GH = Differential temperature advection term

Similar documents
Dynamics of Upper-Level Waves

Fundamental Meteo Concepts

Synoptic-Dynamic Meteorology in Midlatitudes

Quasi-Geostrophic Implications

Cyclones and Anticyclones, Ridges and Troughs

Final Examination, MEA 443 Fall 2008, Lackmann

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points.

Synoptic Meteorology II: Petterssen-Sutcliffe Development Theory Application March 2015

Use of dynamical concepts in weather forecasting

Characteristic blocking events over Ural-Siberia in Boreal Winter under Present and Future Climate Conditions

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points.

Diabatic processes and the structure of the warm conveyor belt

(! g. + f ) Dt. $% (" g. + f ) + f

THE EXTRATROPICAL TRANSITION OF TYPHOON WINNIE (1997): SELF-AMPLIFICATION AFTER LANDFALL

Geopotential tendency and vertical motion

Isentropic Analysis. Much of this presentation is due to Jim Moore, SLU

Synoptic Meteorology II: Self-Development in the IPV Framework. 5-7 May 2015

Occlusion cyclogenesis II

DANISH METEOROLOGICAL INSTITUTE

Meteorology Lecture 15

Errata: Midlatitude Synoptic Meteorology (July, 2014)

Example of the "Vorticity Advection" Pitfall

Height Tendency Diagnostics Using a Generalized Omega Equation, the Vorticity Equation, and a Nonlinear Balance Equation

Divergence, Spin, and Tilt. Convergence and Divergence. Midlatitude Cyclones. Large-Scale Setting

Lower-Tropospheric Height Tendencies Associated with the Shearwise and Transverse Components of Quasigeostrophic Vertical Motion

NOTES AND CORRESPONDENCE

10B.2 THE ROLE OF THE OCCLUSION PROCESS IN THE EXTRATROPICAL-TO-TROPICAL TRANSITION OF ATLANTIC HURRICANE KAREN

Interaction of Potential Vorticity Anomalies in Extratropical Cyclogenesis. Part I: Static Piecewise Inversion

Nonlinear baroclinic dynamics of surface cyclones crossing a zonal jet

Synoptic Meteorology II: Potential Vorticity Inversion and Anomaly Structure April 2015

Cyclolysis: A Diagnosis of Two Extratropical Cyclones

Quasi-Geostrophic ω-equation. 1. The atmosphere is approximately hydrostatic. 2. The atmosphere is approximately geostrophic.

Jacob Bjerknes Halvor Solberg Tor Bergeron

A Cyclogenesis south of the Alps. Manfred Kurz Neustadt/Weinstraße

Jacob Bjerknes Halvor Solberg Tor Bergeron

Suggested reading: Lackmann (2011), Sections

Name SOLUTIONS T.A./Section Atmospheric Science 101 Homework #6 Due Thursday, May 30 th (in class)

Using simplified vorticity equation,* by assumption 1 above: *Metr 430 handout on Circulation and Vorticity. Equations (4) and (5) on that handout

Dynamic Meteorology 1

Isentropic Thinking & Airstreams Analysis

A more detailed and quantitative consideration of organized convection: Part I Cold pool dynamics and the formation of squall lines

Tropical Cyclone Formation/Structure/Motion Studies

p. 4, 1 st two lines should read: k-hat unit vector maintains right angles with the horizontal unit vectors.

Observational climatology and characteristics of wintertime atmospheric blocking over Ural Siberia

P1.52 AN EXAMINATION OF JUPITER S GREAT RED SPOT AND OTHER VORTICES USING THE EPIC MODEL 2. DATA

Lec 10: Interpreting Weather Maps

Description of the ET of Super Typhoon Choi-Wan (2009) based on the YOTC-dataset

Aviation Hazards: Thunderstorms and Deep Convection

Diabatic processes and the structure of extratropical cyclones

A new look at the w-equation

3. Midlatitude Storm Tracks and the North Atlantic Oscillation

Fixed Rossby Waves: Quasigeostrophic Explanations and Conservation of Potential Vorticity

Diabatic processes modifying potential vorticity in a North Atlantic cyclone

THE INFLUENCE OF ROTATIONAL FRONTOGENESIS AND ITS ASSOCIATED SHEARWISE VERTICAL MOTIONS ON THE DEVELOPMENT OF AN UPPER-LEVEL FRONT

P5.7 A COMPREHENSIVE CLIMATOLOGY OF APPALACHIAN COLD AIR DAMMING. Christopher M. Bailey + Gary M. Lackmann + Gail Hartfield* Kermit Keeter*

Diagnostic Study of a Severe Thunderstorm over Jeddah

ATM OCN 452. The Frontal Cyclone. Fall 2013

San Francisco State University Department of Earth & Climate Sciences Fall 2017

Vertical structure. To conclude, we will review the critical factors invloved in the development of extratropical storms.

Interpreting Petterssen s Extratropical Cyclone* Self-Development Eqn. (based in part on notes by James T. Moore)

Introduction to Conceptual Models

Middle-Latitude Cyclone

Chapter 10: Mid-latitude Cyclones Mid-Latitude Cyclones

Chapter 10: Mid-latitude Cyclones

Fall 2015 Laboratory 7 Quasigeostrophic Forcing Functions 300 points. You are provided with the following for 12 UTC 12/4/12 (a) WRF-NAM

Origin of the Summertime Synoptic-Scale Wave Train in the Western North Pacific*

Atmospheric dynamics and meteorology

Multiscale Analyses of Inland Tropical Cyclone Midlatitude Jet Interactions: Camille (1969) and Danny (1997)

Mid-Latitude Cyclones and Fronts. Lecture 12 AOS 101

DYNAMICAL STRUCTURES AND PRECIPITATION DISTRIBUTIONS OF TRANSITIONING TROPICAL CYCLONES IN EASTERN CANADA,

The purpose of this thesis is to present two multiscale analyses of inland tropical

Measurement of Rotation. Circulation. Example. Lecture 4: Circulation and Vorticity 1/31/2017

2015/16 Winter Monsoon in East Asia

AN EXTRATROPICAL CYCLONE ATLAS

The Extratropical Transition of Tropical Cyclones

1/25/2010. Circulation and vorticity are the two primary

Middle Latitude Cyclones a storm that forms at middle and high latitudes, outside of the tropics.

and 24 mm, hPa lapse rates between 3 and 4 K km 1, lifted index values

CONVERGENCE, DIVERGENCE, AND VORTICITY

Part 4. Atmospheric Dynamics

THE LOW-LEVEL JET FOR BUCHAREST S AIRPORTS - A STUDY OF ITS CHARACTERISTICS IN WINTER SEASON BETWEEN 1959 AND 1982

Diagnostics of the prediction and maintenance of Euro-Atlantic blocking

Upper-tropospheric downstream development leading to surface cyclogenesis in the central Mediterranean

On studying the structure of synoptic systems

Weather report 28 November 2017 Campinas/SP

EAS372 Open Book Final Exam 11 April, 2013

Accuracy of GFS Forecasts: An Examination of High-Impact Cold Season Weather Events

Mid-troposphere variables and their association with daily local precipitation

Mesoscale Frontal Waves Associated with Landfalling Atmospheric Rivers

Orographic Cyclogenesis and the Influence of Mountains on Extratropical Cyclones. Learning Objectives. Outline. Climatological Context

Severe weather. Some case studies for medium-range forecasting. T. La Rocca, Department of Synoptic Meteorology, Italian Met. Service, Rome.

Review of Norwegian Cyclone Model and ISU weather data analysis software. Meteorology 411 Iowa State University Week 1 Bill Gallus

Mesoscale Meteorology Assignment #3 Q-G Theory Exercise. Due 23 February 2017

1/18/2011. From the hydrostatic equation, it is clear that a single. pressure and height in each vertical column of the atmosphere.

1. Rossby and Ertel 2. Conservation and invertibility - a useful combination 2.1 Action at a distance

Analysis of the December 26 th, 2004 North Carolina Winter Storm

Victor Homar * and David J. Stensrud NOAA/NSSL, Norman, Oklahoma

Revisiting the Structure and Characteristics of an Early Summer Monsoon Trough over South China in 1975

Relationships between Large-Scale Regime Transitions and Major Cool-Season Precipitation Events in the Northeastern United States

18.6 COLD-AIR DAMMING EROSION: PHYSICAL MECHANISMS, SYNOPTIC SETTINGS, AND MODEL REPRESENTATION

Transcription:

QG Theory and Applications: Height Tendency Equation Atmos 5110 Synoptic Dynamic Meteorology I Instructor: Jim Steenburgh jim.steenburgh@utah.edu 801-581-8727 Suite 480/Office 488 INSCC Suggested reading: Lackmann (2011), Section 2.4 Usage The QG height tendency equation is used to understand and diagnose the development and decay of large-scale weather systems. Derivation Derived from the QG thermodynamic and vorticity equations. See Lackmann (2011) for details. The Height tendency Equation! # + p (f ) # p )- χ = f )V2 4 6 1 # Φ + f9 f ) p! f ) V 2 4 6 Φ p 9- # Yeah, it s daunting, but easier if you think of it as A=B+C where: χ = :; :> :< :< (Geopotential Tendency) A =! # + p (f ) # )- χ p B = f 0 V2 g 6 1 f 0 2 Φ + f9 = Vorticity advection term C = E f 2 0 V 2 g F Φ GH = Differential temperature advection term p p ***Note that these terms are not synonymous with the differential vorticity advection and temperature advection terms of the omega equation 1

Term A Essentially the 3-D Laplacian acting on χ. For sinusoidal (wave-like) patterns, the Laplacian can be approximated by a minus sign. A =! # + p (f ) # Z )- χ ~ χ p t, Z t f )V2 4 6 1 # Φ + f9 f ) p! f # ) V 2 4 6 Φ p 9- Term B Vorticity advection term Z t f )V2 4 6 1 f ) # Φ + f9 Z t L f )V2 4 6 1 f ) # Φ + f9m Cyclonic vorticity advection (positive in NH) results in falling heights Anticyclonic vorticity advection (negative in NH) results in rising heights Typically evaluate @ 500 mb 2

Term C Temperature advection term Z t p! f # ) V 2 4 6 Φ p 9- # Z t p! f ) V 2 4 6 Φ p 9- z O V 2 4 TQ Positive differential temperature advection results in height falls Negative differential temperature advection results in height rises Examples 3

Term C in practice Warm advection above an upper-level trough tends to deepen the trough Cold advection beneath an upper-level trough tends to deepen the trough Best case for trough amplification is upper-level warm advection and lowerlevel cold advection Cold advection above an upper-level ridge tends to build the ridge Warm advection beneath an upper-level ridge tends to build the ridge Best case for ridge amplification is upper-level cold advection and lower level warm advection Rules of thumb are shortcuts ultimately how the temperature advection changes with height is what matters Class Activity Using the IDV Diagnostics -> QG-HeightTend bundle, evaluate the right-hand terms and 500-mb height tendency over North America over the past two days. Be sure to examine the differential temperature advection by examining multiple levels and using the vertical probe. Additional applications The height tendency equation is sometimes used to diagnose low-level cyclone and anticyclone development: Warm advection above a surface cyclone (e.g., @ 850 mb) will tend to deepen the cyclone Cold advection above a surface anticyclone will tend to deepen the anticyclone Diabatic effects If diabatic effects are considered, then the height tendency equation contains an additional term that implies: 4

Z t J, where J = diabatic heating rate z Positive differential diabatic heating yields height falls Negative differential diabatic heating yields height rises Synoptic Application A maximum in condensational warming in the lower-to-middle tropospheric height falls and upper-level height rises important in cyclogenesis! 5