Nicola Patmore & Ralf Toumi (contact: Space and Atmospheric Physics Group, Imperial College London Abstract A Tropopause.

Slides:



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

Analysis of Eastern Indian Ocean Cold and Warm Events: The air-sea interaction under the Indian monsoon background Qin Zhang RSIS, Climate Prediction Center,
Chap. 5 Conceptual models of synoptic Tropical disturbances in summer Definition of tropical disturbances : A discrete tropical weather system of apparently.
Precipitation Over Continental Africa and the East Atlantic: Connections with Synoptic Disturbances Matthew A. Janiga November 8, 2011.
EASTERLY WAVE STRUCTURAL EVOLUTION OVER WEST AFRICA AND THE EAST ATLANTIC Matthew A. Janiga Department of Atmospheric and Environmental Sciences, University.
Chapter 9 Vertical Motion. (1) Divergence in two and three dimensions. The del “or gradient” operator is a mathematical operation performed on something.
Response of the Atmosphere to Climate Variability in the Tropical Atlantic By Alfredo Ruiz–Barradas 1, James A. Carton, and Sumant Nigam University of.
General circulation in the tropics
Upper-level Mesoscale Disturbances on the Periphery of Closed Anticyclones Thomas J. Galarneau, Jr. and Lance F. Bosart University at Albany, State University.
Strong Polar Anticyclone Activity over the Northern Hemisphere and an Examination of the Alaskan Anticyclone Justin E. Jones, Lance F. Bosart, and Daniel.
USE OF HS3 DATA TO UNDERSTAND THE TROPICAL CYCLONE OUTFLOW LAYER John Molinari, Kristen Corbosiero, Stephanie Stevenson, and Patrick Duran University at.
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.
Influence of tropopause-level disturbances on convection Geraint Vaughan.
Jet Streams Lessons 25/26 Jet Streams Defined as a narrow ribbon of fast moving air : –1000’s of miles in length, –up to 200 miles wide, –approx.. 2.
II. Synoptic Atmospheric Destabilization Processes Elevated Mixed Layer (EML) Synoptic Lifting Dynamic Destabilization Differential Advection.
Long lived Thundersnow March 23, 1966 By Kathy Lovett and Leah Smeltzer Authors: Patrick S. Market, Rebecca L. Ebert-Cripe Michael Bodner.
Multiscale Analyses of Tropical Cyclone-Midlatitude Jet Interactions: Camille (1969) and Danny (1997) Matthew S. Potter, Lance F. Bosart, and Daniel Keyser.
Cargese International School, COST ACTION 723, UTLS, 3-15 Oct., 2005 Water Vapour Variation in the Upper Troposphere and Lower Stratosphere over the Asian.
Modulation of eastern North Pacific hurricanes by the Madden-Julian oscillation. (Maloney, E. D., and D. L. Hartmann, 2000: J. Climate, 13, )
ENSO impact to atmospheric circulation system for summer Motoaki Takekawa Tokyo Climate Center, Japan Meteorological Agency (JMA) 1.
The Influence of Solar Forcing on Tropical Circulation JAE N. LEE DREW T. SHINDELL SULTAN HAMEED.
Isentropic Analysis Techniques: Basic Concepts March 5, 2004 Adapted from Professor Jim Moore of St. Louis University.
The troposphere, except in shallow, narrow, rare locations, is stable to dry processes. For the purpose of synoptic analysis, these areas can be ignored.
Trimodal distribution of ozone and water vapor in the UT/LS during boreal summer Timothy J Dunkerton NorthWest Research Associates WARM SEASON.
Formation processes of tripolar climate anomaly over East Asia in summer Nagio Hirota and Masaaki Takahashi CCSR, University of Tokyo 2008/6/23.
Where PV2 >> PV1 (so PV1 / PV2 is nearly zero) Low-to-mid tropospheric PV generated by diabatic heating is dominant over PV generated due to near surface.
1 IPV and the Dynamic Tropopause John W. Nielsen-Gammon Texas A&M University
The Indian Monsoon A monsoon seasonal change is characterized by a variety of physical mechanisms which produce strong seasonal winds, a wet summer.
The Linear and Non-linear Evolution Mechanism of Mesoscale Vortex Disturbances in Winter Over Western Japan Sea Yasumitsu MAEJIMA and Keita IGA (Ocean.
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.
The quasi-geostrophic omega equation (see Bluestein, Volume I; eq (  2 + (f 0 2 /  )  2 /∂p 2 )  = (-f 0 /  )  /  p{-v g  p (  g + f)}
ATS/ESS 452: Synoptic Meteorology
Key Terms and Concepts ELR--Environmental Lapse Rate 5°C-6.5°C/1000 m – temperature of the STILL air as you ascend through the troposphere. ALR--Adiabatic.
NSF Proposal Impacts of Rossby Wave Breaking and Potential Vorticity Streamer Formation on the Environment of the Tropical and Subtropical North Atlantic.
1 Longitudinally-dependent ozone recovery in the Antarctic polar vortex revealed by satellite-onboard ILAS-II observation in 2003 Kaoru Sato Department.
Applications of ‘IPV’ thinking for time-dependent dynamical processes (p. 202, Bluestein, 1993) The purpose of this discussion is to utilize ‘IPV’ thinking.
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?
Results Time mean SSTs display regions of large fronts but also thermostats associated with mode waters (Fig. 2, upper panel). Large fronts are typically.
On the mechanism of eastward-propagation of super cloud clusters (SCCs) over the equator – Impact of precipitation activities on climate of East Asia –
Inertia-Gravity waves and their role in mixing Geraint Vaughan University of Manchester, UK.
Adiabatic Westward Drift in Monsoon Depressions Introduction and Methods Boos et al
Contrasting potential vorticity structures in two summer extratropical cyclones Oscar Martínez-Alvarado NCAS-Atmospheric Physics Sue Gray John Methven.
UTLS Workshop Boulder, Colorado October , 2009 UTLS Workshop Boulder, Colorado October , 2009 Characterizing the Seasonal Variation in Position.
A Subtropical Cyclonic Gyre of Midlatitude Origin John Molinari and David Vollaro.
An Investigation of Model-Simulated Band Placement and Evolution in the 25 December 2002 Northeast U.S. Banded Snowstorm David Novak NOAA/ NWS Eastern.
10/25/ th Cyclone Workshop1 Analysis of the potential vorticity budget of a tropopause polar cyclone Steven M. Cavallo and Gregory J. Hakim University.
African easterly wave dynamics in a full-physics numerical model. Gareth Berry and Chris Thorncroft. University at Albany/SUNY, Albany, NY,USA.
Analysis of Typhoon Tropical Cyclogenesis in an Atmospheric General Circulation Model Suzana J. Camargo and Adam H. Sobel.
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.
Forces and accelerations in a fluid: (a) acceleration, (b) advection, (c) pressure gradient force, (d) gravity, and (e) acceleration associated with viscosity.
Day Meridional Propagation of Global Circulation Anomalies ( A Global Convection Circulation Paradigm for the Annular Mode) Ming Cai 1 and R-C.
Juliane Schwendike and Sarah Jones The Interaction between Convection and African Easterly Waves:
PV Thinking and the Dynamic Tropopause
The Active 2008 Atlantic Hurricane Season Links to Known Climate Factors Gerry Bell NOAA Lead Seasonal Hurricane Forecaster Climate Prediction Center.
Makoto INOUE and Masaaki TAKAHASHI (CCSR, Univ. of Tokyo)
32nd Conference on Hurricanes and Tropical Meteorology
Michael S. Fischer and Brian H. Tang
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
The Genesis of Hurricane Guillermo: TEXMEX Analyses and a Modeling Study BISTER AND EMANUEL.
Constant Pressure Maps
Interannual variability of transport via the Asian Summer Monsoon
Impact of the vertical resolution on Climate Simulation using CESM
Double tropopauses during idealized baroclinic life cycles
(Geopotential height, and wind > 50 kt)
Daniel M. Alrick 14th Cyclone Workshop Monday, September 22, 2008
Richard B. Rood (Room 2525, SRB)
Water Vapour Imagery and
Simulations of the transport of idealized short-lived tracers
Department of Physics and Astronomy, University of Louisville, KY, USA
Presentation transcript:

Nicola Patmore & Ralf Toumi (contact: Space and Atmospheric Physics Group, Imperial College London Abstract A Tropopause Moist Pool over Arid Asia Minor Introduction HALOE Results ERA-40 Results  -PV Analysis using ERA-40  Various authors have shown the importance of the northern hemisphere monsoon systems in the hydration of the upper troposphere. However, the mechanisms through which the monsoons moisten the tropopause layer have remained unconfirmed.  This study uses data from the ECMWF ERA-40 reanalysis model and observational data from the HALOE instrument onboard UARS, to study water vapour distributions over the strongest monsoon system: the Asian Summer Monsoon (ASM). 126mb Diabatic Heating and PV Generation Source of Diabatic Heating Conclusions and Future Work Acknowledgements 150mb 100mb70mb Figure 3: ERA-40 JJA Vertical Wind Velocity (Shaded: red=ascending, blue=descending) and Horizontal Wind Velocity (Vectors). [ Contours: 150mb (2Pas -1 ), 100mb & 70mb (1Pas -1 )] Figure 2: ERA-40 JJA Water Vapour(ppmv). 150mb 100mb70mb Figure 1: HALOE Water Vapour (ppmv) JJA ( )  ERA-40 shows a similar moist pool to HALOE, but suggests a continuous westward motion with height.  At 150mb, the water vapour distribution reflects the strong convection of the monsoon over India (Fig. 3).  Above 150mb, moisture forms a pool to the south of the anticyclone core, overlying Asia Minor.  The moist pools at 100mb and 70mb appear to overlie a region of descent.  Figure 4 shows the variability of water vapour on an isentropic level. The pool moves longitudinally with time and appears to form through a series of discreet cross-isentropic pulses. 395K Potential Vorticity (PVU) Longitude Figure 5: Left: ERA-40 JJA Averaged N at 395K. Above: Expansion of Potential Vorticity at 395K, day 43, 12/07/94  Figures 4 and 5 show that the moist pool is trapped within the region of low potential vorticity at the anticyclone core.  Figure 6 shows a band of diabatic heating at ~40N. Periodic intensifications of this heating could incite the localised negative PV tendencies and water vapour pulses shown in figures 4 and 5.  Water vapour ascending within these localised regions would be immediately trapped within the PV anomaly.  No similar PV anomalies form over India or Myanmar.  How could a source of water vapour at ~40N, create the Asia Minor moist pool?  PV tendencies at ~40N are quickly removed by isentropic advection (Fig 7a). The newly formed PV and water vapour anomalies are advected around the anticyclone.  The region over Asia Minor experiences a continuous negative PV tendency (Fig 7). Water vapour is trapped in this region and gradually builds over the summer. Figure 6: 395K ERA-40 July (Interval: 0.5Kday -1 red(+), blue (-))  Diabatic heating at ~40N can not be explained by latent heating, as relative humidities do not exceed 30%  We propose that heating may result from the vertical turbulent mixing of heat, within the westerly jet.  The Richardson Number is naturally low at ~40N, due to the strong vertical wind shear (Fig 8).  We suggest that synoptic disturbances may result in a strengthening of the jet or weakening of the local buoyancy stability. Small perturbations to this sensitive region have the potential to cause temporary dynamic instabilities, leading to vertical mixing and heat transfer. Diabatic Heating (Q/cp) (b) Diabatic Advection PV (c) Diabatic Creation PV Figure 7: Three dominant components of PV tendency at 395k. Calculated using ERA-40, averaged July (Interval: 0.2PVUday -1, red (+), blue(-)) Green indicates zero PV tendency Figure 8: ERA-40 Richardson Number, July  At 126mb, HALOE shows two moist pools. The pool over the Bay of Bengal results from the strong convection of the monsoon beneath. The pool over Asia Minor is unexpected, as it overlies an arid region.  By 100mb, only the Asia Minor moist pool remains. This pool is still present at 86mb, but fades by 70mb. 100mb Time  A tropopause moist pool forms over Asia Minor, overlying a region of mean descent.  The pool is trapped within the low PV anomaly of the monsoon anticyclone.  The pool forms through trapping of water vapour that ascends in discreet pulses from below. These pulses appear to be linked to local increases in diabatic heating and intense low PV generation.  The source of the diabatic heating is work in progress. We suggest that the source is vertical diffusion of heat resulting from temporary dynamic instabilities. We are currently investigating the potential of transient perturbations in horizontal advection heating to incite these instabilities. Satellite and reanalysis data show the presence of a summertime “moist pool”, extending from ~150mb to 70mb, over the arid Asia Minor region (Iraq to Pakistan). The pool appears to form through the trapping of water vapour, which ascends in discreet pulses. The localised ascending regions are associated with intense low PV formations at ~40N. Diabatic heating along the westerly jet appears to be linked to the negative PV tendencies, however the source of the diabatic heating is unconfirmed. We suggest that perturbations to the jet may cause temporary dynamic instabilities, which could result in mixing and vertical diffusion of heat into the tropopause layer. 86mb Figure 4: ERA-40 JJA Averaged 25-45N at 395K. 395K Water Vapour (ppmv)  Periodically, regions of intense low PV form on the northern side of the anticyclone, at ~40N. After formation, these anomalies are advected southwards and around the anticyclone core. The formation of low PV anomalies is associated with the pulses of water vapour seen in figure 4. (a) Isentropic Advection PV We would like to thank the UK Natural Environmental Research Council (NERC) for funding this work. ERA-40 data was obtained from the British Antarctic Data Centre (BADC), courtesy of ECMWF. HALOE data was obtained from the HALOE homepage at the NASA Langley Research Centre website.