Basic Jet Streak Adjustments & Frontogenesis MEA 444 January 13, 2005.

Slides:



Advertisements
Similar presentations
The Quasi-Geostrophic Omega Equation (without friction and diabatic terms) We will now develop the Trenberth (1978)* modification to the QG Omega equation.
Advertisements

SO441 Synoptic Meteorology Extratropical cyclones Visible satellite image 26 Oct Low pressure mb. Image courtesy NASA Cloud pattern typically.
Squall Lines Loosely defined: A line of either ordinary cells or supercells of finite length (10- hundreds of km) that may contain a stratiform rain region.
Stratus. Outline  Formation –Moisture trapped under inversion –Contact layer heating of fog –Fog induced stratus –Lake effect stratus/strato cu  Dissipation.
SO441 Synoptic Meteorology Fronts Lesson 8: Weeks Courtesy: Lyndon State College.
Conceptual Models of Cold Fronts: Anacoldfront Katacoldfront.
The Temporal Behavior of Numerically Simulated Multicell- Type Storms. Part II: The Convective Life Cycle and Cell Regeneration RobertG. Fovell and Pei-Hua.
Atmospheric Destabilization Processes Upper Level Mixed Layer Synoptic Lifting Dynamic Destabilization Differential Advection.
Cold Front Aloft Model Comments The lower portions of Pacific weather systems are destroyed as they cross the Rockies. The upper short-wave and its associated.
Midlatitude Cyclones Equator-to-pole temperature gradient tilts pressure surfaces and produces westerly jets in midlatitudes Waves in the jet induce divergence.
Chapter 10 Mid-latitude Cyclones Chapter 10 Mid-latitude Cyclones.
Extratropical Cyclones – Genesis, Development, and Decay Xiangdong Zhang International Arctic Research Center.
Convective Dynamics Squall Lines Adapted from material from the COMET Program.
General Circulation and Kinetic Energy
A Compare and Contrast Study of Two Banded Snow Storms Part I – January 6 th, 2002.
A brief synopsis of Johnson and Mapes: Mesoscale Processes and Severe Convective Weather From Severe Convective Storms sections 3.3b, 3.3c.1, 3.4 By Matt.
Fronts and Mid-latitude Cyclones
Extratropical Synoptic-Scale Processes and Severe Convection John Monteverdi Doswell, C.A. III, and L.F. Bosart, 2001: Extratropical synoptic-scale processes.
Jet Streams.
THE DISTINCTION BETWEEN LARGE- SCALE AND MESOSCALE CONTRIBUTION TO SEVERE CONVECTION: A CASE STUDY EXAMPLE Paper by Charles A. Doswell III Powerpoint by.
Drylines By: Allie Vegh. Definition: A dryline is a zone of strong horizontal moisture gradient separating warm, moist air from hot, dry air in the boundary.
Mesoscale Processes and Severe Convective Weather Richard H. Johnson and Brian E. Mapes Presentation by Chris Medjber Severe Convective Storms, Meteorological.
Typhoons and tropical cyclones
Section 3.5, 3.5a, 3.5b Overview For Storm-generated Mesoscale processes 1.Local Effects 2.Advective Effects.
Upper-Level Frontogenesis Cliff Mass University of Washington.
Second MSC/COMET Winter Weather Course, Boulder, Slantwise Convection: An Operational Approach The Release of Symmetric Instability.
Air Masses and Fronts – II. Brief review An air mass is a large body of air whose properties of temperature and humidity are fairly similar in any horizontal.
Depression 2/M John R. Jaromahum. Depressions  or 'lows' play an important part in the weather  tending to bring rain and strong winds. Depressions.
The Ageostrophic Wind Equation Remember from before: – The “forcing” terms in the QG omega equation are geostrophic – “Weather” results from ageostrophic.
II. Synoptic Atmospheric Destabilization Processes Elevated Mixed Layer (EML) Synoptic Lifting Dynamic Destabilization Differential Advection.
Model Simulations of Extreme Orographic Precipitation in the Sierra Nevada Phillip Marzette ATMS 790 March 12, 2007.
AOSS 401, Fall 2006 Lecture 19 October 26, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Formation of the Extratropical Cyclone (Cyclogenesis)
The simplest theoretical basis for understanding the location of significant vertical motions in an Eulerian framework is QUASI-GEOSTROPHIC THEORY QG Theory:
Split Fronts and Cold Fronts Aloft Steven Koch North Carolina State University COMAP 99 Monday, 9 August 1999.
Mesoscale Instabilities James T. Moore Cooperative Institute for Precipitation Systems Saint Louis University Dept. of Earth & Atmospheric Sciences
PRECIPITATION PROCESSES AT FRONTS. POSSIBLE CONDITIONS PRESENT AT FRONT 1.Air ahead of the front is stable to all forms of instability Forcing mechanism.
Squall Lines Photographs © Todd LindleyTodd Lindley.
Fronts and Frontogenesis
Structure and dynamical characteristics of mid-latitude fronts.
ADVENTURE IN SYNOPTIC DYNAMICS HISTORY
Frontogenesis – Kinematics & Dynamics
13th Cyclone Workshop 25 October 2005 Pacific Grove, CA1 A Study of the Effect of Horizontal Contrasts in Static Stability on Frontal Behavior Mark T.
The Linear and Non-linear Evolution Mechanism of Mesoscale Vortex Disturbances in Winter Over Western Japan Sea Yasumitsu MAEJIMA and Keita IGA (Ocean.
The Use of Conceptual Models in the Forecast Process for Frontal Precipitation Events Steven Koch North Carolina State University COMAP 99 9 August 1999.
Overview of Tropical Cyclones AOS 453 April 2004 J. P. Kossin CIMSS/UW-Madison.
Section 8 Vertical Circulation at Fronts
ATS-113 Seven Day Snowfall Totals. Fronts Arise because different air masses don’t mix readily –When two air masses come in contact, they retain their.
Jets Dynamics Weather Systems – Fall 2015 Outline: a.Why, when and where? b.What is a jet streak? c.Ageostrophic flow associated with jet streaks.
Deep Convection, Severe Weather, and Appalachian Lee/Prefrontal Troughs Daniel B. Thompson, Lance F. Bosart and Daniel Keyser Department of Atmospheric.
ATS/ESS 452: Synoptic Meteorology Friday 08 January 2016 Review Material Overview of Maps Equations of Motion Advection Continuity.
Lecture 18 Lake Effect Storms. Homework Due Friday, December 12, 2014 TYU Ch 13: 2,4,,6, 7,18 ; TYPSS 3 TYU Ch 16: 1, 2, 3, 7, 11 ; TYPSS 2 Extra Credit,
Chapter 9 Winds: Small scale and local systems. Scales of motion Smallest - microscale (few meters or less) Middle - Mesoscale (few to about 100 km) Large.
1 This is the footer Midlatitude Weather systems Geraint Vaughan University of Manchester NCAS Director of Observations.
ATMS 316- Mesoscale Meteorology Packet#6 Interesting things happen at the boundaries, or at.
SO254 Extratropical cyclones
Instability Baroclinic instability (needs vertical shear,
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
A Compare and Contrast Study of Two Banded Snow Storms
Meteorología sinóptica
Dynamics of Thunderstorms Part 1: Downdraft Organization Lecture 12a
Atmospheric Destabilization Processes
Downdraft Storms Lecture 12a
Cyclogenesis in Polar Airstreams
The November 26, 2014 banded snowfall case in southern NY
Cold Frontal Zone N E Reproduced from Synoptic-Dynamic Meteorology in Midlatitudes, Vol. II.
The Course of Synoptic Meteorology
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
Mesoscale Dynamics Introduction.
Presentation transcript:

Basic Jet Streak Adjustments & Frontogenesis MEA 444 January 13, 2005

The Problem of Scale Interaction Definitions of Scales in the Atmosphere: (i) as deduced from observations (ii) as resulting from sizes of observational networks (iii) as defined by theoretical considerations (e.g., Lagrangian Time Scales)

Scale-interactive processes Synoptic forcing of mesoscale weather phenomena Generation of internal mesoscale instabilities Interactions of cloud and precipitation processes with mesoscale dynamics Influence of orography, boundary layer, and surface properties on mesoscale weather system development and evolution Feedback contributions of mesoscale systems to larger-scale processes Energy budgets associated with mesoscale systems Mechanisms and processes associated with statosphere-troposphere exchange.

Ageostrophic Motions Near Jets Straight JetUniform Jet

Frontogenesis Equation

Vorticity Tendency Eqns.

Vorticity Equations in Cartesian Coordinates

Stretching Deformation Confluence and diffluence associated with a jet maximum.

Shearing Deformation Horizontal Shear in the presence of a positive along-front temperature gradient.

Shearing

Stretching

Tilting

Diabatic Forcing

Katafronts The schematic diagram presented below is that of a katafront. The front-relative flow for a katafront is one in which the ascent core slopes forward, resulting in all the precipitation being prefrontal.

Anafronts The schematic diagram presented below is that of an anafront. The front-relative flow for an anafront is one in which the ascent core slopes rearwards over the top of the cold frontal surface, resulting in all the precipitation being postfrontal.

Cold Fronts Aloft A Cold Front Aloft (CFA) can be characterized as "the leading edge of a transition zone above the surface that separates advancing cold air from warmer air" (Locatelli, et al. 1995). Thus, a CFA is a cold frontal zone that is located in the lower to middle troposphere above the surface, but which has become split from the surface front. For example, this can happen when a front passes over a mountain range due to the drag from the topography on the surface front, particularly in combination with strong sensible heating over the elevated terrain, which can effectively erase the thermal structure of the low-level cold front.

Cold Fronts Aloft (cont'd.) A pronounced rainband is usually associated with the CFA, which in some instances is capable of producing severe weather hundreds of kilometers ahead of the surface front. This can create unanticipated consequences for the forecast process, such as: CFAs and attendant convective weather have been documented during Cold Air Damming events over the cooler air east of the Appalachians, when traditional logic would argue against the possibility of significant convection over such stably stratified air. CFAs have been shown to be responsible for generating lines of sever thunderstorms to the east of the dryline, and to thereafter support the continual eastward movement of the squall line for hundreds of miles ahead of the surface dryline. Evidence is accumulating that some CFAs are highly unbalanced phenomena. Thus, they can initiate a geostrophic adjustment process, during which a major gravity-inertia wave event can transpire.

History of CFAs The causes of "prefrontal squall lines" have been mysteries to meteorologists. Holzman (1936) and Lichtblau (1936): Most significant winter precipitation events in the Midwest are associated with CFAs. Crawford (1950): No prefrontal instability lines of any importance over the southeastern states exist without a warm tongue at 850 mb and strong cold advection at 700 mb. Browning (1985): Suggested that many squall lines in the Midwest might be associated with split CFAs. Locatelli et al. (1989): Discovered a CFA rainband that developed in the lee of the Rocky Mountains and moved eastward off the Atlantic Coast.

Useful Criteria for Labeling a Cold Front Aloft Main precipitation band is well ahead of a surface trough. Pronounce temperature gradient (cold advection) in the mid-troposphere associated with the band. Cloud band in satellite imagery well ahead of surface trough. Forecast vertical velocity field shows strong upward motion feature at least 200 km ahead of surface trough.

Useful Criteria for Labeling a Cold Front Aloft (cont'd.) Vertical cross section of θ e and winds indicates the presence of a mid-level front (CFA) ahead of the surface front. Geostrophic wind along the suspected CFA has a concentrated region of vertical and lateral shear revealed by the field of absolute momentum. Zero isodop in the radial velocity display from WSR-88D shows mid-level "backward S" pattern above a low-level "S"

CFA Model Rocky Mountains block eastward progress of cold air at low levels and destroy thermal contrast due to strong sensible heating. Cold air continues to advance at mid levels ahead of surface trough. Suggested that a thermally direct vertical circulation results from quasi-geostrophic frontogenesis, and ageostrophic isallobaric forcing at low levels due to the changing pressure gradient caused by cold advection aloft. The midlevel zone of frontogenesis well ahead of surface trough is shown to be capable of triggering prefrontal squall lines.

Split Cold Front When the surface pressure trough takes the form of a cold front with a line of maximum θ e running from the surface front to the base of the front aloft, we have a split cold front.

Cold Frontal Rainbands Strong lifting of the leading edge of the cold front produces a narrow band of heavy rainfall. The cold-frontal gradient of the surface is very different from the conventional synoptic conceptual model. Wider bands of precipitation exist behind the surface cold front. These can be associated with local steepening of the cold front. These wide bands have some similarities to surge rainbands such as their movement through the system and the local enhancement of the baroclinic zone (although wide bands have weaker circulations). The wide bands are also oriented along the vertical shear vector.

Process Leading to the Formation of Cold Frontal Rainbands