A Characterization of Atmospheric Blocking Huw C. Davies

Slides:



Advertisements
Similar presentations
Taher A. Sharif Department of Atmospheric science, University of AlFateh, Tripoli, Libya
Advertisements

© University of Reading TAC-3 Conference June 2012 The dependence of contrail formation on weather pattern and altitude.
Large-scale context for the UK floods in Summer 2007 Submitted to Weather, 14 May 2008 Mike Blackburn 1 John Methven 2 and Nigel Roberts 3 (1) National.
Mihir Kumar Dash*, Dhrubajyoti Samanta* and P. C. Pandey** * Indian Institute of Technology, Kharagpur * Indian Institute of Technology, Bhubaneswar.
Decadal Variation of the Holton-Tan Effect Hua Lu, Thomas Bracegirdle, Tony Phillips, Andrew Bushell DynVar/SNAP Workshops, April, 2013, Reading,
Extreme cold events over Asia: role of stratospheric wave reflection By Debashis Nath & Chen WEN International Workshop on High Impact weather Research.
Ocean’s Role in the Stratosphere-Troposphere Interaction Yulia A. Zyulyaeva Moscow State University P.P.Shirshov Institute of Oceanology, RAS, Moscow 1/17.
Annular Modes of Extra- tropical Circulation Judith Perlwitz CIRES-CDC, University of Colorado.
Potential vorticity and the dynamic tropopause
The influence of the stratosphere on tropospheric circulation and implications for forecasting Nili Harnik Department of Geophysics and Planetary Sciences,
Spring Onset in the Northern Hemisphere: A Role for the Stratosphere? Robert X. Black Brent A. McDaniel School of Earth and Atmospheric Sciences Georgia.
Blocking and Rossby Wave-breaking
Vorticity.
Pei-Yu Chueh 2010/7/1.  From 1948 to 2005 for DJF found decreases over the Arctic, Antarctic and North Pacific, an increase over the subtropical North.
Review of Northern Winter 2010/11
General circulation in the tropics
Contemporaneous and Antecedent Links of Atlantic and Pacific Circulation Features with North American Hydroclimate: Structure and Interannual Variability.
GLOBAL CHANGES IN OUR ATMOSPHERE: a top-down point of view  Atmospheric Science 101  Structure of atmosphere  Important relationships  The Northern.
Upper-Level Precursors Associated with Subtropical Cyclone Formation in the North Atlantic Alicia M. Bentley, Daniel Keyser, and Lance F. Bosart University.
Variability of Tropical to Extra-tropical Transport in the Lower Stratosphere Mark Olsen UMBC/GSFC Anne Douglass, Paul Newman, and Eric Nash.
Seasonal outlook of the East Asian Summer in 2015 Motoaki Takekawa Tokyo Climate Center Japan Meteorological Agency May th FOCRAII 1.
The speaker took this picture on 11 December, 2012 over the ocean near Japan. 2014/07/29 AOGS 11th Annual Meeting in Sapporo.
1 Introduction to Isentropic Coordinates: a new view of mean meridional & eddy circulations Cristiana Stan School and Conference on “the General Circulation.
Stratospheric harbingers of anomalous weather regimes. M.P. Baldwin and T.J Dunkerton Science, 294:581. Propagation of the Arctic Oscillation from.
Objectives:  Types of blocking ridges  Storms that typically accompany the block.  Numerical models and ensembles forecast these ridges as much as 10.
Part II: Where are we going? Like an ocean... The waves crash down... Introducing OCEAN ATMOSPHERE INTERACTION.
Trimodal distribution of ozone and water vapor in the UT/LS during boreal summer Timothy J Dunkerton NorthWest Research Associates WARM SEASON.
Teleconnections Current Weather Current Weather Finish ENSO Finish ENSO North Atlantic and Arctic Oscillations North Atlantic and Arctic Oscillations Pacific.
Large-scale surface wind extremes in the Mediterranean Shira Raveh-Rubin and Heini Wernli Institute for Atmospheric and Climate Science (IACETH), ETH Zurich.
1 IPV and the Dynamic Tropopause John W. Nielsen-Gammon Texas A&M University
The Modulation of Tropopause- level Wave Breaking by the Madden Julian Oscillation Richard Moore 1, Olivia Martius 2, Thomas Spengler 2 & Huw Davies 2.
Long-Term Changes in Northern and Southern Annular Modes Part I: Observations Christopher L. Castro AT 750.
COMET Feb. 20, 2002 IPV and the Dynamic Tropopause John W. Nielsen-Gammon1 Outline PV basics Seeing the world through PV Waves and vortices Nonconservation.
How do Long-Term Changes in the Stratosphere Affect the Troposphere?
NSF Proposal Impacts of Rossby Wave Breaking and Potential Vorticity Streamer Formation on the Environment of the Tropical and Subtropical North Atlantic.
Overview of 2012/2013 winter over South Korea
Characterization of the composition, structure, and seasonal variation of the mixing layer above the extratropical tropopause as revealed by MOZAIC measurements.
Applications of ‘IPV’ thinking for time-dependent dynamical processes (p. 202, Bluestein, 1993) The purpose of this discussion is to utilize ‘IPV’ thinking.
Dynamic tropopause analysis; What is the dynamic tropopause?
PAPER REVIEW R Kirsten Feng. Impact of global warming on the East Asian winter monsoon revealed by nine coupled atmosphere-ocean GCMs Masatake.
Modes of variability and teleconnections: Part II Hai Lin Meteorological Research Division, Environment Canada Advanced School and Workshop on S2S ICTP,
Rossby wave breaking (RWB) Definition Detection / Measurement Climatology Dynamics – Impact on internal variability (NAO / NAM) – Impact on surface turbulent.
Climate Variability and Basin Scale Forcing over the North Atlantic Jim Hurrell Climate and Global Dynamics Division National Center for Atmospheric Research.
Extreme Temperature Regimes during the Cool Season Robert X. Black Rebecca Westby School of Earth and Atmospheric Sciences Georgia Institute of Technology,
Madden/Julian Oscillation: Recent Evolution, Current Status and Forecasts Update prepared by Climate Prediction Center / NCEP April 5, 2005.
Day Meridional Propagation of Global Circulation Anomalies ( A Global Convection Circulation Paradigm for the Annular Mode) Ming Cai 1 and R-C.
Potential vorticity and the invertibility principle (pp ) To a first approximation, the atmospheric structure may be regarded as a superposition.
The impact of tropical convection and interference on the extratropical circulation Steven Feldstein and Michael Goss The Pennsylvania State University.
Teleconnections Current Weather Current Weather Finish ENSO Finish ENSO North Atlantic and Arctic Oscillations North Atlantic and Arctic Oscillations Pacific.
Potential Vorticity Streamers and Tropical Cyclogenesis During the 2007 North Atlantic Hurricane Season T. J. Galarneau 1, L. F. Bosart 1, and R. McTaggart-Cowan.
Impact of the representation of the stratosphere on tropospheric weather forecasts Sana Mahmood © Crown copyright 07/0XXX Met Office and the Met Office.
Forecast errors associated with midlatitude weather systems Heini Wernli – ETH Zurich With contributions from: Christian Grams, Hanna Joos, Erica Madonna,
PV Thinking and the Dynamic Tropopause
An Overview of the Lower and Middle Atmosphere
The “Perfect Storms” of 1991:
Pogoreltsev A., Ugrjumov A..
Static Stability in the Global UTLS Observations of Long-term Mean Structure and Variability using GPS Radio Occultation Data Kevin M. Grise David W.
Michael S. Fischer and Brian H. Tang
MID-LATITUDE WEATHER SYSTEMS: PART IV: SURFACE-UPPER AIR LINKAGE
Blocking Patterns Objectives: Types of blocking ridges
Composite patterns of DJF U200 anomalies for (a) strong EAJS, (b) weak EAJS, (c) El Niño and (d) La Niña.
The “Perfect Storms” of 1991:
Richard Moore1, Olivia Martius2, Thomas Spengler2 & Huw Davies2
Extra-tropical Flow Dynamics & THORPEX: Some Core Aspects
Tropical/extratropical forcing on wintertime variability of the extratropical temperature and circulation Bin Yu1 and Hai Lin2 1. Climate Research Division,
Extratropical stratoshere-troposphere exchange in a 20-km-mesh AGCM
Prospects for Wintertime European Seasonal Prediction
Downstream Development and Kona Low Genesis
Water Vapour Imagery and
Characteristics of 2018/2019 winter monsoon in Japan
Presentation transcript:

A Characterization of Atmospheric Blocking Huw C. Davies & Mischa Croci-Maspoli Institute for Atmospheric and Climate Science, ETH Zurich, Switzerland & MeteoSwiss, Zurich, Switzerland

OUTLINE I Spatial Structure - Basis for the characterization II Temporal Features - Credibility of the characterization III Dynamics - Utility of the characterization . via consideration of :- block origin & resilience, quasi-stationarity & formation IV Relationship with other Phenomena

Conventional Perspective Spatial Structure Conventional Perspective Notable features: . surface anticyclone, with ridge aloft & local easterly flow elevated tropopause & jet bifurcation Tropopause SLP anomaly & 500hPa pattern Latitudinal cross-section of height anomaly

An Alternative Characterization Spatial Structure An Alternative Characterization Block also evident as : . a negative PV anomaly on upper-level isentropes - anomaly located beneath an elevated tropopause PV=2 latitude [°N] - contiguous anomalies present at surface and upper-level

Essence of Characterization Spatial Structure Essence of Characterization A BLOCK constitutes . “a LENS of low PV located beneath an elevated tropopause”. Develop an "identification and tracking" tool that can catalogue every block (sic. negative PV lens) in terms of its: - amplitude, location, structure, movement and duration.

Some Salient Features II: Temporal Features A Block / PV Lens occurs in preferred geographical regions, persists for supra-synoptic time scales, and during its mature phase does NOT undergo significant : . - change of shape despite being subject to large-scale deformation (sic. a structurally resilient system) - translation despite its location within band of zonal mean westerlies (sic. a quasi-stationary system)

Credibility of Characterization II: Temporal Features Credibility of Characterization (B) Synoptic Simultaneity 1 2 3 4 5 6 7 8 9 10 Lens Climatology Comparable ! T&M P&H 13% 10% 5% 1% DJF TIME (days) 476 events -> 3.5 per month

Essence of a Block Quasi-stationarity

Questions III: Dynamics Questions prompted by “Lens” characterization of a Block: Origin of the ‘Lens’ (i.e. the negative PV anomaly) ? (B) Dynamics of system’s structural resilience ? (C) Dynamics of the system’s quasi-stationary ? Establishment of the overall PV pattern ? (- i.e. of the lens plus contiguous features)

(A) Origin of Lens III: Dynamics NOTE: Two possible sources for anomalously low PV near tropopause : - advection from low latitudes - convection (- diabatic cross-isentropic flow) from the low troposphere. ASSESS relative contribution by - examining backward trajectories from the ‘Lens’ Indication that two major sources contribute to the ‘Lens’ - tropopause-level air from far-upstream, and - low level moist air-stream ascending after passing over warm SST anomaly

(A) Origin of Lens III: Dynamics TWO INFERENCES QUERY : Is the LENS formation influenced by ascent of the coherent moist airstream ? NUMERICAL EXPERIMENT : Modify nature of airstream by changing the positive upstream anomalies in SST and land surface temperature TWO INFERENCES - Block formation sensitive to upstream surface conditions, - THE ULTIMATE TEST of a model’s cloud dynamics and microphysics is the delivery of ‘correct’ PV distribution aloft. Verifiying ECMWF Analysis Control Simulation

(B) Resilience III: Dynamics How does a “PV-Lens” retain its coherent structure ? (i) PV-lens in a horizontal uniformly sheared flow

(C) Quasi-stationarity III: Dynamics (C) Quasi-stationarity What keeps a PV Lens quasi-stationary ? (i) PV-lens in a horizontal uniformly sheared westerly flow

(C) Quasi-stationarity III: Dynamics (C) Quasi-stationarity IMPLICATION: STATIONARITY requires a richer anomalous PV pattern - isolated LENS does not suffice High PV Low PV Consider the typical instantaneous PV distribution on an isentropic surface crossing the tropopause. North High PV Low PV

Dynamics An Example of a Block with a di-polar PV configuration

(C) Quasi-stationary: Schematic of possible alternative configurations III: Dynamics High PV Low PV

(C) Alternative quasi-stationary configurations III: Dynamics An Example of a Block with a tri-polar PV configuration

(D) Establishment of overall PV-pattern III: Dynamics (D) Establishment of overall PV-pattern BREAKING WAVE(s) SCENARIOS TYPE C TYPE A High PV Low PV High PV Low PV High PV Low PV High PV Low PV High PV Low PV

(D) Establishment of overall PV-pattern III: Dynamics (D) Establishment of overall PV-pattern BREAKING WAVE(s) SCENARIOS High PV Low PV High PV Low PV

(D) Establishment of overall PV-pattern III: Dynamics (D) Establishment of overall PV-pattern EXAMPLE OF A BLOCK FORMATION Breaking wave (TYPE A) .. Secluded Lens (TYPE C) PV on 320K PVU

(D) Establishment of overall PV-pattern III: Dynamics (D) Establishment of overall PV-pattern HOVEMOELLER COMPOSITE (centred on Block) Meridional Velocity from Day-6 to DAY+6 ATLANTIC PACIFIC

(D) Establishment of overall PV-pattern III: Dynamics (D) Establishment of overall PV-pattern COMPOSITE OF BREAKING WAVES ATLANTIC PACIFIC TYPE A TYPE C

Forcing, Patterns of Climate Variability (PCV) and BLOCKS IV: Related Phenomena Forcing, Patterns of Climate Variability (PCV) and BLOCKS CONVENTIONAL CAUSAL CHAIN Forcing PCV Character of Weather Systems AN ALTERNATIVE CAUSAL CHAIN Forcing Weather Systems PCV

Troposphere - Stratosphere Linkage IV: Related Phenomena Forcing, Sudden Stratospheric Warmings and BLOCKS Troposphere - Stratosphere Linkage Baldwin and Dunkerton 2001

Sudden Stratospheric Warming & BLOCKS IV: Related Phenomena Sudden Stratospheric Warming & BLOCKS

Sudden Stratospheric Warmings & BLOCKS IV: Related Phenomena Sudden Stratospheric Warmings & BLOCKS SSW rules OK !! ? A. Scaife Blocks rule OK !! ? Evolution of mean zonal wind at 600N between 1000 and 0.1 hPa

PCV, the NAO and BLOCKS IV: Related Phenomena NAO - Normalized time-traces of the Atlantic Blocking Frequency and the NAO - index for the three winter months Blocking Frequency NAO - r = -0.65

The NAO & BLOCKS IV: Related Phenomena Evolution of NAO index during a blocking event total tracks short tracks (< 10 days) short duration (< 10 days) random random long duration (> 10 days) long tracks (> 10 days) random random

SOME POSSIBLE INFERENCES What is a BLOCK ?? Requisite for representation of BLOCKS in models