International School on Applications with the Newest Multi-spectral Environmental Satellites held in Brienza from 18 to 24 Sep 2011

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International School on Applications with the Newest Multi-spectral Environmental Satellites held in Brienza from 18 to 24 Sep 2011 Paul Menzel, Valerio Tramutoli, & Filomena Romana

Su 1 4 pm Lecture 1 Instruments and Orbits Mo 9 12 am Lecture 2 Radiative Transfer in the Earth Atmosphere Homework 1 (due Thursday) Mo 2 5 pm Lab 1 Planck Function and Intro to Hydra Tu 9 12 am Review Lecture 1 & 2, Lab 1 Lecture 3 Spectral signatures from Earth Tu 2 5 pm Lab 2 Interrogating Multispectral Data We 9 12 am Review Lecture 3, Lab 2 Lecture 4 Sounding with broad band and hyperspectral IR Quiz 1 We 2 5 pm Lab 3 Investigations with Imagers and Sounders Th 9 12 am Review Quiz 1, Lecture 4, Lab 3 Homework 2 (due Saturday) Lecture 5 Microwave and time continuous (geostationary) measurements Th 2 5 pm Lab 4 Investigations of clouds and moisture with MODIS, AIRS and AMSU Lab Assign and start Student Projects Fr 9 12 am Review Homework 1, Lecture 5, Lab 4 Lab Student Projects Fr 2 5 pm Lab Student Projects Sa 9 12 am Lab Student Presentations using MODIS, IASI, AIRS, SEVIRI Review Homework 2 Lecture 6 Summary Quiz 2 2

Remote Sensing Schools have been held in Bologna, Italy (Sep 01) Rome, Italy (Jun 02) Maratea, Italy (May 03) Bertinoro, Italy (Jul 04) Andanes, Norway (Feb 06) Cape Town, South Africa (Apr 06) Krakow, Poland (May 06) Ostuni, Italy (Jun 06) Benevento, Italy (Jun 07) Sao Paulo, Brazil (Nov 07) Monteponi, Sardinia (Sep 08) Istanbul, Turkey (Oct 08) Perth, Western Australia (Feb 09) Sasso di Castalda, Italy (Jul 09) New Dehli, India (Feb 11)

Objective of School An in depth explanation of methods and techniques used to extract information from environmental satellite data, with emphasis on the latest measuring technologies. The course will consist of lectures, laboratory sessions, group lab projects, homework and tests. The results from each of the group projects will be presented to the class by the participating students. English is the official language of the School. All provided material will be in English. 4

Lectures and Labs Lectures and laboratory exercises emphasize investigation of high spatial resolution visible and infrared data (from MODIS and SEVIRI), high spectral resolution infrared data (from AIRS and IASI), and microwave sounding data (AMSU). Text for the classroom and a visualization tool for the labs are provided free; Applications with Meteorological Satellites is used as a resource text from ftp://ftp.ssec.wisc.edu/pub/menzel/ and HYDRA is used to interrogate and view multispectral data in the labs from http://www.ssec.wisc.edu/hydra/. Homework assignments and classroom tests are administered to verify that good progress is being was made in learning and mastering the materials presented. Classroom size is usually between twenty and thirty students. 5

Lectures 6

Applications with Meteorological Satellites is used as a resource text It is available for free at ftp://ftp.ssec.wisc.edu/pub/menzel/ CHAPTER 1 - EVOLUTION OF SATELLITE METEOROLOGY CHAPTER 2 - NATURE OF RADIATION * CHAPTER 3 - ABSORPTION, EMISSION, REFLECTION, AND SCATTERING * CHAPTER 4 - THE RADIATION BUDGET CHAPTER 5 - THE RADIATIVE TRANSFER EQUATION (RTE) * CHAPTER 6 - DETECTING CLOUDS * CHAPTER 7 - SURFACE TEMPERATURE * CHAPTER 8 - TECHNIQUES FOR DETERMINING ATMOSPHERIC PARAMETERS * CHAPTER 9 - TECHNIQUES FOR DETERMINING ATMOSPHERIC MOTIONS CHAPTER 10 - AN APPLICATION OF GEOSTATIONARY SATELLITE SOUNDING DATA CHAPTER 11 - SATELLITE ORBITS CHAPTER 12 - RADIOMETER DESIGN CONSIDERATIONS * CHAPTER 13 - ESTABLISHING CLIMATE RECORDS FROM MULTISPECTRAL MODIS MEASUREMENTS CHAPTER 14 - THE NEXT GENERATION OF SATELLITE SYSTEMS CHAPTER 15 INVESTIGATING LAND, OCEAN, AND ATMOSPHERE WITH MULTISPECTRAL MEASUREMENTS * * indicates chapters covered References, problems sets, and quizzes are included in the Appendices 7

Agenda includes material from Chapters 2, 3, 5, and 12 CHAPTER 2 - NATURE OF RADIATION 2.1 Remote Sensing of Radiation 2-1 2.2 Basic Units 2-1 2.3 Definitions of Radiation 2-2 2.5 Related Derivations 2-5 CHAPTER 3 - ABSORPTION, EMISSION, REFLECTION, AND SCATTERING 3.1 Absorption and Emission 3-1 3.2 Conservation of Energy 3-1 3.3 Planetary Albedo 3-2 3.4 Selective Absorption and Emission 3-2 3.7 Summary of Interactions between Radiation and Matter 3-6 3.8 Beer's Law and Schwarzchild's Equation 3-7 3.9 Atmospheric Scattering 3-9 3.10 The Solar Spectrum 3-11 3.11 Composition of the Earth's Atmosphere 3-11 3.12 Atmospheric Absorption and Emission of Solar Radiation 3-11 3.13 Atmospheric Absorption and Emission of Thermal Radiation 3-12 3.14 Atmospheric Absorption Bands in the IR Spectrum 3-13 3.15 Atmospheric Absorption Bands in the Microwave Spectrum 3-14 3.16 Remote Sensing Regions 3-14 CHAPTER 5 - THE RADIATIVE TRANSFER EQUATION (RTE) 5.1 Derivation of RTE 5-1 5.10 Microwave Form of RTE 5-28 CHAPTER 12 - RADIOMETER DESIGN CONSIDERATIONS 12.3 Design Considerations 12-1 8

Lectures are given with powerpoint presentations 9

Material includes equations c 2 /λt Planck s Law B(λ,T) = c 1 / λ 5 / [e -1] (mw/m 2 /ster/cm) where λ = wavelengths in cm T = temperature of emitting surface (deg K) c 1 = 1.191044 x 10-5 (mw/m 2 /ster/cm -4 ) c 2 = 1.438769 (cm deg K) Wien's Law db(λ max,t) / dλ = 0 where λ(max) =.2897/T indicates peak of Planck function curve shifts to shorter wavelengths (greater wavenumbers) with temperature increase. Note B(λ max,t) ~ T 5. Stefan-Boltzmann Law E = B(λ,T) dλ = T 4, where = 5.67 x 10-8 W/m2/deg4. o states that irradiance of a black body (area under Planck curve) is proportional to T 4. Brightness Temperature c 1 T = c 2 / [λ ln( + 1)] is determined by inverting Planck function λ 5 10 B λ

And some derivations, I = sfc B (T(p s )) (p s ) + ( p) B (T(p)) (p) p The emissivity of an infinitesimal layer of the atmosphere at pressure p is equal to the absorptance (one minus the transmittance of the layer). Consequently, ( p) (p) = [1 - ( p)] (p) Since transmittance is an exponential function of depth of absorbing constituent, p+ p p ( p) (p) = exp [ - k q g -1 dp] * exp [ - k q g -1 dp] = (p + p) p o Therefore ( p) (p) = (p) - (p + p) = - (p). So we can write I = sfc B (T(p s )) (p s ) - B (T(p)) (p). p which when written in integral form reads p s I = sfc B (T(p s )) (p s ) - B (T(p)) [ d (p) / dp ] dp. o 11

Labs 12

HYperspectral viewer for Development of Research Applications - HYDRA MSG, GOES Freely available software For researchers and educators Computer platform independent Extendable to more sensors and applications Based in VisAD (Visualization for Algorithm Development) Uses Jython (Java implementation of Python) runs on most machines 512MB main memory & 32MB graphics card suggested on-going development effort Rink et al, BAMS 2007 MODIS, AIRS, IASI, AMSU, CALIPSO Developed at CIMSS by Tom Rink Tom Whittaker Kevin Baggett With guidance from Paolo Antonelli Liam Gumley Paul Menzel Allen Huang http://www.ssec.wisc.edu/hydra/ 13

Viewing remote sensing data with HYDRA 14

AIRS 20-July-2002 Ascending LW_Window 15

IASI 16

AMSU 17

Access to visualization tools and data For hydra http://www.ssec.wisc.edu/hydra/ For MODIS data and quick browse images http://rapidfire.sci.gsfc.nasa.gov/realtime For MODIS data orders http://ladsweb.nascom.nasa.gov/ For AIRS data orders http://daac.gsfc.nasa.gov/ 18

Orbits and Instruments Lectures in Brienza 18 Sep 2011 Paul Menzel UW/CIMSS/AOS

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All Sats on NASA J-track http://science.nasa.gov/realtime/jtrack/3d/jtrack3d.html 21

M E T E O R 3 M ( R u s sia n F e d e r a t io n ) F Y - 1 ( C h in a ) Oc e a n o g ra p h ic Missio n s A T G O E S -E (U S A ) 7 5 W I ON A R Y OR B I T 8 5 0 K M G O E S - W ( U S A ) 135W Hig h -re so lu tio n La n d u se Missio n s S U B S A T E L L I T E P O IN T GE OS T R & D o rb it Po la 35 800 Km M T S A T ( J a p a n ) 1 4 0 E Atm o sp h e ric C h e m istry Missio n s M S G ( E U M E T S A T ) 0 L o n g it u d e M E T E O S A T ( E U M E T S A T ) 6 3 E r o rb it G O M S ( R u ssia n F e d e r a tio n ) 76E F Y -2 ( C h in a ) 1 0 5 E Hyd ro lo g ic a l Missio n s N P O E S S ( U S A ) M e to p ( E U M E T S A T ) 22

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Leo coverage of poles every 100 minutes 26

Tracking Polar Atmospheric Motion from Leo Obs 27

Getting to Geostationary Orbit 28

Observations from geostationary orbit the weather moves - not the satellite Verner Suomi 29

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One minute imaging over Florida 31

32

SEVIRI sees dust storm over Africa 33

Five geos are providing global coverage for winds in tropics and mid-lats 34

Comparison of geostationary (geo) and low earth orbiting (leo) satellite capabilities Geo Leo observes process itself (motion and targets of opportunity) repeat coverage in minutes ( t 30 minutes) full earth disk only best viewing of tropics same viewing angle differing solar illumination observes effects of process repeat coverage twice daily ( t = 12 hours) global coverage best viewing of poles varying viewing angle same solar illumination visible, IR imager visible, IR imager (1, 4 km resolution) (1, 1 km resolution) one visible band multispectral in visible (veggie index) IR only sounder IR and microwave sounder (8 km resolution) (1, 17, 50 km resolution) filter radiometer diffraction more than leo filter radiometer, interferometer, and grating spectrometer diffraction less than geo 35

Space-Based component of the Global Observing System (GOS) 36

Leo Observations Terra was launched in 1999 and the EOS Era began MODIS, CERES, MOPITT, ASTER, and MISR reach polar orbit Aqua and ENVISAT followed in 2002 MODIS and MERIS to be followed by VIIRS AIRS and IASI to be followed by CrIS AMSU leading to ATMS 37

Launch of EOS-Terra (EOS-AM) Satellite - A New Era Begins Others include: MISR MOPITT CERES ASTER MODIS 110 MODIS instrument Specifications: Bands 1-2 (0.66,0.86 mm): 250 m Bands 3-7 (0.47, 0.55, 1.24, 1.64, 2.13 mm): 500 m Launch date: December 18, 1999, 1:57 PT Earth viewdoor open date: February 24, 2001 Bands 8-36: 1 km Allen Chu/NASA GSFC 38

Followed by the launch of EOS-Aqua (EOS-PM) Satellite Thermometer in the Sky AMSR-E AMSU HSB Launch date: May 4, 2002, 2:55 PDT Earth view door open date: June 25, 2002 MODIS AIRS CERES 39

Joint Polar System Welcome METOP Congratulations ESA / EUMETSAT IASI 40

Atmospheric Products: Examples Winds Total Water Vapor Temperature 500 mb Rain Rate Ozone Aerosol Optical Thickness 41

Land Surface Products: Examples Vegetation Health Quebec Fires/Smoke Snow Solar Radiation Global Lights/Fires 42

Ocean Products: Examples SST Anomalies Hot Spots: Potential Coral Bleaching TOPEX Sea Level QuikSCAT Winds Sea WIFS Ocean Color 43

* provides a regional view Remote Sensing Advantages * enables one to observe & measure the causes & effects of climate & environmental changes (both natural & human-induced) * provides repetitive geo-referenced looks at the same area * covers a broader portion of the spectrum than the human eye * can focus in on a very specific bandwidth in an image * can also look at a number of bandwidths simultaneously * operates in all seasons, at night, and in bad weather 44

Welcome to a Short Course in Remote Sensing 45

Brienza Short Course in Remote Sensing 18 24 Sep 2011 46