Analysis of tropical cloud systems using a cloud-top height data by geostationary satellite split-window measurements trained with CloudSat data NISHI,

Slides:



Advertisements
Similar presentations
Robin Hogan, Richard Allan, Nicky Chalmers, Thorwald Stein, Julien Delanoë University of Reading How accurate are the radiative properties of ice clouds.
Advertisements

Robin Hogan Julien Delanoe University of Reading Remote sensing of ice clouds from space.
Image Interpretation for Weather Analysis Part I 29 October 2009 Dr. Steve Decker.
Enhancement of Satellite-based Precipitation Estimates using the Information from the Proposed Advanced Baseline Imager (ABI) Part II: Drizzle Detection.
Pathfinder –> MODIS -> VIIRS Evolution of a CDR Robert Evans, Peter Minnett, Guillermo Podesta Kay Kilpatrick (retired), Sue Walsh, Vicki Halliwell, Liz.
Precipitation Products PPS Anke Thoss, SMHI User Workshop, February 2015, Madrid.
TRMM Tropical Rainfall Measurement (Mission). Why TRMM? n Tropical Rainfall Measuring Mission (TRMM) is a joint US-Japan study initiated in 1997 to study.
1 An initial CALIPSO cloud climatology ISCCP Anniversary, July 2008, New York Dave Winker NASA LaRC.
1 A First Look at Mid-Level Clouds Using CloudSat, CALIPSO, and MODIS Data Stanley Q. Kidder, J. Adam Kankiewicz, Thomas H. Vonder Haar Cooperative Institute.
Satellite Rainfall Estimation Robert J. Kuligowski NOAA/NESDIS/STAR 3 October 2011 Workshop on Regional Flash Flood Guidance System—South America Santiago.
Microwindow Selection for the MIPAS Reduced Resolution Mode INTRODUCTION Microwindows are the small subsets of the complete MIPAS spectrum which are used.
ATS 351 Lecture 8 Satellites
16/06/20151 Validating the AVHRR Cloud Top Temperature and Height product using weather radar data COST 722 Expert Meeting Sauli Joro.
Image Interpretation for Weather Analysis Part I 21 October 2010 Dr. Steve Decker.
A 21 F A 21 F Parameterization of Aerosol and Cirrus Cloud Effects on Reflected Sunlight Spectra Measured From Space: Application of the.
Surface Skin Temperatures Observed from IR and Microwave Satellite Measurements Catherine Prigent, CNRS, LERMA, Observatoire de Paris, France Filipe Aires,
Millimeter and sub-millimeter observations for Earth cloud hunting Catherine Prigent, LERMA, Observatoire de Paris.
An artificial neural networks system is used as model to estimate precipitation at 0.25° x 0.25° resolution. Two different networks are being developed,
GOES-13 Science Team Report SST Images and Analyses Eileen Maturi, STAR/SOCD, Camp Springs, MD Andy Harris, CICS, University of Maryland, MD Chris Merchant,
Image Interpretation for Weather Analysis Part I 11 November 2008 Dr. Steve Decker.
Model and remote-sensing data SOEE1400 Lecture 5.
Incorporating Meteosat Second Generation Products in Season Monitoring Blessing Siwela SADC Regional Remote Sensing Unit November
Spaceborne Weather Radar
Satellite basics Estelle de Coning South African Weather Service
Cyclone composites in the real world and ACCESS Pallavi Govekar, Christian Jakob, Michael Reeder and Jennifer Catto.
Influence of ice supersaturation, temperature and dynamics on cirrus occurrence near the tropopause N. Lamquin (1), C.J. Stubenrauch (1), P.-H. Wang (2)
Applications and Limitations of Satellite Data Professor Ming-Dah Chou January 3, 2005 Department of Atmospheric Sciences National Taiwan University.
Anthony DeAngelis. Abstract Estimation of precipitation provides useful climatological data for researchers; as well as invaluable guidance for forecasters.
Orbit Characteristics and View Angle Effects on the Global Cloud Field
Satellite and Radar Imagery
Lecture 6 Observational network Direct measurements (in situ= in place) Indirect measurements, remote sensing Application of satellite observations to.
DoD Center for Geosciences/Atmospheric Research at Colorado State University Annual Review April 17-19, Development of Satellite Products for the.
Precipitation Retrievals Over Land Using SSMIS Nai-Yu Wang 1 and Ralph R. Ferraro 2 1 University of Maryland/ESSIC/CICS 2 NOAA/NESDIS/STAR.
A43D-0138 Towards a New AVHRR High Cloud Climatology from PATMOS-x Andrew K Heidinger, Michael J Pavolonis, Aleksandar Jelenak* and William Straka III.
AGU 2002 Fall Meeting NASA Langley Research Center / Atmospheric Sciences Validation of GOES-8 Derived Cloud Properties Over the Southeastern Pacific J.
SATELLITE METEOROLOGY BASICS satellite orbits EM spectrum
Estimation of Cloud and Precipitation From Warm Clouds in Support of the ABI: A Pre-launch Study with A-Train Zhanqing Li, R. Chen, R. Kuligowski, R. Ferraro,
Weather Forecasting Chapter 9 Dr. Craig Clements SJSU Met 10.
BIOPHYS: A Physically-based Algorithm for Inferring Continuous Fields of Vegetative Biophysical and Structural Parameters Forrest Hall 1, Fred Huemmrich.
Optical properties Satellite observation ? T,H 2 O… From dust microphysical properties to dust hyperspectral infrared remote sensing Clémence Pierangelo.
Andrew Heidinger and Michael Pavolonis
VALIDATION AND IMPROVEMENT OF THE GOES-R RAINFALL RATE ALGORITHM Background Robert J. Kuligowski, Center for Satellite Applications and Research, NOAA/NESDIS,
Center for Satellite Applications and Research (STAR) Review 09 – 11 March 2010 Using CALIPSO to Explore the Sensitivity to Cirrus Height in the Infrared.
CBH statistics for the Provisional Review Curtis Seaman, Yoo-Jeong Noh, Steve Miller and Dan Lindsey CIRA/Colorado State University 12/27/2013.
Yuying Zhang, Jim Boyle, and Steve Klein Program for Climate Model Diagnosis and Intercomparison Lawrence Livermore National Laboratory Jay Mace University.
Next Week: QUIZ 1 One question from each of week: –5 lectures (Weather Observation, Data Analysis, Ideal Gas Law, Energy Transfer, Satellite and Radar)
Modeling GOES-R µm brightness temperature differences above cold thunderstorm tops Introduction As the time for the launch of GOES-R approaches,
ISCCP Calibration 25 th Anniversary Symposium July 23, 2008 NASA GISS Christopher L. Bishop Columbia University New York, New York.
Preparing for GOES-R: old tools with new perspectives Bernadette Connell, CIRA CSU, Fort Collins, Colorado, USA ABSTRACT Creating.
Use of Solar Reflectance Hyperspectral Data for Cloud Base Retrieval Andrew Heidinger, NOAA/NESDIS/ORA Washington D.C, USA Outline " Physical basis for.
ISCCP SO FAR (at 30) GOALS ►Facilitate "climate" research ►Determine cloud effects on radiation exchanges ►Determine cloud role in global water cycle ▬
Daily observation of dust aerosols infrared optical depth and altitude from IASI and AIRS and comparison with other satellite instruments Christoforos.
Real-time Display of Simulated GOES-R (ABI) Experimental Products Donald W. Hillger NOAA/NESDIS, SaTellite Applications and Research (STAR) Regional And.
Visible optical depth,  Optically thicker clouds correlate with colder tops Ship tracks Note, retrievals done on cloudy pixels which are spatially uniform.
Satellites Storm “Since the early 1960s, virtually all areas of the atmospheric sciences have been revolutionized by the development and application of.
An Overview of Satellite Rainfall Estimation for Flash Flood Monitoring Timothy Love NOAA Climate Prediction Center with USAID- FEWS-NET, MFEWS, AFN Presented.
Developing a Dust Retrieval Algorithm Jeff Massey aka “El Jeffe”
UCLA Vector Radiative Transfer Models for Application to Satellite Data Assimilation K. N. Liou, S. C. Ou, Y. Takano and Q. Yue Department of Atmospheric.
1 A conical scan type spaceborne precipitation radar K. Okamoto 1),S. Shige 2), T. Manabe 3) 1: Tottori University of Environmental Studies, 2: Kyoto University.
Assimilating Cloudy Infrared Brightness Temperatures in High-Resolution Numerical Models Using Ensemble Data Assimilation Jason A. Otkin and Rebecca Cintineo.
NASA, CGMS-44, 7 June 2016 Coordination Group for Meteorological Satellites - CGMS LIMB CORRECTION OF POLAR- ORBITING IMAGERY FOR THE IMPROVED INTERPRETATION.
Visible vicarious calibration using RTM
Benjamin Scarino, David R
Seung-Hee Ham and B.J. Sohn Seoul National University, Korea
DCC method implementation in FY3/MERSI and FY2
Robert Joycea, Pingping Xieb, and Shaorong Wua
Relationships inferred from AIRS-CALIPSO synergy
GOES visible (or “sun-lit”) image
Winds in the Polar Regions from MODIS: Atmospheric Considerations
Representing Climate Data II
Presentation transcript:

Analysis of tropical cloud systems using a cloud-top height data by geostationary satellite split-window measurements trained with CloudSat data NISHI, Noriyuki (Kyoto University) HAMADA, Atsushi (University of Tokyo) HIROSE, Hitoshi (Kyoto Universtiy)

Abstract New tropical-subtropical cloud top dataset has been completed and opened in our web-site. – Almost real-time update – Archive is available since June 2005 – Area covered by MTSAT-1R and MTSAT2 You can get cloud top height with 1-hour and 0.04° resolution – Best precision is obtained for upper tropospheric cloud – cirriform clouds, nimbostratus, cumulonimbus…

Tb (11μm) Example image on the web (19Z 01Jul2010) Tb (11μm)-Tb(12μm)) Optical Thickness SD for CloudTop CloudTop SD for Optical Thickness

Outline of the data We have made lookup tables for estimating the cloud-top height and visible optical thickness of upper-tropospheric clouds by the infrared brightness temperature (T B ) at 10.8 μm (T11) and its difference from T B at 12 μm (ΔT) measured by a geostationary satellite Influence of satellite zenith angle (SZA) on the brightness temperature around the rim of satellite field-of-view is reduced by creating LUT separately for the regions with a width of 15˚ SZA

Features – Hourly estimates (day&night) within wide area can be obtained by using only geostationary satellite data – Estimates have (ideally) no bias, since lookup tables were trained with cloud radar measurements onboard CloudSat – Reliability of estimate at each point is offered at the same time (less than 1 km for the upper-tropospheric clouds)

Estimation of cloud parameter by split-window method  Utilizing the diference of absorption coefficient between 11μm and 12μm  Particularly for ice phase  Applicable both daytime and night (with no use of visible channel) (After HITRAN2000)

Estimation of cloud parameter by split-window method  By using the difference between two channel, we can distinguish the difference of cloud top height between two clouds with same T11 value but different cloud top and optical depth 255K 270K Tb 11μm Tb 12μm DENSE 255K 270K 265K DENSE THIN

Split-window T B -- cloud top height, optical thickness high thick T 11, T 12 : 11,12um Tb z T : cloud top height τ : visible optical thickness  T := T 11 – T 12 Estimation by traditional method with only T 11 Observed value Model parameter

Problem in the method with using radiative transfer model  Simplified too much  Too sensitive to the variation of the model parameter We made lookup table by purely experically with cloud radar ・ We should prepare a different lookup table for each satellite.

Data 1: geostationary satellite  MTSAT-1R, MTSAT-2  11μm, 12μm T B (brightness temperature) – T 11, T 12 TOA radiation affected by cloud and water vapor  Resolution : 0.04 o lon/lat, every hour  Area and period  Jul 2006–  80 o E–160 o W , 45 o S–45 o N 10/ /06/07 学位申請論文公聴会

Data 2: CloudSat  94GHz ( wavelength ~ 3mm ) millimeter-wavelength radar  Resolution: horizontal 1.4 x 2.5km (only just below)  Sampling: Vertically 240m (resolution around 500m)  Merit  Cloud ice, cloud water can be observed, as well as light rain and snow  Possible to get almost all the data in whole cloud layer  Demerit  Observation region is narrow (~2km , only just below)  Only two local time 0130/1330LT  Attenuation due to heavy rain 高度 (km) ~5km ~500km Kochi-Univ. 11/ /06/07 学位申請論文公聴会

Extraction of sample 1. Extracting cloud radar observations that pass a MTSAT grid within 60 seconds from MTSAT observation, and averaging all the radar observation in a MTSAT grid 2. Defining more than two vertically continuous cloud echo bins as cloud layer (using cloud mask data) 3. Calculating:  MTSAT 4-point average: T 11,  T  CloudSat Cloud top height ( z top ) Optical thickness (  vis ) of the highest cloud layer → Regressing z top and  vis with T 11 and  T to obtain lookup table (LUT) ~ 5km MTSAT grid CloudSat swath 12/48

Lookup table 0˚ < Satellite Zenith Angle < 15˚ Dashed line: standard deviation (km) Cloud top estimate (km) CTOP revised version

Estimation error Dashed line: standard deviation (km) CTOP revised version

Example over the central Pacific Ocean BLACK: Our results (estimates, stdev) RED: Aqua/MODIS YDL2_06 (CO2-slicing) Model-based approaches tend to underestimate CTHs even for optically thick clouds such as cumulonimbus/nimbostratus

Veritical distribution of the cloud top Jul-Dec N-7.5N CTOP(revised version) Cloud top estimate (maskout: tau 288 and ΔT < 2.5) ) Large difference from CloudSat direct observation in the region of large zenith angle CloudSat: the highest of at least three continuous cloud mask CloudSat CTOP (revised version) Maximum around E and peak around km are well represented in CTOP

Upper tropospheric cloud top (11-17km) CloudSat CTOP (revised version) Jul-Dec N-7.5N Maximum over the maritime continent and presence of ITCZ/SPCZ are well represented in CTOP

CTOP statistics General distribution of the upper-tropospheric cloud top in CTOP is close to that of CloudSat CloudSat observation is sparse. We can use our CTOP dataset as a complementary one to study climatology and interannual variability of the upper tropospheric clouds. Some problems remain In large zenith angle region (edge of the MTSAT view), the CTOP distribution is somewhat different from that of CloudSat Due to the lack of the sample size in making LUT, the vercial distribution is still ‘noisy’

Revision to version 2 Improve the estimate for very thin clouds (High T 11 and large ΔT) – When making LUT, excluding the pixels that CloudSat indicates ‘no-cloud’ but T 11 is low Some technical revision – Matching the location of pixels of CloudSat and MTSAT, considering the zenith angle of MTSAT – Adjusting the parameters in local regression to extend the parameter range (T 11, ΔT) when making LUT – Avoiding the effect of small difference of viewing angle between T 11 and T 12 observations

Revision to version 2 Ver.1: when CloudSat shows no cloud, the cloud height is set at 0 km. Revised: do not use the pixel with CloudSat height less than 3 km. Ver.1 revised Regression curve around T11=270K Each point shows that each observation

Future plans Making lookup tables (LUTs) for other satellites – current geostationary satellites (MSG, GOES, etc.) – current orbital satellites (Aqua, NOAA, etc.) – past geostationary/orbital satellites for the study of climate  before CloudSat launch – Extension to the mid-latitude with objective analyisis dataset Seeking the possibility to analyze clouds with lower cloud top (<11km) – Congestus clouds…

Conclusion New tropical-subtropical cloud top dataset has been completed and opened in our web-site. – Almost real-time update – Archive is available since June 2005 – Area covered by MTSAT-1R and MTSAT2 You can get cloud top height with 1-hour and 0.04°resolution – Estimation error is also utilized – Best precision is obtained for upper tropospheric cloud – cirriform clouds, nimbostratus, cumulonimbus…

Cloud top dataset (CTOP)

FAQ Why do you use CloudSat rather than CALIPSO – In many cases, cloud top observed by CALIPSO is subvisible cirrus near the cold point tropopause. IR method is not applicable to such an altitude where the temperature does not decrease with height. If we select only the cloud with large optical thickness, we can do the same analysis. However, the result is not so different with one with CloudSat data.

FAQ Is this dataset can be available for any clouds? – No. The main target is visible cirrus, nimbostratus, and cumulonimbus, which has their top is between km. – Subvisible cirrus around the cold point tropopause cannot be included, since the hypothesis that the temperature decreases with height cannot be correct there. So, IR method is not good for that. – Lower cloud (< 11km) is not good for our method. The estimation error is fairly large.