Carbon Monoxide and Ozone measurements in the Canadian High Arctic

Slides:



Advertisements
Similar presentations
Landscape Temperature and Frozen/Thawed Condition over Alaska with Infrared and Passive Microwave Remote Sensing Determination of Thermal Controls on Land-Atmosphere.
Advertisements

Mars’ North and South Polar Hood Clouds Jennifer L. Benson Jet Propulsion Laboratory, California Institute of Technology July 22, 2010 Copyright 2010 California.
A U R A Satellite Mission T E S
NO X Chemistry in CMAQ evaluated with remote sensing Russ Dickerson et al. (2:30-2:45PM) University of Maryland AQAST-3 June 13, 2012 Madison, WI The MDE/UMD.
Interpreting MLS Observations of the Variabilities of Tropical Upper Tropospheric O 3 and CO Chenxia Cai, Qinbin Li, Nathaniel Livesey and Jonathan Jiang.
24/6/05Dr. J.J. Remedios, EOEP review, 27/6/ Highlights of Atmospheric Science from ESA Satellites J.J. Remedios EOS-SRC, Physics and Astronomy,
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California Observing System Simulation.
METO 621 Lesson 27. Albedo 200 – 400 nm Solar Backscatter Ultraviolet (SBUV) The previous slide shows the albedo of the earth viewed from the nadir.
Warm Up 3/4/08 True or False: The seasons are caused by changes in Earth’s distance from the sun. False Does land or water heat more rapidly? Land heats.
Figure 1 Figure 8 Figure 9Figure 10 Altitude resolved mid-IR transmission of H 2 O, CH 4 and CO 2 at Mauna Loa Anika Guha Atmospheric Chemistry Division,
ACKNOWLEDGEMENTS We are grateful to the MOPITT team, especially the groups at University of Toronto and the National Center for Atmospheric Research (NCAR),
Monitoring of tropospheric methane from space: problems and solutions Leonid Yurganov, Larrabee Strow, Scott Hannon University of Maryland Baltimore County,
Page 1 Sciamachy Validation Workshop – Bremen December 2004 Contribution to the validation of SCIAMACHY scientific data products for CO, CH 4, CO.
Institute of Environmental Physics University of Bremen Retrieval of Tropospheric Water Vapour from FTIR Solar Absorption Measurements 1 Department of.
The ozone vertical structure determining from ground-based Fourier spectrometer solar IR radiation measurements Ya.A. Virolainen, Yu.M. Timofeyev, D.V.
Water and Methane in the Upper Troposphere and Stratosphere based on ACE-FTS Measurements Acknowledgements: The Canadian Space Agency (CSA) is the primary.
Retrieving cloud optical depth and ice particle size using thermal infrared radiometry: Application to the monitoring of thin ice clouds in an arctic environment.
The Atmosphere: Structure and Temperature
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 1 Atmospheric Infrared.
PARIS-IR U of T FTS TAO Figure 1. The experimental setup for the mini-MANTRA FTS intercomparison campaign. The University of Toronto’s Balloon-Borne Fourier.
Infrared Interferometers and Microwave Radiometers Dr. David D. Turner Space Science and Engineering Center University of Wisconsin - Madison
ARCTAS BrO Measurements from the OMI and GOME-2 Satellite Instruments
BrO Retrievals for UV-Visible Ground-Based Measurements Cristen Adams 1, Annemarie Fraser 1, Kimberly Strong 1, Robyn Schofield 2 1 Department of Physics,
MONTHLY CO AND FIRE COUNTS IN THREE NORTHERN HEMISPHERE REGIONS AND IN THREE LOW LATITUDE REGIONS  With MOPITT CO data and ATSR fire count data, CO emission.
1 Partial and total column SFIT2 retrievals from Eureka DA8 and PARIS-IR FTIR spectra in spring 2004 – 2005, including comparisons with the ACE Satellite.
Objective Data  The outlined square marks the area of the study arranged in most cases in a coarse 24X24 grid.  Data from the NASA Langley Research Center.
1 The Organic Aerosols of Titan’s Atmosphere Christophe Sotin, Patricia M. Beauchamp and Wayne Zimmerman Jet Propulsion Laboratory, California Institute.
Combining Simultaneously Measured UV and IR Radiances from OMI and TES to Improve Tropospheric Ozone Profile Retrievals Dejian Fu 1, John Worden 1, Susan.
Atmosphere: Structure and Temperature Bell Ringers:  How does weather differ from climate?  Why do the seasons occur?  What would happen if carbon.
SPEAKERS: Gabriele Pfister, Scientist III, National Center for Atmospheric Research (NCAR) Brad Pierce, Physical Scientist, NOAA Salient Questions: 1.What.
Spectroscopic Study of Atmospheric Trace Gases Using PARIS-IR from Waterloo Atmospheric Observatory in 2005 and 2006 Dejian Fu, Kaley Walker, Keeyoon Sung,
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology JPL Proprietary Information Charles Miller,
OMI validation workshop - 22 nd June 2006 Louisa. J. Kramer (1), Paul. S. Monks (2), Roland. J. Leigh (1) (1) Earth Observation Science, Space Research.
17.1 Atmosphere Characteristics
Harmonizationof GOME, SCIAMACHY, GOME-2 ozone cross-sections Anna Serdyuchenko, John P. Burrows, Mark Weber, Wissam Chehade University of Bremen, Germany.
Retrieval of biomass burning aerosols with combination of near-UV radiance and near -IR polarimetry I.Sano, S.Mukai, M. Nakata (Kinki University, Japan),
The Atmosphere: Structure and Temperature
Diurnal and Seasonal Variations of Nitrogen Oxides Within Snowpack Air and the Overlying Atmosphere at Summit, Greenland C. Toro 1, R.E. Honrath 1†, L.J.
Composition of the Atmosphere 14 Atmosphere Characteristics  Weather is constantly changing, and it refers to the state of the atmosphere at any given.
A Brief Overview of CO Satellite Products Originally Presented at NASA Remote Sensing Training California Air Resources Board December , 2011 ARSET.
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California Atmospheric Infrared Sounder.
Convective Transport of Carbon Monoxide: An intercomparison of remote sensing observations and cloud-modeling simulations 1. Introduction The pollution.
Figure 1 Figure 8 Figure 9Figure 10 Altitude resolved mid-IR transmission of H 2 O, CH 4 and CO 2 at Mauna Loa Anika Guha Atmospheric Chemistry Division,
The Atmosphere: Structure & Temperature. Atmosphere Characteristics Weather is constantly changing, and it refers to the state of the atmosphere at any.
Ground-based measurements made with PARIS-IR during the ACE Canadian Arctic Validation Campaign in 2004 and 2005 Keeyoon Sung, Kaley Walker, Chris Boone.
WP4: Observations from ground networks. Work package 4 OBSERVATIONS FROM GROUND NETWORKS.
Comparisons of ACE-FTS and PARIS-IR Measurements of Several Trace Gases in the Northern Mid-latitude Atmosphere Dejian Fu, Kaley A. Walker, Keeyoon Sung,
Potential of Observations from the Tropospheric Emission Spectrometer to Constrain Continental Sources of Carbon Monoxide D. B. A. Jones, P. I. Palmer,
Chapter 17 Study Guide Answers
1.
The Atmosphere: Structure & Temperature
Royal Meteorological Institute of Belgium
Planetary Energy Budget
Carbon products: Calibration and validation approaches
Infrared Spectroscopy of the Atmosphere using the FTIR Spectrometer
Carbon monoxide from shortwave infrared measurements of TROPOMI: Algorithm, Product and Plans Jochen Landgraf, Ilse Aben, Otto Hasekamp, Tobias Borsdorff,
J. Kar (UT), H. Bremer (UB), James R. Drummond (UT), F
Colin Michel1, C. Amelynck3, M. Aubinet1, A. Bachy1, P. Delaplace2, A
Explain the significance of Earth’s Atmosphere
Whitney Bader CANDAC/PAHA workshop
Atmosphere Characteristics
Weather: Characteristics & Fronts
Diurnal Variation of Nitrogen Dioxide
By Narayan Adhikari Charles Woodman
The Greenhouse Effect Electromagnetic (EM) radiation, radiation processes “Clear Sky” Exercise Earth-Sun System Greenhouse Gases “Cloudy Sky” Exercise.
Atmospheric CH4 and N2O measurements at Suva, Fiji
Eureka Stratospheric Ozone Differential Absorption LIDAR:
Eureka Stratospheric Ozone Differential Absorption LIDAR revived
Presentation transcript:

Carbon Monoxide and Ozone measurements in the Canadian High Arctic using infrared emission spectroscopy Tran, Sophie1 , Z. Mariani2, E. Lutsch1, S. Conway1, M. Palm3, P. Rowe4, G. Manney5, L. Millan6 and K. Strong1 1 Department of Physics, University of Toronto, Toronto, ON, Canada 2 Cloud Physics and Severe Weather Section, Environment and Climate Change Canada, Toronto, ON, Canada 3 Institute of Environmental Physics, University of Bremen, Germany 4 Department of Geography, University of Idaho, Moscow, ID, USA 5 Department of Physics, New Mexico Institute of Mining and Technology, Socorro, NW, USA 6 NASA Jet Propulsion Laboratory, Pasadena, CA, USA Eureka, NU Image: https://nsidc.org/icelights/files/2010/11/arctic_ams.jpg Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Outline Context and motivation Instrument and measurement site Results for: Carbon Monoxide Ozone Conclusions Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Context and motivation Rapid climate change in the Arctic  importance to improve our knowledge about processes driving these changes, including the atmospheric composition. High Arctic  prolonged periods of total darkness in the winter and continuous daylight in the summer. Polar night To monitor and measure atmospheric composition, ground-based stations are equipped with Fourier Transform Spectrometers (FTS). However, most of them use the Sun as a light source… which leads to a measurement gap during polar night. FTIR measurements from 2007 to 2010 at Eureka (80°N), Nunavut, Canada. (Courtesy of Rodica Lindenmaier) Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Context and motivation During December 1992 and February 1993, Notholt at al. performed the first FTIR measurements to utilize the moon as the infrared source during the polar night at Ny Alesund, Spitsbergen (78.9°N, 11.9°E) to obtain the column densities of several trace gases. Zenith column densities (mol cm-2): Measurements were taken for about a week around full moon. (Notholt et al., 1993) They could also monitor the seasonal cycles of certain trace gases  However, the measurements depend on the moon’s phases and more than half of the polar night can not be documented. (Notholt et al., 1997) Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Context and motivation In addition to documenting the atmospheric composition during the polar night, it’s also important to have good data coverage during the rest of the year. Example of trace gas total columns measured by the 125HR from 2010 to 2015: measurement gaps are due to polar night, weather, reduced on-site operations, instrument issues CO O3 CH4 N2O Need to have complementary measurements to assure the best data coverage through the year Sophie Tran – CAP 2016, June 15th

Retrievals of trace gas column densities Infrared emission spectroscopy E-AERI = Extended-range Atmospheric Emitted Radiance Interferometer Infrared Fourier Transform Spectrometer (FTS) with 1cm-1 resolution Measurements of accurately calibrated downwelling infrared thermal emission from the atmosphere Extended wavelength range covers 400-3000 cm-1 (3-25 µm) to investigate the IR surface cooling in the Arctic High sensitivity to tropospheric trace gases Measurements are independent of sunlight Retrievals of trace gas column densities Retrieval windows Using new SFIT4 retrieval algorithm (before: SFIT2 v393_MP Emission Add-on) Can currently retrieve CO, CH4, N2O, and O3 Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Measurement sites PEARL - Ridge Lab PEARL = Polar Environment Atmospheric Research Laboratory in Eureka, Nunavut (80.05°N, 86.42°W) 610 m 10 m PEARL - 0PAL Ridge Lab Instruments: E-AERI from Oct 2008 to Sept 2009 125HR Bruker from 2006 to 2015 altitude Instruments: P-AERI from 2006 to Feb 2009 E-AERI from 2011 to 2015 0PAL Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Timeseries of column densities for several trace gases Gaps in the dataset are due to cloudy days, no data recorded or no convergence in the retrieval Time series combining two datasets: P-AERI: 2006 to 2009 E-AERI: 2008 to 2015 Measurements of trace gas even during the polar night CO O3 CH4 N2O Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Carbon monoxide AERI 125HR Clear seasonal cycle of CO Identification of CO enhancements periods Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Carbon monoxide Biomass burning event in 2014 125HR data: courtesy from E. Lutsch (paper in preparation) 125HR 125HR 125HR CO AERI  Two main biomass burning events occurred in August 2014, also observed by the AERI instrument (Flexpart model) Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Ozone AERI 125HR Clear seasonal cycle of ozone Good correlation between AERI and 125HR Ozone depletion events in 2007 and 2011 are recorded on both datasets Ozone enhancement event in winter Sophie Tran – CAP 2016, June 15th

Tropopause height Anti-correlation between the tropopause height and ozone total columns Combined with high ozone amount in the atmosphere on January 14-15 (2012) Exceptional ozone enhancement event during the polar night at Eureka in 2012 Source ozone maps: Environment Canada Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Ozone depletion Ozone depletion events identified in 2007 and 2011 at Eureka (Rösevall et al., 2007 ; Kuttippurath et al., 2009; Manney et al., 2011; Lindenmaier et al., 2012) Ozone depletion event occurred from February 7 to February 22, 2016  During the polar night Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Conclusions Use of infrared emission spectroscopy to document the polar night atmospheric trace gas composition and is a great complement to the solar-viewing instruments Clear seasonal cycle of CO and ozone with maximum column densities in winter-early spring due to the absence of photochemical destruction Identification of carbon monoxide enhancements due to biomass burning plumes reaching PEARL in the summer Observation of stratospheric influence on ozone column densities in January 2012 in the Arctic even though the tropopause height seems to drive the ozone amount measured by the AERI Ozone depletion can be monitored using ground-based instrument during the winter Sophie Tran – CAP 2016, June 15th

Sophie Tran – CAP 2016, June 15th Acknowledgements CANDAC and PEARL are supported by: ARIF, AIF/NSRIT, CFCAS, CFI, CSA, EC, GOC-IPY, NSERC, OIT, ORF, INAC, and PCSP Logistical and operational support at Eureka: CANDAC operators Team at the EC Weather Station PEARL site manager Pierre Fogal CANDAC/PEARL PI James R. Drummond CANDAC data manager Yan Tsehtik Canadian Arctic ACE Validation Campaigns supported by: CSA, EC, NSERC, and NSTP PI Kaley Walker Special thanks to Pierre Fogal, Paul Loewen, Mike Maurice, Peter McGovern and Kaley Walker for assistance with ACE Validation Campaigns. Sophie Tran – CAP 2016, June 15th