Figure (a-c). Latitude-height distribution of monthly mean ozone flux for the months of (a) January, (b) April and (c) July averaged over years 2000 to.

Slides:



Advertisements
Similar presentations
Norwegian Institute for Air Research The Tropopause at High Northern Latitudes: Trends and Influence of Atmospheric Dynamics Georg Hansen and.
Advertisements

REFERENCES Alexander et al (2008): Global Estimates of Gravity Wave Momentum Flux from HIRDLS Observations. JGR 113 D15S18 Ern et al (2004): Absolute Values.
Requirements for monitoring the global tropopause Bill Randel Atmospheric Chemistry Division NCAR.
ACCMIP simulations of Climate Change impacts on CO-tracer transport Ruth Doherty, Ian Mackenzie U. Edinburgh Paul Young, Oliver Wild U. Lancaster Mieyun.
Another hint for a changing stratospheric circulation after 2001 Harald Bönisch (1), Andreas Engel (1), Thomas Birner (2), Peter Hoor (3) (1)Institute.
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.
Assimilation of TES O 3 data in GEOS-Chem Mark Parrington, Dylan Jones, Dave MacKenzie University of Toronto Kevin Bowman Jet Propulsion Laboratory California.
CO 2 in the middle troposphere Chang-Yu Ting 1, Mao-Chang Liang 1, Xun Jiang 2, and Yuk L. Yung 3 ¤ Abstract Measurements of CO 2 in the middle troposphere.
ECMWF CO 2 Data Assimilation at ECMWF Richard Engelen European Centre for Medium-Range Weather Forecasts Reading, United Kingdom Many thanks to Phil Watts,
Using beryllium-7 to assess stratosphere-to- troposphere transport in global models 4 th GEOS-Chem Users’ Meeting Harvard University, April 7-10, 2009.
Seasonal Variations in the Mixing Layer in the UTLS Dave MacKenzie University of Toronto GEOS-Chem Meeting April 2009.
Impact of Seasonal Variation of Long-Range Transport on the Middle Eastern O 3 Maximum Jane Liu, Dylan B. Jones, Mark Parrington, Jay Kar University of.
Introduction. A major focus of SCOUT-O3 is the tropics and a key issue here is testing how well existing global 3D models perform in this region. This.
Lessons 22,23,24 Upper Level Winds
Influence of the Brewer-Dobson Circulation on the Middle/Upper Tropospheric O 3 Abstract Lower Stratosphere Observations Models
(a)(b)(c) Simulation of upper troposphere CO 2 from two-dimensional and three-dimensional models Xun Jiang 1, Runlie Shia 2, Qinbin Li 1, Moustafa T Chahine.
Variability of Tropical to Extra-tropical Transport in the Lower Stratosphere Mark Olsen UMBC/GSFC Anne Douglass, Paul Newman, and Eric Nash.
Influence of the sun variability and other natural and anthropogenic forcings on the climate with a global climate chemistry model Martin Schraner Polyproject.
Dynamical control of ozone transport and chemistry from satellite observations and CCMs Mark Weber 1, Ingo Wohltmann 2, Veronika Eyring 3, Markus Rex 2,
SHNHCEF EI ind c-5.3±0.24.5±0.1−0.8±0.1 EI dir c-5.4±0.24.8± ±0.2 E40 ind c−5.7±0.34.9±0.3−0.9±0.2 E40 dir c-4.9±0.64.7± ±0.2 FT08−4.9±0.25.1±0.5-
The speaker took this picture on 11 December, 2012 over the ocean near Japan. 2014/07/29 AOGS 11th Annual Meeting in Sapporo.
© Crown copyright Met Office The Brewer-Dobson circulation in the CMIP5 simulations Steven Hardiman and Neal Butchart (Met Office Hadley Centre) Natalia.
Radiative-dynamical processes modulating the vertical structure of the stratospheric polar vortex José M. P. Silvestre, José M. Castanheira, and Juan Ferreira.
MIR OZONE ISSUES Horizontal (STE) and vertical transport (long life time in UTLS) Photochemical production by precursors (biomass burning, lightning,..)
Transport analysis and source attribution of the tropical CO seasonal and interannual variability in the UT/LS Junhua Liu and Jennifer Logan School of.
Seasonal variability of UTLS hydrocarbons observed from ACE and comparisons with WACCM Mijeong Park, William J. Randel, Louisa K. Emmons, and Douglas E.
Sensitivity of Antarctic climate to the distribution of ozone depletion Nathan Gillett, University of East Anglia Sarah Keeley, University of East Anglia.
Human fingerprints on our changing climate Neil Leary Changing Planet Study Group June 28 – July 1, 2011 Cooling the Liberal Arts Curriculum A NASA-GCCE.
The effect of pyro-convective fires on the global troposphere: comparison of TOMCAT modelled fields with observations from ICARTT Sarah Monks Outline:
Stratosphere and Troposphere Exchange (STE) Above the Tibetan Plateau Wenshou Tian, Min Zhang, Hongying Tian Lanzhou University, Lanzhou, China Martyn.
COST 723 WORKSHOP – SOFIA, BULGARIA MAY 2006 USE OF RADIOSONDE DATA FOR VALIDATION OF REGIONAL CLIMATE MODELLING SIMULATIONS OVER CYPRUS Panos Hadjinicolaou.
NASA/GSFC Tropospheric Ozone Residual M. Schoeberl NASA/GSFC M. Schoeberl NASA/GSFC.
 We also investigated the vertical cross section of the vertical pressure velocity (dP/dt) across 70°W to 10°E averaged over 20°S-5°S from December to.
Modeling and Analysis of the Earth’s Hydrologic Cycle Donald R. Johnson Tom H. Zapotocny Todd K. Schaack Allen J. Lenzen Space Science and Engineering.
A modelling study on trends and variability of the tropospheric chemical composition over the last 40 years S.Rast(1), M.G.Schultz(2) (1) Max Planck Institute.
Dynamical balances and tropical stratospheric upwelling Bill Randel and Rolando Garcia NCAR Thanks to: Qiang Fu, Andrew Gettelman, Rei Ueyama, Mike Wallace,
Dynamical Influence on Inter-annual and Decadal Ozone Change Sandip Dhomse, Mark Weber,
Improved understanding of global tropospheric ozone integrating recent model developments Lu Hu With Daniel Jacob, Xiong Liu, Patrick.
Dynamical Impacts of Antarctic Stratospheric Ozone Depletion on the Extratropical Circulation of the Southern Hemisphere Kevin M. Grise David W.J. Thompson.
UTLS Chemical Structure, ExTL Summary of the talks –Data sets –Coordinates –Thickness of the ExTL (tracers based) Outstanding questions Discussion.
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)
Using CO observations from space to track long-range transport of pollution Daniel J. Jacob with Patrick Kim, Peter Zoogman, Helen Wang and funding from.
UTLS Workshop Boulder, Colorado October , 2009 UTLS Workshop Boulder, Colorado October , 2009 Characterizing the Seasonal Variation in Position.
David Stevenson 1, Colin Johnson 2, Ellie Highwood 3, Bill Collins 2, & Dick Derwent 2 1 School of GeoSciences, University of Edinburgh 2 The Met Office.
A SEARCH FOR FREE ROSSBY WAVES AND FOR VAN LOON’S TEMPERATURE VARIATIONS IN THE SOUTHERN HEMISPHERE STRATOSPHERE Roland Madden, NCAR, USA.
(a)(b)(c) Simulation of upper troposphere CO 2 from two-dimensional and three-dimensional models Xun Jiang 1, Runlie Shia 2, Qinbin Li 1, Moustafa T Chahine.
Variability of CO 2 From Satellite Retrievals and Model Simulations Xun Jiang 1, David Crisp 2, Edward T. Olsen 2, Susan S. Kulawik 2, Charles E. Miller.
Dynamical control of ozone transport and chemistry from satellite observations and coupled chemistry climate models Mark Weber 1, Sandip Dhomse 1, Ingo.
Chapter 6: Present day ozone distribution and trends relevant to climate change A. Gaudel, O. R. Cooper, G. Ancellet, J. Cuesta, G. Dufour, F. Ebojie,
Francois Engelbrecht, Thando Ndarana, Yushi Morioka, Swadhin Behera, Marcus Thatcher, John McGregor, Mary-Jane Bopape, Johan Malherbe Simulating the radiative.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Spectral response functions (SRF) for the ABI IR bands (blue curves with band numbers.
Observational Error Estimation of FORMOSAT-3/COSMIC GPS Radio Occultation Data SHU-YA CHEN AND CHING-YUANG HUANG Department of Atmospheric Sciences, National.
SCSL SWAP/LYRA workshop
Daily Tropospheric Ozone Residual from OMI-MLS
GMI Capabilities Sarah Strode, Jose Rodriguez, Steve Steenrod, Junhua Liu, Susan Strahan, Eric Nielsen.
CCSM Working Group Meeting, February 2008
METO 637 Lesson 12.
Towards IPCC AR6: Open questions in chemistry-climate coupling
A New Tropopause Definition for Use in Chemistry-Transport Models
Atmospheric modelling of the Laki eruption
Variability of CO2 From Satellite Retrievals and Model Simulations
Variability of CO2 From Satellite Retrievals and Model Simulations
Extratropical stratoshere-troposphere exchange in a 20-km-mesh AGCM
Nonlinear modulation of O3 and CO induced by mountain waves in the UTLS region during TREX Mohamed Moustaoui(1), Alex Mahalov(1), Hector Teitelbaum(2)
Shiliang Wu1 Loretta J. Mickley1, Daniel J
NRT Tropospheric and UTLS Ozone From OMI/MLS
Troposphere-to-Stratosphere Transport of VSLS
Simulations of the transport of idealized short-lived tracers
Comparison of ozone profiles from Broadmeadows and Macquarie Island,
Can the increase of Polar Stratospheric Clouds explain the Antarctic Winter Tropospheric warming? Tom Lachlan-Cope (W. M. Connolley, J. Turner, H. Roscoe,
Presentation transcript:

Figure (a-c). Latitude-height distribution of monthly mean ozone flux for the months of (a) January, (b) April and (c) July averaged over years 2000 to The color contours are the 2-D (up-down, north-south) magnitudes normalized to a fixed grid box (300 km in latitude, 1.5 km in vertical height, ratio of 200:1) and expressed in units of ppb/day for that box. The arrows are unit vectors showing the direction of the contoured flux from each grid box. The thick black dashed line shows the 100 hPa surface; the cyan line, the 2- PVU estimate of the tropopause; the green line, the 380 K surface; the dark blue lines, the 250 ppb O 3 surface (upper) and the 120 ppb O 3 surface (lower); and the black line, the e90 tropopause. These latter quantities are approximate, being derived from the monthly zonal mean values and not from the monthly zonal average of the individual profiles. Fig (d-e). Annual cycles of monthly mean, hemisphere- averaged O 3 fluxes (as Tg/yr) for years as measured across (d) 100 hPa and (e) the different iso-surfaces of 250 ppb O 3 (dashed red line), 120 ppb O 3 (dash-dot blue) and e90 tropopause (solid black). The true flux across 100 hPa ([w x O 3 ], dashed lines) is accumulated very time step from the O 3 advection; whereas the common approximation is calculated from the monthly mean residual circulation ([w*]) and zonal mean O 3 ([O 3 ]). The tropospheric column (TC) method accumulates the net change in tropospheric column defined by one of the above iso-surfaces every advection step. Fig (f-g). Latitudinal distribution of O 3 fluxes (as Tg/yr) averaged over 3-month seasons (DJF, solid cyan; MAM, dashed green; JJA, dotted red; SON, dash-dot black) for years across 100 hPa (f) using the residual circulation approximation ([w*]x[O 3 ]) and across the e90 tropopause (g). (h-i) Twelve-month running mean of normalized NH STE O 3 fluxes calculated: with the tropospheric column (TC) method across the e90 tropopause (solid black) and the 250 ppb O 3 iso- surface (solid red); with the lowermost stratosphere (LS) budget method using e90 tropopause (dashed black) and 250 ppb O 3 (dashed red) as the lower boundary; and with the exact flux across 100 hPa (solid green) and the residual circulation at 100 hPa (dashed green). For each method the mean values (as Tg/yr) and correlation coefficients of the interannual variability (lag = 0) with the TC-e90 method are given in the legend. (h) Results are from ECMWF-IFS Cycle 29 show much greater correlations than (i) results from Cycle 36. For a time lag of 3 months, the correlation coefficient of [w x O 3 ] increase to 0.97 (Cycle 29) and to 0.76 (Cycle 36). Is the residual vertical velocity a good proxy for Stratosphere-Troposphere Exchange of ozone? Juno Hsu & Michael Prather, UC Irvine Stratosphere-troposphere exchange (STE) of ozone is key in the budget of tropospheric ozone, in turn affecting climate forcing and global air quality. We investigate the ozone flux pathways in the lowermost stratosphere and compare three commonly used ozone flux diagnostics across the tropopause and nearby iso-surfaces of ozone and pressure by using the UCI chemistry-transport model driven by two different European Centre forecast fields (cycles 29 and 36). STE of ozone calculated based on the ozone mass budget of the lowermost stratosphere and of the tropospheric ozone column yields similar results. However, using the vertical residual velocity as a proxy at best captures the phase of the northern hemisphere (NH) seasonal cycle but fails to capture the interannual variability. The commonly exercised notion that the strength of Brewer-Dobson circulation (BDC) controls STE is not upheld. Climate-change BDC by itself cannot diagnose the ozone STE. Fig (z). The UCI CTM tested this hypothesis with an 8-year set of ECMWF forecast meteorology (years ) using two very different versions: merged cycles 29/31 and the more recent cycle 36. The CTM resolution is T42L57 and uses standard UCI chemistry (Linoz v2 for the stratosphere). Cycle 36 has a much more stagnant lower stratosphere as is diagnosed by STE O 3 flux below. The classic diagnostic test of age-of-air vs. N 2 O (Strahan et al., 2011, JGR) is shown here for both cycles with observations approximated (green line).