Large-scale influences during ACTIVE – Rossby waves and their effects on tropical convection Grant Allen 1 G. Vaughan 1 P. May 2 D. Brunner 3, W. Heyes.

Slides:



Advertisements
Similar presentations
Mihir Kumar Dash*, Dhrubajyoti Samanta* and P. C. Pandey** * Indian Institute of Technology, Kharagpur * Indian Institute of Technology, Bhubaneswar.
Advertisements

The Ocean perspective on frontal air-sea exchange over the wintertime Gulf Stream or…CLIMODE Redux The separated Gulf Stream (GS) is one of the ocean hot.
Weather Dynamics in Earth’s Atmosphere. An atmosphere is a blanket of a gases surrounding a planet. Earth’s atmosphere has distinct layers defined by.
REFERENCES Alexander et al (2008): Global Estimates of Gravity Wave Momentum Flux from HIRDLS Observations. JGR 113 D15S18 Ern et al (2004): Absolute Values.
Stratus. Outline  Formation –Moisture trapped under inversion –Contact layer heating of fog –Fog induced stratus –Lake effect stratus/strato cu  Dissipation.
Conceptual Models of Cold Fronts: Anacoldfront Katacoldfront.
1 This is the footer Ozone in the Tropical Tropopause Layer Geraint Vaughan What determines the ozone concentration in the tropical upper troposphere?
The DIAMET field campaign Geraint Vaughan and the DIAMET team 1 This is the footer.
Requirements for monitoring the global tropopause Bill Randel Atmospheric Chemistry Division NCAR.
Variability in Ozone Profiles at TexAQS within the Context of an US Ozone Climatology Mohammed Ayoub 1, Mike Newchurch 1 2, Brian Vasel 3 Bryan Johnson.
Weismann (1992) Weisman, M. L., 1992: The role of convectively generated rear- inflow jets in the evolution of long-lived mesoconvective systems. J. Atmos.
EASTERLY WAVE STRUCTURAL EVOLUTION OVER WEST AFRICA AND THE EAST ATLANTIC Matthew A. Janiga Department of Atmospheric and Environmental Sciences, University.
Water Vapour Imagery and
The impact of African easterly waves on the environment and characteristics of convection over West Africa Matthew A. Janiga and Chris D. Thorncroft University.
Upper-level Mesoscale Disturbances on the Periphery of Closed Anticyclones Thomas J. Galarneau, Jr. and Lance F. Bosart University at Albany, State University.
Clouds and Climate: Cloud Response to Climate Change ENVI3410 : Lecture 11 Ken Carslaw Lecture 5 of a series of 5 on clouds and climate Properties and.
INTERACTIONS OF MIDDLE LATITUDE TROUGHS AND TROPICAL DISTURBANCES ON 2-4 WEEK TIME SCALES John Molinari and David Vollaro Department of Earth and Atmospheric.
Strong Polar Anticyclone Activity over the Northern Hemisphere and an Examination of the Alaskan Anticyclone Justin E. Jones, Lance F. Bosart, and Daniel.
Quasi-geostrophic theory (Continued) John R. Gyakum.
An introduction to the Inter-tropical Convergence Zone (ITCZ) Chia-chi Wang Dept. Atmospheric Sciences Chinese Culture University Acknowledgment: Prof.
The PV-perspective Part I Based partly on: Weather analysis and forecasting: Applying Satellite Water Vapor Imagery and Potential Vorticity Analysis By.
Influence of tropopause-level disturbances on convection Geraint Vaughan.
Variability of Tropical to Extra-tropical Transport in the Lower Stratosphere Mark Olsen UMBC/GSFC Anne Douglass, Paul Newman, and Eric Nash.
Y. J. ORSOLINI Norwegian Institute for Air Research – NILU C. RANDALL LASP, University of Colorado, Boulder, USA G. MANNEY NASA Jet Propulsion.
Using GPS data to study the tropical tropopause Bill Randel National Center for Atmospheric Research Boulder, Colorado “You can observe a lot by just watching”
An investigation on a peculiar episode of stratosphere-troposphere exchange in the lee of the Alps I. Ialongo, S. Palmieri, G. R. Casale and A. M. Siani*
RGB Airmass and Dust products NASA SPoRT CIRA. RGB Air Mass RED (6.2 – 7.3) –vertical moisture distribution GREEN ( ) – tropopause height based.
Blended Course on the Principles of Satellite Meteorology 21 st April – 15 th July 2009 Classroom June 2009 Final Presentation – Convection – 09May2009.
DYNAMO Webinar Series Dynamics of the Madden-Julian Oscillation Field Campaign Climate Variability & Predictability.
Trimodal distribution of ozone and water vapor in the UT/LS during boreal summer Timothy J Dunkerton NorthWest Research Associates WARM SEASON.
Large-scale surface wind extremes in the Mediterranean Shira Raveh-Rubin and Heini Wernli Institute for Atmospheric and Climate Science (IACETH), ETH Zurich.
Fig. 1: Upper-tropospheric conditions for two major storms: 300 hPa geopotential height (red) and wind speed (shaded grey) Rainfall projections relating.
Stratosphere and Troposphere Exchange (STE) Above the Tibetan Plateau Wenshou Tian, Min Zhang, Hongying Tian Lanzhou University, Lanzhou, China Martyn.
Bauru November 2004 Modelling interpretation of in situ H2O, CH4 and CO2 measured by  SDLA balloon borne instrument (SF2 and SF4 flights). N. Huret(1),G.
Convective intensification induced by a descending dry layer: a case study of CSIP IOP 9 Andrew Russell and Geraint Vaughan Centre for Atmospheric Sciences.
Chapter 7: convective initiation
1 Longitudinally-dependent ozone recovery in the Antarctic polar vortex revealed by satellite-onboard ILAS-II observation in 2003 Kaoru Sato Department.
Characterization of the composition, structure, and seasonal variation of the mixing layer above the extratropical tropopause as revealed by MOZAIC measurements.
Nicola Patmore & Ralf Toumi (contact: Space and Atmospheric Physics Group, Imperial College London Abstract A Tropopause.
HW 3 - Q1 a. Normally P > 0 in the northern hemisphere. Instabilities result if P < 0. Discuss the two types of instability releases that may occur when.
Dynamic tropopause analysis; What is the dynamic tropopause?
Dynamical Influence on Inter-annual and Decadal Ozone Change Sandip Dhomse, Mark Weber,
UTLS Chemical Structure, ExTL Summary of the talks –Data sets –Coordinates –Thickness of the ExTL (tracers based) Outstanding questions Discussion.
Inertia-Gravity waves and their role in mixing Geraint Vaughan University of Manchester, UK.
Mesoscale processes in the polar atmosphere – the context Suzanne Gray University of Reading February 2013.
UTLS Workshop Boulder, Colorado October , 2009 UTLS Workshop Boulder, Colorado October , 2009 Characterizing the Seasonal Variation in Position.
What is the extratropical tropopause and how might it change in the future? Peter Haynes, University of Cambridge. Introduction Simple models for the extratropical.
A Subtropical Cyclonic Gyre of Midlatitude Origin John Molinari and David Vollaro.
Lecture 12 Rossby waves, propagation, breaking, climatic effects
Transport of Air from the Tropical Upper Troposphere into the Extratropical Lower Stratosphere Kenneth Bowman, Cameron Homeyer, Dalon Stone - Texas A&M.
Eastern US Transport Climatology During Average, High and Low Ozone Days Bret A. Schichtel and Rudolf B. Husar Center for Air Pollution Impact and Trend.
Chapter 7: convective initiation squall line development in Illinois a visible satellite image loop of CI in the eastern US 35°N 103°W Fig. 7.2.
Day Meridional Propagation of Global Circulation Anomalies ( A Global Convection Circulation Paradigm for the Annular Mode) Ming Cai 1 and R-C.
Atmospheric Dynamics Suzanne Gray (University of Reading) With thanks to Alan Gadian and Geraint Vaughan. Basic dynamical concepts.
Impact of the representation of the stratosphere on tropospheric weather forecasts Sana Mahmood © Crown copyright 07/0XXX Met Office and the Met Office.
Tropical Jets and Disturbances. African Easterly Waves (Figure obtained from Introduction to Tropical Meteorology, 2 nd Edition, © 2011 COMET.)
PV Thinking and the Dynamic Tropopause
An Overview of the Lower and Middle Atmosphere
PROGRAM B – Project B6.3 ELEVATED FIRE DANGER CONDITIONS ASSOCIATED WITH FOEHN-LIKE WINDS IN EASTERN VICTORIA J.J Sharples, R.O Weber School of Physical,
Tropical Convection and MJO
SO254 Extratropical cyclones
CAST – sonde activities
32nd Conference on Hurricanes and Tropical Meteorology
METO 637 Lesson 12.
Double tropopauses during idealized baroclinic life cycles
Water vapour as an indicator of dynamical processes in the extratropical UTLS inferred from balloon observations Sergey Khaykin (1), A. Lukyanov(1), V.Yushkov.
ATMS 790 Graduate Seminar Presenter: Saroj Dhital Date: March-12, 2018
ExUTLS dynamics and global observations
Water Vapour Imagery and
MPEF DIVergence product Interpretation scheme
Presentation transcript:

Large-scale influences during ACTIVE – Rossby waves and their effects on tropical convection Grant Allen 1 G. Vaughan 1 P. May 2 D. Brunner 3, W. Heyes 1, P. Minnis 4 1 Centre for Atmospheric Science, University of Manchester 2 Bureau of Meteorology, Melbourne, Australia 3 EMPA, Switzerland 4 LARC, NASA Final ACTIVE meeting – Manchester, 21 st May 2009

Scope What are tropical tropopause folds? Why are they important? A case study of a series of folds during the ACTIVE campaign Implications for tropical convection

Isentropic descent – Tropopause folds Plot taken from Holton, 1995 Isentropes =solid lines Isotherms = dashed lines Shaded area = lowermost stratosphere The thermodynamic structure of the tropical troposphere links the sub-tropical lower stratosphere with the tropical troposphere – no barrier to transport (isentropic) One mechanism of such transport is due to breaking Rossby waves and consequent tropopause folding along the STJ

A Region of Interest (ROI) Left: MTSAT WV image – dark areas are dry, blue represent tall/high clouds) NW Australia Domain defined for analysis: Lat: 20  12 O S Lon: O E Region of interest (cross-hatch area above) defined here for further analysis Region defined by the prevalence of an eastward-advancing dry slot (dark area in MTSAT WV image above)

Convective (and other) properties of the ROI Two “tropical drought” periods are defined by grey shaded time periods. Time-series of cloud fraction shows anti-correlation with PV during periods of large-scale descent (ω) Rainfall and mid-level RH are also correlated during the dry periods Together, these trends show that rainfall and cloudiness were much reduced during the passage of a series of tropopause folds (evident as periods of high PV) Concentrate here on the second drought period as a case study

Cloud Cover and Height Derived from MTSAT-1R brightness temperatures using a split-window technique of Minnis et al., 1995 During the drought period, convection is shallow and limited to the coast (where forcing is likely to be strongest)

Rossby waves Arrows= wind direction scaled to speed Colours= Potential vorticity Selected images of ECMWF PV (at 325 K) and wind data show the passage of a series of breaking Rossby waves (red protrusions) over northern Australia during the dry period The double breaking event on 22 Nov (panel b) facilitated the northward propagation of the wave by 23 Nov (panel c). By 27 Nov, a quiescent jet was re-established to the south

Tropopause folds A finger of high PV defines the fold, which enters the ROI on 22 Nov carrying very dry air from the tropopause The PV signature associated with the fold persists until ~ 25 Nov The dry air advected by the fold persists in the ROI even after the PV signature is lost on 27 Nov Colours = PV Black contours = RH % Dashed lines = Equivalent potential temperature Vertical dashed lines define the latitude limits of the ROI

Ozone and humidity profiles Deep dry, ozone-rich layers present between 22 nd – 27 th Nov 13 th and 30 th Nov are typical pre- monsoon examples Spot the odd one out – transition between the influence of the two separate folds

Back trajectories 4-day cluster back trajectories from the enhanced ozone layers observed at Darwin show they originated in or near to the breaking Rossby waves By 30 Nov (panel e), after the drought period, trajectories return to a more climatological tropospheric origin.

Promotion of a large tropical cloud band

Left: Plots of CAPE and CIN diagnosed from ECMWF profiles at 0930 local time on 20 Nov 2005 over N Australia The tropical cloud band developed in a region of high CAPE (> 2000 J/kg), but low CIN (< 100 J/kg) The region of low CAPE and high CIN to the SW of the line indicates the position of the advancing dry slot seen in the satellite images

Dynamics at the point of convective initiation A cross-section of wet-bulb potential temperature (Theta-W above) through the plume shows a region of reduced theta-W above the boundary layer at 14 O S (where convection originated) This reduction of theta-w with height over a moist boundary layer represents a region of high potential instability

Conclusions A series of breaking Rossby waves over northern Australia during November 2005 led to strong modulation of convection over a wide area of the tropics Dry air which descended due to tropopause folding led to a marked reduction in cloud-cover and rainfall for a period of 6 days in total At the edge of one such advancing dry layer, generation of potential instability led to an eruption of a synoptic scale cloud system. Further evidence that mid-latitude tropopause level processes can influence tropical convection and rainfall.