-lived Cape Verde hurricane that reached category 5 intensity on the Saffir-Simpson Hurricane Wind Scale. The catastrophic hurricane made seven landfalls, four of which occurred as a category 5 hurricane across the northern Caribbean Islands. Irma made landfall as a category 4 hurricane in the Florida Keys and struck southwestern Florida at category 3 intensity. Irma caused widespread devastation across the affected areas and was one of the strongest and costliest hurricanes on record in the Atlantic basin. 1 Original report date 9 March 2018. Second version on 30 May 2018 updated casualty statistics for Florida, meteorological statistics for the Florida Keys, and corrected a typo. Third version on 30 June 2018 corrected the year of the last category 5 hurricane landfall in Cuba and corrected a typo in the Casualty and Damage Statistics section. This version corrects the maximum wind gust reported at St. Croix Airport (TISX). Hurricane Irma 2 Hurricane Irma 30 AUGUST–12 SEPTEMBER 2017 SYNOPTIC HISTORY Irma originated from a tropical wave that departed the west coast of Africa on 27 August. The wave was then producing a widespread area of deep convection, which became more concentrated near the northern portion of the wave axis on 28 and 29 August. -
TROPICAL CYCLONE ANALYSIS USING AMSU DATA Stanley Q
P3.2 TROPICAL CYCLONE ANALYSIS USING AMSU DATA Stanley Q. Kidder* CIRA, Colorado State University, Fort Collins, Colorado Mitchell D. Goldberg NOAA/NESDIS/CRAD, Camp Springs, Maryland Raymond M. Zehr and Mark DeMaria NOAA/NESDIS/RAMM Team, Fort Collins, Colorado James F. W. Purdom NOAA/NESDIS/ORA, Washington, D.C. Christopher S. Velden CIMSS, University of Wisconsin, Madison, Wisconsin Norman C. Grody NOAA/NESDIS/Microwave Sensing Group, Camp Springs, Maryland Sheldon J. Kusselson NOAA/NESDIS/SAB, Camp Springs, Maryland 1. INTRODUCTION estimate temperature between the surface and 10 hPa from AMSU observations were generated from collo- Scientific progress often comes about as a result of cated AMSU-A limb adjusted brightness temperatures new instruments for making scientific observations. The and radiosonde temperature profiles. Above 10 hPa, the Advanced Microwave Sounding Unit (AMSU) is one regression coefficients were generated from brightness such new instrument. First flown on the NOAA 15 satel- temperatures simulated from a set of rocketsonde pro- lite launched 13 May 1998, AMSU will fly on the NOAA files. The root mean square (rms) differences between 16 and NOAA 17 satellites as well. AMSU-A temperature retrievals and collocated ra- AMSU is a 20-channel instrument designed to diosondes for the latitude range of 0º to 30º north are make temperature and moisture soundings through less than 2 K. Additional details on the temperature re- clouds. Geophysical parameters such as rain rate, col- trieval procedures and accuracies are given in Goldberg umn-integrated water vapor and column-integrated (1999). cloud liquid water can also be retrieved. The AMSU has Rain rate and column-integrated cloud liquid water significantly improved spatial resolution, radiometric and water vapor are retrieved semi-operationally by the accuracy, and number of channels over the Microwave NESDIS/Microwave Sensing Group using algorithms Sounding Unit, which flew on TIROS N and the NOAA 6 described in Grody et al. -
Estimating Tropical Cyclone Intensity from Infrared Image Data
690 WEATHER AND FORECASTING VOLUME 26 Estimating Tropical Cyclone Intensity from Infrared Image Data MIGUEL F. PIN˜ EROS College of Optical Sciences, The University of Arizona, Tucson, Arizona ELIZABETH A. RITCHIE Department of Atmospheric Sciences, The University of Arizona, Tucson, Arizona J. SCOTT TYO College of Optical Sciences, The University of Arizona, Tucson, Arizona (Manuscript received 20 December 2010, in final form 28 February 2011) ABSTRACT This paper describes results from a near-real-time objective technique for estimating the intensity of tropical cyclones from satellite infrared imagery in the North Atlantic Ocean basin. The technique quantifies the level of organization or axisymmetry of the infrared cloud signature of a tropical cyclone as an indirect measurement of its maximum wind speed. The final maximum wind speed calculated by the technique is an independent estimate of tropical cyclone intensity. Seventy-eight tropical cyclones from the 2004–09 seasons are used both to train and to test independently the intensity estimation technique. Two independent tests are performed to test the ability of the technique to estimate tropical cyclone intensity accurately. The best results from these tests have a root-mean-square intensity error of between 13 and 15 kt (where 1 kt ’ 0.5 m s21) for the two test sets. 1. Introduction estimate the intensity of tropical cyclones was developed by V. Dvorak in the 1970s during the early years of Tropical cyclones (TC) form over the warm waters of satellites (Dvorak 1975). In this technique, an analyst the tropical oceans where direct measurements of their classifies the cloud scene types in visible and infrared intensity (among other factors) are scarce (Gray 1979; satellite imagery and applies a set of rules to calculate McBride 1995). -
Notable Tropical Cyclones and Unusual Areas of Tropical Cyclone Formation
A flood is an overflow of an expanse of water that submerges land.[1] The EU Floods directive defines a flood as a temporary covering by water of land not normally covered by water.[2] In the sense of "flowing water", the word may also be applied to the inflow of the tide. Flooding may result from the volume of water within a body of water, such as a river or lake, which overflows or breaks levees, with the result that some of the water escapes its usual boundaries.[3] While the size of a lake or other body of water will vary with seasonal changes in precipitation and snow melt, it is not a significant flood unless such escapes of water endanger land areas used by man like a village, city or other inhabited area. Floods can also occur in rivers, when flow exceeds the capacity of the river channel, particularly at bends or meanders. Floods often cause damage to homes and businesses if they are placed in natural flood plains of rivers. While flood damage can be virtually eliminated by moving away from rivers and other bodies of water, since time out of mind, people have lived and worked by the water to seek sustenance and capitalize on the gains of cheap and easy travel and commerce by being near water. That humans continue to inhabit areas threatened by flood damage is evidence that the perceived value of living near the water exceeds the cost of repeated periodic flooding. The word "flood" comes from the Old English flod, a word common to Germanic languages (compare German Flut, Dutch vloed from the same root as is seen in flow, float; also compare with Latin fluctus, flumen). -
Objective Estimation of Tropical Cyclone Intensity from Active and Passive Microwave Remote Sensing Observations in the Northwestern Pacific Ocean
remote sensing Article Objective Estimation of Tropical Cyclone Intensity from Active and Passive Microwave Remote Sensing Observations in the Northwestern Pacific Ocean Kunsheng Xiang 1,2,3, Xiaofeng Yang 1,3,* , Miao Zhang 4, Ziwei Li 1 and Fanping Kong 1,2 1 State Key Laboratory of Remote Sensing Science, Institute of Remote Sensing and Digital Earth, Chinese Academy of Sciences, Beijing 100101, China; [email protected] (K.X.); [email protected] (Z.L.); [email protected] (F.K.) 2 University of Chinese Academy of Sciences, Beijing 100049, China 3 The Hainan Key Laboratory of Earth Observation, Sanya 572029, China 4 Key Lab of Radiometric Calibration and Validation for Environmental Satellites, China Meteorological Administration (LRCVES/CMA) and National Satellite Meteorological Center, Beijing 100081, China; [email protected] * Correspondence: [email protected]; Tel.: +86-010-64806215 Received: 18 February 2019; Accepted: 11 March 2019; Published: 14 March 2019 Abstract: A method of estimating tropical cyclone (TC) intensity based on Haiyang-2A (HY-2A) scatterometer, and Special Sensor Microwave Imager and Sounder (SSMIS) observations over the northwestern Pacific Ocean is presented in this paper. Totally, 119 TCs from the 2012 to 2017 typhoon seasons were selected, based on satellite-observed data and China Meteorological Administration (CMA) TC best track data. We investigated the relationship among the TC maximum-sustained wind (MSW), the microwave brightness temperature (TB), and the sea surface wind speed (SSW). Then, a TC intensity estimation model was developed, based on a multivariate linear regression using the training data of 96 TCs. Finally, the proposed method was validated using testing data from 23 other TCs, and its root mean square error (RMSE), mean absolute error (MAE), and bias were 5.94 m/s, 4.62 m/s, and −0.43 m/s, respectively. -
Subsidence Warming As an Underappreciated Ingredient in Tropical Cyclogenesis
NOVEMBER 2015 K E R N S A N D C H E N 4237 Subsidence Warming as an Underappreciated Ingredient in Tropical Cyclogenesis. Part I: Aircraft Observations BRANDON W. KERNS AND SHUYI S. CHEN Rosenstiel School of Marine and Atmospheric Science, University of Miami, Miami, Florida (Manuscript received 15 December 2014, in final form 15 July 2015) ABSTRACT The development of a compact warm core extending from the mid-upper levels to the lower troposphere and related surface pressure falls leading to tropical cyclogenesis (TC genesis) is not well understood. This study documents the evolution of the three-dimensional thermal structure during the early developing stages of Typhoons Fanapi and Megi using aircraft dropsonde observations from the Impact of Typhoons on the Ocean in the Pacific (ITOP) field campaign in 2010. Prior to TC genesis, the precursor disturbances were characterized by warm (cool) anomalies above (below) the melting level (;550 hPa) with small surface pressure perturbations. Onion-shaped skew T–logp profiles, which are a known signature of mesoscale subsidence warming induced by organized mesoscale convective systems (MCSs), are ubiquitous throughout the ITOP aircraft missions from the precursor disturbance to the tropical storm stages. The warming partially erodes the lower-troposphere (850–600 hPa) cool anomalies. This warming results in increased surface pressure falls when superposed with the upper-troposphere warm anomalies associated with the long-lasting MCSs/cloud clusters. Hydrostatic pressure analysis suggests the upper-level warming alone would not result in the initial sea level pressure drop associated with the transformation from a disturbance to a TC. -
Microwave Instruments and Tropical Cyclone Applications
CMA Tropical Cyclone Analysis VISIT Using Polar Orbiter Satellite Imagery Derrick Herndon University of Wisconsin – CIMSS Direct Broadcast Workshop Miami, February 9-13, 2015 Microwave Sounders AMSU, SSMIS & ATMS ARCHER MIMIC-TPW Dvorak Super Typhoon Jelewat 2012 First … How are Tropical Cyclones Analyzed? Dvorak Technique Vern Dvorak – circa late 1970’s “The Dvorak tropical cyclone (TC) intensity estimation technique has been the primary method of monitoring tropical systems for more than three decades. The technique has likely saved tens of thousands of lives in regions where over one billion people are directly affected by TCs (commonly called hurricanes, typhoons, or cyclones). The Dvorak technique’s practical appeal and demonstrated skill in the face of tremendous dynamic complexity” - Velden et al 2006 Dvorak Technique • Intensity is inferred from patterns and features • 24 hour change requirement addresses diurnal changes unrelated to intensity • TC position relative to convective features important for accurate intensity estimates • Most accurate for estimating TC central pressure • DT is most objective for eye scenes • Method has stood the test of time however some changes can be made to improve estimates. Dvorak Technique - Flow Locate System Es9mate Intensity Data T Number Model Expected T Number 1. Cloud system 2. 24 hour changes measurements Eye Pa5ern Adjusted Model T number Curved Band Paern recogni9on Shear Covered center Choose best es9mate Apply constraints Final intensity Enhanced IR Scene Types Dvorak Technique Dvorak -
Tropical Cyclones Are Not Formed Near the Equator
CHAPTER 3.3 ATMOSPHERIC CIRCULATION & WEATHER SYSTEMS Atmospheric Pressure The weight of a column of air contained in a unit area Isobar is a line connecting points that from the mean sea level to the top of the atmosphere have equal values of pressure. Isobars are is called the atmospheric pressure. The atmospheric analogous to the contour lines on a relief pressure is expressed in units of milibar. At sea level the map. The spacing of isobars expresses average atmospheric pressure is 1,013.2 milibar. Due the rate and direction of change in air to gravity the air at the surface is denser and hence has pressure. This change in air pressure is higher pressure. referred as pressure gradient. The distribution of atmospheric pressure over the globe is known as horizontal distribution of pressure. It is shown on maps with the help of isobars. The horizontal distribution of atmospheric pressure is not uniform in the world. It varies from time to time at a given place; it varies from place to place over short distances. The factors responsible for variation in the horizontal Air Pressure : The fundamental rule about distribution of pressure are as follows: gases is that when they are heated, they Air Temperature: The earth is not heated uniformly become less dense and expand in volume because of unequal distribution of insolation, and rise. Hence, air pressure is low in diff erential heating and cooling of land and water equatorial regions and it is higher in polar surfaces. regions. Along the equator lies a belt of Generally there is an inverse relationship between low pressure known as the “equatorial low air temperature and air pressure.