Flying the Tropics
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
January — March Year 2017
VOL 2 ISSUE 01 JANUARY — MARCH YEAR 2017 2016/17 DRY SEASON SUMMARY Dominica's dry season officially runs from December to May each year. The 2016 wet season, which prolonged into December resulting in a delay to the start of the 2016/17 dry season, was recorded as a normal season as it relates to rainfall amounts. A weak La Niña (the cooling of the Eastern Equatorial Pacific Ocean) was observed towards the end of 2016 and a transition to ENSO– neutral is expected during the period January to March 2017. La Niña tends to shift rainfall chances for January-February-March 2017 to above to normal in the southern-most is- lands of the Caribbean. With this occurrence, above to normal rainfall amounts are expected, resulting in less solar radiation and more cooling by clouds and more rainfall than last year. Temperatures are also expected to be closer to normal. IN THIS ISSUE Pg.1 2016/17 Dry-Season Dominica’s Climate Pg.2 Looking back at 2016 Pg.3 2016 Hurricane Season Looking ahead Pg.4 Seasonal Forecast Chart 1. Mid-December ENSO prediction plume DOMINICA’S CLIMATE Rainfall received during the dry season are usually generated by the annual migration of the North Atlantic Subtropical High, low level clouds which move with the easterly trade winds, southward dipping frontal boundaries and trough sys- tems. The dry season runs from December to May when the seas are cooler and thunderstorms and rainfall activity are relatively low. On average approximately 40% of the annual rainfall is recorded in elevated and eastern areas and ap- proximately 25% along the western coast. -
Advanced Lectures on Dynamical Meteorology
ADVANCED LECTURES ON DYNAMICAL METEOROLOGY Roger K. Smith Fassung: WS 02/03 Contents 1 INTRODUCTION 3 1.1Somerevision........................... 4 1.1.1 Themomentumequationinheightcoordinates..... 4 1.2TheBoussinesqapproximation.................. 5 1.3Theanelasticapproximation................... 5 1.4Pressurecoordinates....................... 6 1.5Otherpressurecoordinatesystems................ 7 1.6Isentropiccoordinates....................... 7 1.7Sigmacoordinates......................... 7 2 SMALL-AMPLITUDE WAVES IN A STABLY-STRATIFIED ROTATING ATMOSPHERE 9 2.1 Boundary waves .......................... 17 2.2Theeffectsofshear........................ 19 2.3Theenergyequation....................... 20 2.4Simplifiedsolutionsandfilteredequations........... 21 2.5 ‘Sound-proofing’ the equations .................. 21 2.6Thehydrostaticapproximation................. 23 2.7 Sound-proofed hydrostatic approximation . ......... 24 2.8 Variation of mean density with height; the equivalent incom- pressibleatmosphere....................... 24 2.9Geostrophicmotion........................ 24 3 WAVES ON MOVING STRATIFIED FLOWS 29 3.1Freewaves............................. 30 3.2Forcedwaves........................... 31 3.3Mountainwaves.......................... 34 3.4LinearTheory........................... 35 3.5Flowoverisolatedtopography.................. 39 3.6Trappedleewaves......................... 45 1 4 ENERGETICS OF WAVES ON STRATIFIED SHEAR FLOWS 55 4.1Slowlyvaryingwavetrainsorwavepackets........... 60 5 SHEARING INSTABILITY 66 5.1 Helmholtz instability -
Weather Review and Outlook Towering Cumulus- Danny Gregoria by David Ross and Rob Molleda
Winter 2013 Welcome to this edition of Tropical Winds. Another hurricane season to be thankful for In This Issue… (…unless you are a hurricane junkie…). In Weather Review…………….….1 this edition, we will discuss what occurred Severe Weather Climo………...….7 during this year’s wet season and what to Hurricane Season 2013……………9 expect for the dry season. Also, we will talk about tornado climatology across South Employee Spotlight……………12 Florida. A look back at the 2013 Atlantic hurricane season will follow. To finish on a happy note, we will introduce you to another one of our devoted forecasters, Chris Duke. Happy Holidays!!! Weather Review and Outlook Towering Cumulus- Danny Gregoria By David Ross and Rob Molleda Looking Back at the Rainy Season May – October 2013 Synopsis The recently-concluded rainy season was wetter than normal across most of South Florida. It was very wet over most of southwest Florida where rainfall totals for the period from May 18th to October 10th (the duration of this year’s wet season) were in the 40 to 50 inch range, with a few spots exceeding 50 inches (Figure 1). This almost equals a year’s worth of rain in less than five months! Isolated spots in southeast Florida also recorded over 50 inches of rain, with most of this area receiving between 35 and 45 inches. Every month of the rainy season featured above normal rainfall over different parts of south Florida, with July being the wettest month overall due to a more widespread rainfall coverage, and August being the driest mostly across the eastern half of the peninsula (Figure 2). -
Low Level Wind Patterns Over the Indian Ocean
Low level wind patterns over the Indian Ocean Langlade Sébastien, tropical cyclone forecaster based on Hastenrath and Polzin, 2004, Dynamics of the windfield over the equatorial Indian Ocean, Q. J. R. Meteorol. Soc. (2004), 130, pp. 503–517 La Réunion, 2019/11/04 OUTLINE ■ Indian Ocean annual cycle and associated low level wind patterns ― Background ― Austral summer ― Austral winter ― Austral spring / autumn ■ Other wind patterns ■ Conclusion Tropical Indian Ocean surface winds patterns: Background Hastenrath etal., 2004 ■ 1 Austral summer 2 Austral autumn 3 Austral winter 2 Austral spring Tropical Indian Ocean surface winds patterns: Background Hastenrath etal., 2004 ■ 1 Austral summer 2 Austral autumn 3 Austral winter 2 Austral spring Austral summer (January to March) Austral summer (January to March) H L Austral summer (January to March) H L Austral summer (January to March) Monsoon Trough H (MT) L h Austral summer (January to March) Monsoon Trough définition: Low level trough (surface to 850 hPa) located equator within the mixing area between the monsoon and tradewinds flow. Associated equatorial winds have a strong meridional component. → Low level large scale vorticity associated. Austral summer (January to March) 18th February 2009 Winds at 925 hPa Equator Monsoon Trough (MT) Austral winter (June to August) Austral winter (June to August) L H L H Austral winter (June to August) L H Austral winter (June to August) ≥ 28 kt ≥ 16 kt H ≤ 4 kt L≤ 4 kt ≥ 16 kt Austral winter (June to August) India and south-eastern Asia monsoons ≥ 28 kt -
Mesoscale Interactions in Tropical Cyclone Genesis
OCTOBER 1997 SIMPSON ET AL. 2643 Mesoscale Interactions in Tropical Cyclone Genesis J. SIMPSON Earth Sciences Directorate, NASA/Goddard Space Flight Center, Greenbelt, Maryland E. RITCHIE Department of Meteorology, Naval Postgraduate School, Monterey, California G. J. HOLLAND Bureau of Meteorology Research Centre, Melbourne, Australia J. HALVERSON* Visiting Fellow, University Space Research Association, NASA/Goddard Space Flight Center, Greenbelt, Maryland S. STEWART NEXRAD OSF/OTB, National Weather Service, NOAA, Norman, Oklahoma (Manuscript received 21 November 1996, in ®nal form 13 February 1997) ABSTRACT With the multitude of cloud clusters over tropical oceans, it has been perplexing that so few develop into tropical cyclones. The authors postulate that a major obstacle has been the complexity of scale interactions, particularly those on the mesoscale, which have only recently been observable. While there are well-known climatological requirements, these are by no means suf®cient. A major reason for this rarity is the essentially stochastic nature of the mesoscale interactions that precede and contribute to cyclone development. Observations exist for only a few forming cases. In these, the moist convection in the preformation environment is organized into mesoscale convective systems, each of which have associated mesoscale potential vortices in the midlevels. Interactions between these systems may lead to merger, growth to the surface, and development of both the nascent eye and inner rainbands of a tropical cyclone. The process is essentially stochastic, but the degree of stochasticity can be reduced by the continued interaction of the mesoscale systems or by environmental in¯uences. For example a monsoon trough provides a region of reduced deformation radius, which substantially improves the ef®ciency of mesoscale vortex interactions and the amplitude of the merged vortices. -
Indian Monsoon Basic Drivers and Variability
Indian Monsoon Basic Drivers and Variability GOTHAM International Summer School PIK, Potsdam, Germany, 18-22 Sep 2017 R. Krishnan Indian Institute of Tropical Meteorology, Pune, India The Indian (South Asian) Monsoon Tibetan Plateau India Indian Ocean Monsoon circulation and rainfall: A convectively coupled phenomenon Requires a thermal contrast between land & ocean to set up the monsoon circulation Once established, a positive feedback between circulation and latent heat release maintains the monsoon The year to year variations in the seasonal (June – September) summer monsoon rains over India are influenced internal dynamics and external drivers Long-term climatology of total rainfall over India during (1 Jun - 30 Sep) summer monsoon season (http://www.tropmet.res.in) Interannual variability of the Indian Summer Monsoon Rainfall Primary synoptic & smaller scale circulation features that affect cloudiness & precipitation. Locations of June to September rainfall exceeding 100 cm over the land west of 100oE associated with the southwest monsoon are indicated (Source: Rao, 1981). Multi-scale interactions Low frequency Synoptic Systems:Lows, sub-seasonal Depressions, MTC variability – Large scale Active and monsoon Break monsoon Organized convection, Embedded mesoscale systems , heavy rainfall (intensity > 10 cm/day) Winds at 925hPa DJF West African Monsoon Asian Monsoon Austral Monsoon JJA Courtesy: J.M. Slingo, Univ of Reading Land/Sea Temperature contrasts Nov./Dec. West African Monsoon Asian Monsoon Austral Monsoon May/June Courtesy: -
Variations and Seasonal Prediction of Wet and Dry Season Precipitation Over the Maritime Continent: Roles of ENSO and Monsoon Circulation
Science and Technology Infusion Climate Bulletin NOAA’s National Weather Service 39th NOAA Annual Climate Diagnostics and Prediction Workshop St. Louis, MO, 20-23 October 2014 Variations and Seasonal Prediction of Wet and Dry Season Precipitation over the Maritime Continent: Roles of ENSO and Monsoon Circulation Tuantuan Zhang1, Song Yang1, and Xingwen Jiang2 1Department of Atmospheric Sciences, Sun Yat-sen University, Guangzhou, Guangdong, China 2Institute of Plateau Meteorology, China Meteorological Administration, Chengdu, Sichuan, China 1. Introduction The authors analyze the seasonal-interannual variations of precipitation over the Maritime Continent (MC) and their relationships with large-scale climate anomalies. They also investigate the predictability of MC precipitation variations. The hindcast of the National Centers for Environmental Prediction (NCEP) Climate Forecast System version 2 (CFSv2) and several analysis/reanalysis products are used. 2. Results The seasonal evolution of MC precipitation does not apparently exhibit distinct features for four seasons. Instead, it is clearly characterized by a wet season (from December to March) and a dry season (from July to October) (Figs. 1 and 2). The Fig. 1 Observed monthly mean of MC precipitation (mm day-1, black line) and its standard deviations (shaded) from January to December. The MC domain can be seen from Fig. 2. The horizontal line denotes the annual average of MC precipitation. July- October are defined as dry season and December-March as wet season. Fig. 2 Anomalies of observed precipitation (mm day-1, shading) and 850-hPa winds (m s-1, vectors) in (a) wet season (December-March) and (b) dry season (July-October). The domain used to define the MC is outlined with red boxes. -
Analysis of Summer Monsoon Fluctuations Over India
February 1976 M. Murakami 15 Analysis of Summer Monsoon Fluctuations over India By Masato Murakami Meteorological Research Institute, Tokyo (Manuscript received 26 August 1975, in revised form 17 November 1975) Abstract Temporal fluctuations appearing in the summer monsoon over India are investigated by using the data of 1962. By the method of spectrum analysis, it is revealed that two major periodicities exist, at least, in the temporal fluctuation of the monsoon. One is the oscillation around 5 days period and the other is around 15 days pericd. The oscillation around 5 days period appears mainly in the range from the north Bay of Bengal through the monsoon trough region in northern India. The structure of the disturbance which causes this periodicity is examined by the method of cross spec- trum analysis. The results show that the disturbance is a westward-moving one and its longitudinal wavelength is about 30*. This disturbance seems to represent the so-called monsoon low. The vertical structure of these monsoon lows indicates that their cyclonic circulation is prevailing in the lower troposphere and the axis of the trough slightly tilts westward. Moreover, the monsoon low is accompanied with a distinct warm core in the upper troposphere. In the lower levels, the amplitude of the temperature is small and the disturbance is neither warm- nor cold cored. It is also shown that the monsoon low has a steering level at the height around 500 mb level. The oscillation around 15 days period is revealed to be in connection with the active/weak cycle of monsoon. The intense wind fluctuations associated with this cycle appear both in the upper and the lower troposphere, being in phase with each other. -
Significant Tornado Drought”
FLORIDA’S UNPRECEDENTED DRY SEASON “SIGNIFICANT TORNADO DROUGHT” Bart Hagemeyer, CCM National Weather Service Forecast Office Melbourne, Florida 1. INTRODUCTION The author has been researching Florida tornadoes since 1989 and documented every known tornado death in Florida history; totaling 207 since the first recorded death in 1882. Significant tornadoes, those of Enhanced Fujita Scale (EF) 2 and greater (WSEC, 2006), are most likely to cause fatalities and serious injuries. They typically occur in Florida under two distinct synoptic scenarios (Hagemeyer, 1997): 1) in the warm sector of extratropical cyclones (ET) associated with a strong jet stream during the dry season (November through April) when strong shear and instability combine to produce supercell thunderstorms; and 2) in outer rainbands in the right front quadrant of tropical or hybrid cyclones in the Gulf of Mexico or northwest Caribbean Sea, during the hurricane season, where very strong low-level shear and convergence can produce rotating storms and at times supercell thunderstorms. Tornadoes up to EF4 and EF3 strength have occurred in the extratropical and tropical scenarios respectively. 160 tornado deaths have been associated with extratropical cyclones and 38 deaths with tropical/hybrid cyclones. Outside of these two organized tropical and extratropical cyclone scenarios, significant tornadoes and tornado deaths in Florida are extremely rare. During the wet season from May to October only 9 other tornado deaths have occurred in the history of Florida that were not associated with a tropical/hybrid system. The fatalities with these rare, weaker tornado deaths were typically a result of people caught in highly vulnerable locations such as small boats and campers. -
Spotter Newsletter Volume 10: Wet Season
Hawai'i Ho'ohekili Skywarn Weather Spotter Newsletter National Weather Service, Honolulu, HI Wet Season Edition, 2014/2015 Issued — Nov 2014 Spotter Newsletter Volume 10 Inside this edition: El Nino watch continues! Wet Season begins! A review of the Central Pacific Hurricane Season. And more!!! El Nino Watch! ENSO neutral conditions persist, but indicators are pointing toward an El Nino event later this year. Sea surface temperatures (SST) are above average across the equatorial Pacific (see fig) - with continued above average SST, El Nino is likely to form. Climate models predict above normal air temperatures for Hawaii through the rest of 2014. Wet Season Rainfall Outlook for the State of Hawaii — Kevin Kodama, Service Hydrologist October 2014 through April 2015 NOAA’s Climate Prediction Center (CPC): El Nino still expected to develop by the end of 2014. - 55 to 60 percent probability of forming (lower probability than initially forecasted) - Projected to be weak. Probabilities favor below average rainfall through spring 2015, but not as dry as the 2009–2010 and 1997-1998 El Nino wet seasons. A weak El Nino usually allows some heavy rain events to impact the state. Some drought development is expected by early 2015, mainly affecting agriculture sector and those sensitive to short term rainfall shortages (e.g. catchment systems). Extreme drought conditions are not expected this season. It’s been a busy Hurricane Season Since the last newsletter, we have had 5 tropical cyclones pass in the Central Pacific!! through the Central Pacific. We still have the rest of November before the end of hurricane season. -
Tropical Cyclone: Climatology
ESCI 344 – Tropical Meteorology Lesson 5 – Tropical Cyclones: Climatology References: A Global View of Tropical Cyclones, Elsberry (ed.) The Hurricane, Pielke Tropical Cyclones: Their evolution, structure, and effects, Anthes Forecasters’ Guide to Tropical Meteorology, Atkinsson Forecasters Guide to Tropical Meteorology (updated), Ramage Global Guide to Tropical Cyclone Forecasting, Holland (ed.) Reading: Introduction to the Meteorology and Climate of the Tropics, Chapter 9 A Global View of Tropical Cyclones, Chapter 3 REQUIREMENTS FOR FORMATION In order for a tropical cyclone to form, the following general conditions must be present: Deep, warm ocean mixed layer. ◼ Sea-surface temperature at least 26.5C. ◼ Mixed layer depth of 45 meters or more. Relative maxima in absolute vorticity in the lower troposphere ◼ Need a preexisting cyclonic disturbance. ◼ Must be more than a few degrees of latitude from the Equator. Small values of vertical wind shear. ◼ Disturbance must be in deep easterly flow, or in a region of light upper- level winds. Mean upward vertical motion with humid mid-levels. GLOBAL CLIMATOLOGY Note: Most of the statistics given in this section are from Gray, W.M., 1985: Tropical Cyclone Global Climatology, WMO Technical Document WMO/TD-72, Vol. I, 1985. About 80 tropical cyclones per year world-wide reach tropical storm strength ( 34 kts). About 50 – 55 each year world-wide reach hurricane/typhoon strength ( 64 kts). The rate of occurrence globally is very steady. Global average annual variation is small (about 7%). Extreme variations are in the range of 16 to 22%. Variability within a particular region is much larger than global variability. Most (87%) form within 20 of the Equator. -
THE Official Magazine of the OCEANOGRAPHY SOCIETY
OceThe OFFiciaaL MaganZineog OF the Oceanographyra Spocietyhy CITATION Jackson, C.R., J.C.B. da Silva, and G. Jeans. 2012. The generation of nonlinear internal waves. Oceanography 25(2):108–123, http://dx.doi.org/10.5670/oceanog.2012.46. DOI http://dx.doi.org/10.5670/oceanog.2012.46 COPYRIGHT This article has been published inOceanography , Volume 25, Number 2, a quarterly journal of The Oceanography Society. Copyright 2012 by The Oceanography Society. All rights reserved. USAGE Permission is granted to copy this article for use in teaching and research. Republication, systematic reproduction, or collective redistribution of any portion of this article by photocopy machine, reposting, or other means is permitted only with the approval of The Oceanography Society. Send all correspondence to: [email protected] or The Oceanography Society, PO Box 1931, Rockville, MD 20849-1931, USA. doWNLoaded From http://WWW.tos.org/oceanography SPECIAL ISSUE On InTERNAL WAVES BY CHRISTOPHER R. JACKSON, JOSÉ C.B. Da SILVA, AND GUS JEANS THE GENERATION OF NONLINEAR InTERNAL WAVES ABSTRACT. Nonlinear internal waves are found in many parts of the world ocean. Their widespread distribution is a result of their origin in the barotropic tide and in the variety of ways they can be generated, including by lee waves, tidal beams, resonance, plumes, and the transformation of the internal tide. The differing generation mechanisms and diversity of generation locations and conditions all combine to produce waves that range in scale from a few tens of meters to kilometers, but with all properly described by solitary wave theory. The ability of oceanic nonlinear internal waves to persist for days after generation and the key role internal waves play in connecting large-scale tides to smaller-scale turbulence make them important for understanding the ocean environment.