The Microwave Temperature Profiler (MTP) on START-08 MJ Mahoney - JPL/Caltech Julie Haggerty - NCAR Jan 9, 2008.

Slides:



Advertisements
Similar presentations
Atmospheric Structure
Advertisements

METO621 Lesson 18. Thermal Emission in the Atmosphere – Treatment of clouds Scattering by cloud particles is usually ignored in the longwave spectrum.
GOES Cloud Products and Cloud Studies Height Techniques Introduction GOES Sounder Currently there are three techniques being used to generate cloud top.
Distribution of H 2 O and SO 2 in the atmosphere of Venus Yung Y. 1, Zhang X. 1, Liang M.-C. 2 and Parkinson C. 3 1 California Institute of Technology.
Microwindow Selection for the MIPAS Reduced Resolution Mode INTRODUCTION Microwindows are the small subsets of the complete MIPAS spectrum which are used.
Atmospheric Sounding Temperature and water vapor profiling Atmospheric sounding Atmospheric sounding is retrieving vertical profiles of temperature trace-
Mountain Waves entering the Stratosphere. Mountain Waves entering the Stratosphere: New aircraft data analysis techniques from T-Rex Ronald B. Smith,
Atmospheric Emission.
Weighting Functions for Microwave and Infra-Red Satellite Nadir Sounding Remote Sensing I Lecture 7 Summer 2006.
Gravity Waves – #1 The NSF/NCAR G-V Research Aircraft: A New Observing Platform for Environmental Research.
Lessons 22,23,24 Upper Level Winds
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.
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.
Gravity Waves Geraint Vaughan University of Manchester, UK
MICROWAVE TEMPERATURE PROFILER (mTP)
LIDAR: Introduction to selected topics
Comparison of temperature data from HIPPO-1 flights using COSMIC profiles and Microwave Temperature Profiler. Kelly Schick 1,2,3 and Julie Haggerty, Ph.D.
Horizontal Distribution of Ice and Water in Arctic Stratus Clouds During MPACE Michael Poellot, David Brown – University of North Dakota Greg McFarquhar,
Chapter 5 Remote Sensing Crop Science 6 Fall 2004 October 22, 2004.
Evaluation of Microwave Scatterometers and Radiometers as Satellite Anemometers Frank J. Wentz, Thomas Meissner, and Deborah Smith Presented at: NOAA/NASA.
Boundary layer temperature profile observations using ground-based microwave radiometers Bernhard Pospichal, ISARS 2006 Garmisch-Partenkirchen AMMA - Benin.
Page 1 Validation by Balloons and Aircraft - ESRIN - 9– 13 December 2002 Observations of aerosol and clouds obtained during the M-55 Geophysica ENVISAT.
William Crosson, Ashutosh Limaye, Charles Laymon National Space Science and Technology Center Huntsville, Alabama, USA Soil Moisture Retrievals Using C-
Lesson 01 Atmospheric Structure n Composition, Extent & Vertical Division.
Physics of the Atmosphere II
COSMIC GPS Radio Occultation Temperature Profiles in Clouds L. LIN AND X. ZOU The Florida State University, Tallahassee, Florida R. ANTHES University Corporation.
Jet Stream. 250 mb isotach Main Upper Tropospheric Jets Closely Associated with the Tropopause.
HIRDLS Ozone V003 (v ) Characteristics B. Nardi, C. Randall, V.L. Harvey & HIRDLS Team HIRDLS Science Meeting Boulder, Jan 30, 2008.
Water Vapour & Cloud from Satellite and the Earth's Radiation Balance
UTLS Transport & STE Summary “Finding Nemo” Gettelman, Neu, Mullendore.
Center for Satellite Applications and Research (STAR) Review 09 – 11 March 2010 Using CALIPSO to Explore the Sensitivity to Cirrus Height in the Infrared.
COMPARATIVE TEMPERATURE RETRIEVALS BASED ON VIRTIS/VEX AND PMV/VENERA-15 RADIATION MEASUREMENTS OVER THE NORTHERN HEMISPHERE OF VENUS R. Haus (1), G. Arnold.
Stratosphere-Troposphere Analyses of Regional Transport (START) Experiment Investigators: Laura Pan (PI) Andy Weinheimer (Integration and Payload) Rushan.
BRIAN J. DROUIN, VIVIENNE PAYNE, FABIANO OYAFUSO, KEEYOON SUNG, Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Dr., Pasadena,
The Influence of loss saturation effects on the assessment of polar ozone changes Derek M. Cunnold 1, Eun-Su Yang 1, Ross J. Salawitch 2, and Michael J.
How accurately we can infer isoprene emissions from HCHO column measurements made from space depends mainly on the retrieval errors and uncertainties in.
The Deep Convective Clouds and Chemistry (DC3) Field Experiment Mary C. Barth (NCAR), W. H. Brune (PSU), C. A. Cantrell (U. Colorado), S. A. Rutledge (CSU),
Inertia-Gravity waves and their role in mixing Geraint Vaughan University of Manchester, UK.
Satellites Storm “Since the early 1960s, virtually all areas of the atmospheric sciences have been revolutionized by the development and application of.
Horizontal Variability In Microphysical Properties of Mixed-Phase Arctic Clouds David Brown, Michael Poellot – University of North Dakota Clouds are strong.
A Combined Radar-Radiometer Approach to Estimate Rain Rate Profile and Underlying Surface Wind Speed over the Ocean Shannon Brown and Christopher Ruf University.
Layers of the Atmosphere 1.  The atmosphere is divided into layers according to major changes in its temperature.  Gravity holds the layers of the atmosphere.
Atmosphere Layers. Vertical Structure of the Earth’s Atmosphere Vertical temperature (T) profile: troposphere stratosphere mesosphere Thermosphere (contains.
1 Atmospheric Radiation – Lecture 13 PHY Lecture 13 Remote sensing using emitted IR radiation.
Transport of Air from the Tropical Upper Troposphere into the Extratropical Lower Stratosphere Kenneth Bowman, Cameron Homeyer, Dalon Stone - Texas A&M.
Three-year analysis of S-HIS dual-regression retrievals using co-located AVAPS and CPL Measurements D. H. DeSlover, H. E. Revercomb, J. K. Taylor, F. Best,
Earth’s Atmosphere.
Radiometric Measurements of Whitecaps and Surface Fluxes Magdalena D. Anguelova Remote Sensing Division Naval Research Laboratory Washington, DC, USA In.
Microwave Emission Signature of Snow-Covered Lake Ice Martti Hallikainen (1), Pauli Sievinen (1), Jaakko Seppänen (1), Matti Vaaja (1), Annakaisa von Lerber.
The NCAR Microwave Temperature Profiler: Data Applications from Recent Deployments Julie Haggerty, Kelly Schick, Chris Davis National Center for Atmospheric.
Comparison of Temperature Data from HIPPO-1 Flights Using COSMIC and Microwave Temperature Profiler Kelly Schick 1,2,3 and Julie Haggerty 4 1 Monarch High.
17.1 Atmosphere Characteristics  D) Variable Components Water vapor 1) Water vapor is the source of all clouds and precipitation. water vapor absorbs.
Challenges associated with ice and large particles in the TTL
G. Mevi1,2, G. Muscari1, P. P. Bertagnolio1, I. Fiorucci1
Seasonal Differences of UTLS Exchange Processes between Spring and Summer in the Subtropics and Polar Region Simone Tilmes, Laura Pan, Louisa Emmons, Hans.
Winds in the Polar Regions from MODIS: Atmospheric Considerations
G. Mevi1,2, G. Muscari1, P. P. Bertagnolio1, I. Fiorucci1
Microwave Remote Sensing
Earth’s Atmosphere.
The Earth’s Warm Fuzzy Blanket
University of Colorado and NCAR START08/Pre HIPPO Workshop
The Earth’s Warm Fuzzy Blanket
GOES -12 Imager April 4, 2002 GOES-12 Imager - pre-launch info - radiances - products Timothy J. Schmit et al.
The Earth’s Atmosphere
ExUTLS dynamics and global observations
Cirrus Clouds near the mid-latitude tropopause
REM Sleep Reorganizes Hippocampal Excitability
The Layered Atmosphere:
6.1: Properties of the Atmosphere
Peering through Jupiter’s clouds with radio spectral imaging
Presentation transcript:

The Microwave Temperature Profiler (MTP) on START-08 MJ Mahoney - JPL/Caltech Julie Haggerty - NCAR Jan 9, 2008

The NSF/NCAR GV Microwave Temperature Profiler (MTP) Top View Bottom View Radiometer Frequency Synthesizer DC Power Supplies Cal Target Controller Board Step Motor Scan Mirror HDPE Window

Molecular oxygen absorption is the result of 44 rotational spectral lines from 50 to 835 GHz; 37 lines are in the 60 GHz band. Below ~10 km the lines are heavily pressure- broadened and line shape is not important. Above 10 km line shape starts to matter. The Molecular Oxygen Absorption Spectrum (0-20 km)

Applicable Height In the R-J limit the oxygen emission from a thin layer (dr) is proportional to the temperature times the absorption coefficient times the layer thickness attenuated by the intervening absorption: where W(r) is the weighting function. If the absorption coefficient is nearly constant and the temperature changes proportional to range (r) then: MTP Measurements Technique

MTP Performance During CRAVE Above: The overall MTP performance relative to flight level for 23 comparisons with Ticosondes (1-sigma error bars are shown). Left: Examples of two MTP retrievals (pink) compared to Ticosondes (white).

Data Products - Temperature Profile An Altitude Temperature Profile (ATP) from the NASA DC-8 MTP. The yellow dots are the retrieved temperatures, the horizonal yellow line is the aircraft altitude and the horizontal dashed line is the tropopause altitude. Other information is also shown.

Data Products - Temperature Curtain CTC for DC-8 TOTE-VOTE transit flight from Fairbanks, Alaska to Hawaii Flight level is black trace, tropopause is shown as white dots The polar jet is at 57N and the subtropical jet is at 33N; note double trop region

. ATPs can be used to identify constant theta, or isentrope, levels -- the streamlines on which air parcels flow. The figure above illustrates DC-8 observations of a dramatic mountain lee wave which occurred over the Norwegian Mountains on January 25, 2000 during the first SOLVE campaign. The green area shows the terrain cross-section, while the black traces show MTP isentropes and the blue trace the DC-8 flight altitude. Data Products - Isentropes A. Dornbrack et al., Evidence for inertia-gravity waves forming polar stratospheric clouds over Scandinavia, J. Geophys. Res., 107(D20), 8287, doi: /2001JD000452, 2002.