An alternative mechanistic model of the Antartic polar vortex Walter Legnani 1, Rolando Garcia 2, Pablo Jacovkis 3, Murry Salby 4, and Pablo Canziani 5,6.

Slides:



Advertisements
Similar presentations
Parameterization of orographic related momentum
Advertisements

A Characterization of Atmospheric Blocking Huw C. Davies
Ocean’s Role in the Stratosphere-Troposphere Interaction Yulia A. Zyulyaeva Moscow State University P.P.Shirshov Institute of Oceanology, RAS, Moscow 1/17.
Section 5: Kelvin waves 1.Introduction 2.Shallow water theory 3.Observation 4.Representation in GCM 5.Summary.
Cumulus Forced; pushed upward by external forces, i.e. lifting by surface convergence, topography etc. Active; growing upward from self-forcing, i.e. buoyancy,
Lecture IV of VI (Claudio Piani) 3D N-S equations: stratification and compressibility, Boussinesq approximation, geostrophic balance, thermal wind.
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.
Tropical Convection: A Product of Convergence. But What Drives Convergence?  ONE THEORY: CISK  Conditional Instability of the Second Kind  A Positive.
The ENSO : El Niño and the Southern Oscillation J.P. Céron (Météo-France) and R. Washington (Oxford University)
Shear Instability Viewed as Interaction between Counter-propagating Waves John Methven, University of Reading Eyal Heifetz, Tel Aviv University Brian Hoskins,
Mountain Waves entering the Stratosphere. Mountain Waves entering the Stratosphere: New aircraft data analysis techniques from T-Rex Ronald B. Smith,
Baroclinic Instability in the Denmark Strait Overflow and how it applies the material learned in this GFD course Emily Harrison James Mueller December.
EQUATORIAL WAVES part 2: Vertical Propagation & the QBO.
Lessons 22,23,24 Upper Level Winds
Triggering of the Madden-Julian Oscillation by equatorial ocean dynamics. Benjamin G. M. Webber IAPSO-IAMAS JM10: Monsoons, Tropical Cyclones and Tropical.
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”
The simplest theoretical basis for understanding the location of significant vertical motions in an Eulerian framework is QUASI-GEOSTROPHIC THEORY QG Theory:
1.Introduction 2.Description of model 3.Experimental design 4.Ocean ciruculation on an aquaplanet represented in the model depth latitude depth latitude.
Operation of Backscatter Lidar at Buenos Aires (34.6 S / 58.5 W) for the Retrieval and Analysis the Atmospheric Parameters in Cirrus Clouds, Tropopause.
Structure and dynamical characteristics of mid-latitude fronts.
Flash Flood event over central Argentina: a case study Paola Salio (1), Yanina Garcia Skabar (2) and Matilde Nicolini (1) (1) Departamento de Ciencias.
ADVENTURE IN SYNOPTIC DYNAMICS HISTORY
Physics of the Atmosphere II
Jeff Forbes (CU), Xiaoli Zhang (CU), Sean Bruinsma (CNES), Jens Oberheide (Clemson U), Jason Leonard (CU) 1 Coupling to the Lower Atmosphere, an Observation-Based.
Lecture 19-20: Natural convection in a plane layer. Principles of linear theory of hydrodynamic stability 1 z x Governing equations: T=0T=0 T=AT=A h =1.
A Statistical Analysis on the Stratosphere-Troposphere Coupled Variability by Using Large Samples obtained from a Mechanistic Circulation Model Yoko NAITO.
Application of the two-step method for the solution of the inverse gravity problem for the Kolárovo anomaly.
The use of an Adaptive Mesh Refinement Transport Code to study the 2002 Antarctic polar vortex evolution Walter E. Legnani 1, Pablo O. Canziani 2,3, Alan.
THE INTERANNUAL SPATIAL VARIABILITY OF THE SOUTHERN HEMISPHERE TOTAL OZONE COLUMN MIDLATITUDE MAXIMUM: AN INDICATOR OF TROPOSPHERIC- STRATOSPHERIC COUPLED.
Overview of Tropical Cyclones AOS 453 April 2004 J. P. Kossin CIMSS/UW-Madison.
AOS 100: Weather and Climate Instructor: Nick Bassill Class TA: Courtney Obergfell.
EVAT 554 OCEAN-ATMOSPHERE DYNAMICS TIME-DEPENDENT DYNAMICS; WAVE DISTURBANCES LECTURE 21.
Model evolution of a START08 observed tropospheric intrusion Dalon Stone, Kenneth Bowman, Cameron Homeyer - Texas A&M Laura Pan, Simone Tilmes, Doug Kinnison.
Chapter 5 - PBL MT 454 Material Based on Chapter 5 The Planetary Boundary Layer.
The simplifed momentum equations Height coordinatesPressure coordinates.
Lecture 11 Picking up pieces from previous lectures + – result of surface force balance – scales of motion – mesoscale systems: sea breeze, land breeze.
HOW DOES THIS ENERGY MOVE? Vertical and Horizontal Movements Within the Troposphere and Global Pressure Belts. This is when we start putting the pieces.
A signal in the energy due to planetary wave reflection in the upper stratosphere J. M. Castanheira(1), M. Liberato(2), C. DaCamara(3) and J. M. P. Silvestre(1)
AOSS 401, Fall 2006 Lecture 18 October 24, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Contrasting potential vorticity structures in two summer extratropical cyclones Oscar Martínez-Alvarado NCAS-Atmospheric Physics Sue Gray John Methven.
Governing Equations II
Atmosphere. What makes up our atmosphere?  Nitrogen  Oxygen  Argon.
The ENSO Signal in Stratospheric Temperatures from Radiosonde Observations Melissa Free NOAA Air Resources Lab Silver Spring 1.
The impact of solar variability and Quasibiennial Oscillation on climate simulations Fabrizio Sassi (ESSL/CGD) with: Dan Marsh and Rolando Garcia (ESSL/ACD),
ATMOSPHERE OBJECTIVE 1 1.What are the structural components of the
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.
Matthew J. Hoffman CEAFM/Burgers Symposium May 8, 2009 Johns Hopkins University Courtesy NOAA/AVHRR Courtesy NASA Earth Observatory.
Model calculationsMeasurements An extreme precipitation event during STOPEX I J.Reuder and I. Barstad Geophysical Institute, University of Bergen, Norway.
AOSS 401, Fall 2006 Lecture 7 September 21, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
An Overview of the Lower and Middle Atmosphere
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.
Vorticity Vertical component of vorticity: i.e., the rotation about the local vertical There are three types of vorticity used in geophysical fluid dynamics.
EVAT 554 OCEAN-ATMOSPHERE DYNAMICS
  Robert Gibson1, Douglas Drob2 and David Norris1 1BBN Technologies
ATOC 4720 class31 1. Coordinate systems 2. Forces.
Double tropopauses during idealized baroclinic life cycles
National Center for Atmospheric Research
The Atmosphere of Earth
Changes in the Free Atmosphere
ATMOSPHERE OBJECTIVE 1 1.What are the structural components of the
ATOC 4720: class 6: Winds and precipitation
Lower Tropospheric Frontogenesis
Structure of the Atmosphere
Conformational Isomers Configurational Isomers cis-trans isomers isomers that contain chirality centers.
A Multiscale Numerical Study of Hurricane Andrew (1992)
Department of Physics and Astronomy, University of Louisville, KY, USA
Layers of the Atmosphere
Aim: What are global winds and ocean currents?
Presentation transcript:

An alternative mechanistic model of the Antartic polar vortex Walter Legnani 1, Rolando Garcia 2, Pablo Jacovkis 3, Murry Salby 4, and Pablo Canziani 5,6 1 Instituto de Cálculo, Universidad de Buenos Aires - Argentina 2 National Center for Atmospheric Research - U.S.A. 3 Instituto de cálculo/Departamento de Computacion, Universidad de Buenos Aires - Argentina 4 UCenter for Atmospheric Theory and Analysis University of Colorado - U.S.A. 5 Programa de Estudios de Procesos Atmosféricos en el Cambio Global –Pontificia Universidad Católica Argentina/CONICET – Argentina 6 Departamento de Ciencias de la Atmosfera y los Océanos, Universidad de Buenos Aires/CONICET - Argentina A quasi-3D global atmospheric model was developed to study the dynamics of the Antartic polar vortex. The atmospheric system is represented by shallow water equations system together with thermodynamics, from a classical point of view. The integration of the equations on the horizontal plane was made using a Hough harmonic base. These conform an orthonormal system which is the eingensystem of the shallow water operator of the linearised system of equations. The non-linearities were retained in the forcing terms of the equations. Thus the model uses the non linear shallow water systems of equations. In the vertical, the model was adjusted at each time step using a spline base to fit the solution between two consecutive model layers, on isentropic surfaces. This mechanistic model is forced from below at the lower boundary (near the tropopause) with the temperature from NCEP reanalysis, while the upper boundary is free. The model was developed to study the dynamical behaviour of the Antartic polar vortex, in particular the interaction with synoptic scale disturbances of tropospheric origin. The model was able to reproduce observations that show that synoptic scale perturbations of tropospheric origin can penetrate sufficiently into the lower stratosphere and can thus significantly contribute to the deformation of the polar vortex. The models equations Model Results Model Validation Model’s Output for event type II (from 14 to 21km) Results with all wave Results with wave components components in the forcing up to wave number 4 Model’s Output for event type I (from 14 to 21km) Results with all wave Results with wave components components in the forcing up to wave number 4 Summing up The model uses a month warm up period (September) to reproduce the dyamical and thermodynamical conditions of the atmosphere. The validation with datasets was completely successfully. The outputs shown on the left, show that the presence of the synoptic scale waves, with zonal wave numbers greater than 4 have an important contribution in the shape of the polar vortex for certain conditions, dependent on the mean flow and longer planetary wave structure. The model presented here is a mechanistic one, because it uses an input as temperature of tropopause to integrate the isentropic shallow water equations with to purpose of reproduce a certain picture of the atmosphere. For an event type II the presence of synoptic scale waves is important to conform the real structure of the vortex, in the cases studied. For events type I, the activity of synoptic scale waves do not contribute on the conformation of the main structure of the polar vortex. Shallow water equations in isentropic coordinates The coordiante system Spectral solution (using Hough harmonics) of the system in the horizontal direction and interpolation beta spline scheme in the vertical direction NCAR University of Colorado Boulder