Surface Cyclolysis in the North Pacific Ocean. Part I
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Air Masses and Fronts
CHAPTER 4 AIR MASSES AND FRONTS Temperature, in the form of heating and cooling, contrasts and produces a homogeneous mass of air. The plays a key roll in our atmosphere’s circulation. energy supplied to Earth’s surface from the Sun is Heating and cooling is also the key in the formation of distributed to the air mass by convection, radiation, and various air masses. These air masses, because of conduction. temperature contrast, ultimately result in the formation Another condition necessary for air mass formation of frontal systems. The air masses and frontal systems, is equilibrium between ground and air. This is however, could not move significantly without the established by a combination of the following interplay of low-pressure systems (cyclones). processes: (1) turbulent-convective transport of heat Some regions of Earth have weak pressure upward into the higher levels of the air; (2) cooling of gradients at times that allow for little air movement. air by radiation loss of heat; and (3) transport of heat by Therefore, the air lying over these regions eventually evaporation and condensation processes. takes on the certain characteristics of temperature and The fastest and most effective process involved in moisture normal to that region. Ultimately, air masses establishing equilibrium is the turbulent-convective with these specific characteristics (warm, cold, moist, transport of heat upwards. The slowest and least or dry) develop. Because of the existence of cyclones effective process is radiation. and other factors aloft, these air masses are eventually subject to some movement that forces them together. During radiation and turbulent-convective When these air masses are forced together, fronts processes, evaporation and condensation contribute in develop between them. -
Extratropical Cyclones and Anticyclones
© Jones & Bartlett Learning, LLC. NOT FOR SALE OR DISTRIBUTION Courtesy of Jeff Schmaltz, the MODIS Rapid Response Team at NASA GSFC/NASA Extratropical Cyclones 10 and Anticyclones CHAPTER OUTLINE INTRODUCTION A TIME AND PLACE OF TRAGEDY A LiFE CYCLE OF GROWTH AND DEATH DAY 1: BIRTH OF AN EXTRATROPICAL CYCLONE ■■ Typical Extratropical Cyclone Paths DaY 2: WiTH THE FI TZ ■■ Portrait of the Cyclone as a Young Adult ■■ Cyclones and Fronts: On the Ground ■■ Cyclones and Fronts: In the Sky ■■ Back with the Fitz: A Fateful Course Correction ■■ Cyclones and Jet Streams 298 9781284027372_CH10_0298.indd 298 8/10/13 5:00 PM © Jones & Bartlett Learning, LLC. NOT FOR SALE OR DISTRIBUTION Introduction 299 DaY 3: THE MaTURE CYCLONE ■■ Bittersweet Badge of Adulthood: The Occlusion Process ■■ Hurricane West Wind ■■ One of the Worst . ■■ “Nosedive” DaY 4 (AND BEYOND): DEATH ■■ The Cyclone ■■ The Fitzgerald ■■ The Sailors THE EXTRATROPICAL ANTICYCLONE HIGH PRESSURE, HiGH HEAT: THE DEADLY EUROPEAN HEAT WaVE OF 2003 PUTTING IT ALL TOGETHER ■■ Summary ■■ Key Terms ■■ Review Questions ■■ Observation Activities AFTER COMPLETING THIS CHAPTER, YOU SHOULD BE ABLE TO: • Describe the different life-cycle stages in the Norwegian model of the extratropical cyclone, identifying the stages when the cyclone possesses cold, warm, and occluded fronts and life-threatening conditions • Explain the relationship between a surface cyclone and winds at the jet-stream level and how the two interact to intensify the cyclone • Differentiate between extratropical cyclones and anticyclones in terms of their birthplaces, life cycles, relationships to air masses and jet-stream winds, threats to life and property, and their appearance on satellite images INTRODUCTION What do you see in the diagram to the right: a vase or two faces? This classic psychology experiment exploits our amazing ability to recognize visual patterns. -
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. -
Types of Fronts Stationary Front a Front That Is Not Moving
Types of Fronts Stationary front A front that is not moving. Types of Fronts Cold front is a leading edge of colder air that is replacing warmer air. Types of Fronts Warm front is a leading edge of warmer air that is replacing cooler air. Types of Fronts Occluded front: When a cold front catches up to a warm front. Types of Fronts Dry Line Separates a moist air mass from a dry air mass. A.Cold Front is a transition zone from warm air to cold air. A cold front is defined as the transition zone where a cold air mass is replacing a warmer air mass. Cold fronts generally move from northwest to southeast. The air behind a cold front is noticeably colder and drier than the air ahead of it. When a cold front passes through, temperatures can drop more than 15 degrees within the first hour. The station east of the front reported a temperature of 55 degrees Fahrenheit while a short distance behind the front, the temperature decreased to 38 degrees. An abrupt temperature change over a short distance is a good indicator that a front is located somewhere in between. B. Warm Front. • A transition zone from cold air to warm air. • A warm front is defined as the transition zone where a warm air mass is replacing a cold air mass. Warm fronts generally move from southwest to northeast . The air behind a warm front is warmer and more moist than the air ahead of it. When a warm front passes through, the air becomes noticeably warmer and more humid than it was before. -
Piecewise Potential Vorticity Diagnosis of a Rapid Cyclolysis Event
1264 MONTHLY WEATHER REVIEW VOLUME 130 Surface Cyclolysis in the North Paci®c Ocean. Part II: Piecewise Potential Vorticity Diagnosis of a Rapid Cyclolysis Event JONATHAN E. MARTIN AND NATHAN MARSILI Department of Atmospheric and Oceanic Sciences, University of WisconsinÐMadison, Madison, Wisconsin (Manuscript received 19 March 2001, in ®nal form 26 October 2001) ABSTRACT Employing output from a successful numerical simulation, piecewise potential vorticity inversion is used to diagnose a rapid surface cyclolysis event that occurred south of the Aleutian Islands in late October 1996. The sea level pressure minimum of the decaying cyclone rose 35 hPa in 36 h as its associated upper-tropospheric wave quickly acquired a positive tilt while undergoing a rapid transformation from a nearly circular to a linear morphology. The inversion results demonstrate that the upper-tropospheric potential vorticity (PV) anomaly exerted the greatest control over the evolution of the lower-tropospheric height ®eld associated with the cyclone. A portion of the signi®cant height rises that characterized this event was directly associated with a diminution of the upper-tropospheric PV anomaly that resulted from negative PV advection by the full wind. This forcing has a clear parallel in more traditional synoptic/dynamic perspectives on lower-tropospheric development, which emphasize differential vorticity advection. Additional height rises resulted from promotion of increased anisotropy in the upper-tropospheric PV anomaly by upper-tropospheric deformation in the vicinity of a southwesterly jet streak. As the PV anomaly was thinned and elongated by the deformation, its associated geopotential height perturbation decreased throughout the troposphere in what is termed here PV attenuation. -
Weather Fronts
Weather Fronts Dana Desonie, Ph.D. Say Thanks to the Authors Click http://www.ck12.org/saythanks (No sign in required) AUTHOR Dana Desonie, Ph.D. To access a customizable version of this book, as well as other interactive content, visit www.ck12.org CK-12 Foundation is a non-profit organization with a mission to reduce the cost of textbook materials for the K-12 market both in the U.S. and worldwide. Using an open-source, collaborative, and web-based compilation model, CK-12 pioneers and promotes the creation and distribution of high-quality, adaptive online textbooks that can be mixed, modified and printed (i.e., the FlexBook® textbooks). Copyright © 2015 CK-12 Foundation, www.ck12.org The names “CK-12” and “CK12” and associated logos and the terms “FlexBook®” and “FlexBook Platform®” (collectively “CK-12 Marks”) are trademarks and service marks of CK-12 Foundation and are protected by federal, state, and international laws. Any form of reproduction of this book in any format or medium, in whole or in sections must include the referral attribution link http://www.ck12.org/saythanks (placed in a visible location) in addition to the following terms. Except as otherwise noted, all CK-12 Content (including CK-12 Curriculum Material) is made available to Users in accordance with the Creative Commons Attribution-Non-Commercial 3.0 Unported (CC BY-NC 3.0) License (http://creativecommons.org/ licenses/by-nc/3.0/), as amended and updated by Creative Com- mons from time to time (the “CC License”), which is incorporated herein by this reference. -
A Review of Convective and Artificial Vortices for Power Generation
A.T. Mustafa et al., Int. J. Sus. Dev. Plann. Vol. 10, No. 5 (2015) 650–665 A REVIEW OF CONVECTIVE AND ARTIFICIAL VORTICES FOR POWER GENERATION A.T. MUSTAFA, H.H. AL-KAYIEM & S.I.U. GILANI Department of Mechanical Engineering, Universiti Teknologi PETRONAS, Malaysia 31750 Tronoh, Perak, Malaysia. ABSTRACT Thermal energy transfer in the atmosphere occurs from a high temperature zone to a low one by means of convective vortices where mechanical energy is produced. There are two ways of driving vertical flow in the core of a vortex: (1) by the direct action of buoyancy acting on hot air and (2) by producing a vertical pressure gradient along the axis of a vortex because of core development involving the lateral spread of the vortex with height. In particular, it indicates that the intensity of convective vortices depends on the depth of the convec- tive layer via thermodynamic efficiency, the enthalpy perturbation across them, and the existence of sources of vorticity. The atmospheric vortex engine (AVE) is a device for producing an artificial vortex. The operation of AVE is based on the fact that the atmosphere is heated from the bottom and cooled at the top. By artificial vortex generation, it is aimed to eliminate the physical solar updraft tower and reduce the capital cost of solar chimney power plants. This paper reviews natural convective vortices and vortex creation via physical prin- ciples of vortex generation. Vortex analysis and modelling are presented. Furthermore, a new model of a solar vortex engine (SVE) is proposed and discussed. An idea on utilizing the solar energy as the heat source for establishing the vortex and operating the SVE model is adopted. -
The Rapid Growth and Decay of an Extratropical Cyclone Over the Central Paci®C Ocean
358 WEATHER AND FORECASTING VOLUME 19 The Rapid Growth and Decay of an Extratropical Cyclone over the Central Paci®c Ocean JONATHAN E. MARTIN Department of Atmospheric and Oceanic Sciences, University of WisconsinÐMadison, Madison, Wisconsin JASON A. OTKIN Cooperative Institute for Meteorological Satellite Studies, Space Science and Engineering Center, University of WisconsinÐMadison, Madison, Wisconsin (Manuscript received 22 April 2003, in ®nal form 6 November 2003) ABSTRACT The life cycle of a central Paci®c cyclone, characterized by a 48-h interval of rapid ¯uctuation in its intensity, is examined. The cyclone of interest underwent a period of explosive cyclogenesis from 1200 UTC 4 November to 1200 UTC 5 November 1986, followed 12 h later by a period of unusually rapid decay. Output from a numerical simulation of this event, run using the ®fth-generation Pennsylvania State University±National Center for Atmospheric Research (PSU±NCAR) Mesoscale Model (MM5), is used to perform a piecewise potential vorticity (PV) inversion in order to diagnose the life cycle of this unusual cyclone. The analysis reveals that the presence of lower-tropospheric frontogenetic forcing in an environment char- acterized by reduced static stability (as measured by high values of the K index) produced a burst of heavy precipitation during the development stage of the cyclone's life cycle. The associated latent heat release produced a substantial diabatic PV anomaly in the middle troposphere that was, in turn, responsible for the majority of the lower-tropospheric height falls associated with the explosive cyclogenesis. Subsequent height rises during the rapid cyclolysis stage resulted from the northward migration of the surface cyclone into a perturbation geopotential ridge associated with a negative tropopause-level PV anomaly. -
Absorption Abyssal Circulation Acoustic Measurements/Effects
1 Absorption 2 Abyssal circulation 3 Acoustic measurements/effects 4 Adaptation 5 Adaptive models 6 Advection 7 Aerosols/particulates 8 Aerosol hygroscopicity 9 Aerosol indirect effect 10 Aerosol nucleation 11 Aerosol optical properties 12 Aerosol radiative effect 13 Aerosol-cloud interaction 14 Africa 15 Ageostrophic circulations 16 Agriculture 17 Air pollution 18 Air quality 19 Air quality and climate 20 Air quality and health 21 Air quality forecasts 22 Air quality trends 23 Aircraft observations 24 Airflow 25 Airshed modeling 26 Air-sea interaction 27 Albedo 28 Algorithms 29 Altimetry 30 Amazon region 31 Anelastic models 32 Angular momentum 33 Animal studies 34 Annual variations 35 Annular mode 36 Anomalies 37 Antarctic Oscillation 38 Antarctica 39 Anthropogenic effects/forcing 40 Anticyclones 41 Aqueous-phase chemistry 42 Arctic 43 Arctic Oscillation 44 Artificial intelligence 45 Asia 46 Asymmetry 47 Atlantic Ocean 48 Atmosphere 49 Atmosphere-land interaction 50 Atmosphere-ocean interaction 51 Atmospheric circulation 52 Atmospheric composition 53 Atmospheric electricity 54 Atmospheric oxidation 55 Atmospheric river 56 Australia 57 Automated systems 58 Automatic weather stations 59 Baroclinic flows 60 Baroclinic models 61 Barotropic flows 62 Bayesian methods 63 Behavioral models 64 Bias 65 Biennial oscillation 66 Biofouling 67 Biomass burning 68 Biosphere emissions 69 Biosphere-atmosphere interactions 70 Blocking 71 Boreal meteorology 72 Bottom currents/bottom water 73 Boundary conditions 74 Boundary currents 75 Boundary layer 76 -
Lecture 14. Extratropical Cyclones • in Mid-Latitudes, Much of Our Weather
Lecture 14. Extratropical Cyclones • In mid-latitudes, much of our weather is associated with a particular kind of storm, the extratropical cyclone Cyclone: circulation around low pressure center Some midwesterners call tornadoes cyclones Tropical cyclone = hurricane • Extratropical cyclones derive their energy from horizontal temperature con- trasts. • They typically form on a boundary between a warm and a cold air mass associated with an upper tropospheric jet stream • Their circulations affect the entire troposphere over a region 1000 km or more across. • Extratropical cyclones tend to develop with a particular lifecycle . • The low pressure center moves roughly with the speed of the 500 mb wind above it. • An extratropical cyclone tends to focus the temperature contrasts into ‘fron- tal zones’ of particularly rapid horizontal temperature change. The Norwegian Cyclone Model In 1922, well before routine upper air observations began, Bjerknes and Sol- berg in Bergen, Norway, codified experience from analyzing surface weather maps over Europe into the Norwegian Cyclone Model, a conceptual picture of the evolution of an ET cyclone and associated frontal zones at ground They noted that the strongest temperature gradients usually occur at the warm edge of the frontal zone, which they called the front. They classified fronts into four types, each with its own symbol: Cold front - Cold air advancing into warm air Warm front - Warm air advancing into cold air Stationary front - Neither airmass advances Occluded front - Looks like a cold front -
Extreme Wet Seasons – Their Definition and Relationship with Synoptic-Scale
Weather Clim. Dynam., 2, 71–88, 2021 https://doi.org/10.5194/wcd-2-71-2021 © Author(s) 2021. This work is distributed under the Creative Commons Attribution 4.0 License. Extreme wet seasons – their definition and relationship with synoptic-scale weather systems Emmanouil Flaounas, Matthias Röthlisberger, Maxi Boettcher, Michael Sprenger, and Heini Wernli Institute for Atmospheric and Climate Science, ETH Zurich, Zurich, Switzerland Correspondence: Emmanouil Flaounas (emmanouil.fl[email protected]) Received: 30 June 2020 – Discussion started: 8 July 2020 Revised: 24 December 2020 – Accepted: 13 January 2021 – Published: 1 February 2021 Abstract. An extreme aggregation of precipitation on the But interlatitudinal influences are also shown to be impor- seasonal timescale, leading to a so-called extreme wet sea- tant: tropical moisture exports, i.e., the poleward transport son, can have substantial environmental and socio-economic of tropical moisture, can contribute to extreme wet seasons impacts. This study has a twofold aim: first to identify and in the midlatitudes, while breaking Rossby waves, i.e., the statistically characterize extreme wet seasons around the equatorward intrusion of stratospheric air, may decisively globe and second to elucidate their relationship with specific contribute to the formation of extreme wet seasons in the weather systems. tropics. Three illustrative examples provide insight into the Extreme wet seasons are defined independently at every synergetic effects of the four identified weather systems on grid point of ERA-Interim reanalyses as the consecutive 90 d the formation of extreme wet seasons in the midlatitudes, the period with the highest accumulated precipitation in the 40- Arctic and the (sub)tropics. -
ESCI 107 – the Atmosphere Lesson 13 – Fronts and Midlatitude Cyclones
ESCI 107 – The Atmosphere Lesson 13 – Fronts and Midlatitude Cyclones Reading: Meteorology Today , Chapters 11 and 12 GENERAL A front is a boundary between two air masses. ο Usually there is a sharp temperature contrast across a front. ο There is often also a contrast in moisture across a front. ο There is a shift in wind direction across a front. Because the two air masses have different temperatures and different humidities they are of different density. The lighter air mass will overrun the denser air mass, which causes lifting along the frontal zone. This is why fronts are associated with clouds and precipitation. Because air masses are associated with areas of high pressure, and fronts separate these air masses, fronts themselves lie in regions of low pressure, or troughs. THE POLAR FRONT The polar front is a nearly continuous front that separates the polar easterly winds from the midlatitude westerlies. The position of the polar front is closely approximated by the position of the polar jet stream When a low-pressure system forms on the polar front then ο on the west side of the low, cold air is pushed southward as a cold front ο on the east side of the low, warm air is pushed northward as a warm front WARM FRONTS Warm air advances into region formerly covered by cold air. Weather map symbol is red line with circular teeth. Warm air rides up and over cold air. The frontal surface slopes very shallowly with height (about 1:200). The front moves forward at 15 - 20 mph.