The Use of Spectral and Angular Information In Remote Sensing

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Presentation transcript:

The Use of Spectral and Angular Information In Remote Sensing ARSET UTAH-DEQ Training Course April 22 – 25, 2013 ARSET-AQ - The NASA Applied Remote SEnsing Training Program Richard Kleidman Rob Levy Lorraine Remer SSAI/NASA Goddard SSAI/NASA Goddard UMBC

Reflectance Scattering Angle How spectral MODIS-Terra launched in 2001. Overall MODIS capabilities 36 spectral channels in one view direction. Data is used to create over 44 different geophysical products. How spectral information is used to create geophysical products is discussed in the presentation: Principles of Earth Remote Sensing – Spectra The seven primary channels used for aerosol retrieval are illustrated here. Many channels One direction Reflectance Scattering Angle

Spectral optical properties of aerosol The larger dust particles interact with the longer infrared wavelengths but not the smaller smoke particles which remain invisible. Both dust and smoke interact with the shorter wavelengths reflecting light back to the sensor. Dust Smoke This distinction is made possible by the wide spectral range of the MODIS sensor. from Y. Kaufman

Spectral optical properties of aerosol Here you can see the spectral response of the large and small particles. Dust / Sea Salt Smoke / Pollution wavelength in µm

Physical Properties Angstrom Exponent The Angstrom exponent is often used as a qualitative indicator of mean aerosol particle size Values greater than 2 - small particles Values less than 1 – large particles For measurements of optical thickness 1 and 2 taken at two different wavelengths 1 and 21

Physical Properties The angstrom exponent really represents the slope of the spectral response. For measurements of optical thickness 1 and 2 taken at two different wavelengths 1 and 2 wavelength in µm

Reflectance Scattering Angle MISR launched in 2001 Views in 9 different directions. Each view has 4 spectral channels. MISR Multi-directional measurements Reflectance Scattering Angle

Optical Properties Scattering Phase Function The directional light scattering due to the aerosol particles Backscatter Forward scatter Incoming Radiation

Optical Properties Scattering Phase Function – the amount of light scattered in each direction relative to the incoming direction.

flaming SMOKE smoldering Typical aerosols and their properties flaming SMOKE smoldering The phase function: relative angular distribution of scattered light heavily depends on the size and shape of aerosol particles

Optical Properties Sample Phase Functions

Introduction to the AERONET Sunphotometer Ground Based Network Richard Kleidman SSAI/NASA Goddard Lorraine Remer UMBC

PI: Brent Holben, NASA GSFC Intro to AERONET Aerosol Robotic Network http://aeronet.gsfc.nas.gov PI: Brent Holben, NASA GSFC

AERONET: The “ground” based satellite Several hundred sites around the globe

Two types of measurements Direct ‘sun’ Approx 4 per hour Measurements of direct solar extinction in ≥4  Assumes molecular and gas extinction. Derives spectral aerosol optical depth (AOD) --> relative aerosol size Derives H2O optical depth from 936 nm. Diffuse ‘sky’ Approx 1 per hour, + specific times Measurements of sky radiance in 4 (1020, 870, 670 and 440 nm) At discrete azimuth angles along sun’s ‘alumcantur’ (constant 0) At discrete zenith angles along sun’s ‘principle plane’ (constant 0) Uses RT (LUT) to invert spectral/angular radiance to retrieve aerosol size, shape and composition.

More about direct ‘sun’ Direct Sun Products: Spectral AOD () (accuracy:  = ±0.01 for L2) Angstrom Exponent () Total column water vapor (w) Statistics: Daily averages, monthly averages Fine and coarse AOD Fine and coarse fraction

AERONET Data Quality AERONET data is unique among sun photometer networks This is due to the consistent high quality calibration methodology applied to all of its instruments

AERONET Data Quality + Level 1.0 - unscreened data but may not have final calibration applied + Level 1.5 - cloud-screened data but may not have final calibration applied. These data are not quality assured. + Level 2.0 - pre- and post-field calibration applied, cloud-screened, and quality-assured data Next data release will have a near-real time level 2 product. If available: Level 2 is always preferred

Map of Aeronet Sites

Sites can be searched by: Location (clicking on the map) Data Level Dates of available data Length of data record

Aeronet Data Data Plots Yearly Monthly Select data level and format data type Select month or year Select day Available wavelengths for this instrument Number in brackets is average value for the time period Data Plots Yearly Monthly

Aeronet Data Data Plots Monthly Daily Select data level and format data type Select month or year Select day Available wavelengths for this instrument Number in brackets is average value for the time period Data Plots Monthly Daily

Reference Slides

Sunphotometry L = F0, exp[-m] Measurement of the sun direct beam Direct application of Beer-Bouguer-Lambert’s extinction law L = F0, exp[-m] where  is wavelength, m=m(0) is “air mass” (function of solar zenith angle, 0), L=L(0) is radiance, F0=F0(0) is solar irradiance and is total optical depth. Total optical depth is sum of contributions from molecular scattering, gas absorption, aerosol scatter/absorption, and cloud scattering/absorption. Depending on wavelength (), different assumptions can be made to neglect one or more of the contributing optical depths. Sunphotometer measurements date back to early 1900’s via pioneering work of Ångstrom.

Hundreds of Nearly Identical Sunphotometers (CE-318) Manufactured by Cimel Electronique (France) CE-318-1: Standard Model (with 1020, 870, 675, 440, 936, 340 and 380 nm filters) CE-318-2: Polar Model (with 1020, 870P1, 675, 440, 870P2, 870, 936, and 870P3 nm filters) CE-318-N (after 2004): Models with varying # of filters, wavelength ranges, polarization, etc. Robot mount for automatic sun tracking Includes satellite transmitter for remote deployment Owned by P.I. Operated and deployed by GSFC AERONET team Carefully calibrated at GSFC before and after field deployment. Products quality controlled at GSFC Primarily to retrieve aerosol properties, but also cloud properties, gas and H2O absorption. Originally, AERONET intended for “ground truth” for EOS.

More about diffuse ‘sky’ Measurement of spectral sky reflectance Plus assumptions of surface optical properties at site (MODIS surface albedo products) Results Size distribution in 22 size bins --> comparable aerosol lognormal properties (assuming two modes) Spectral absorption (and single scattering albedo, 0) Refractive Index (complex) Phase function (+ Assymetry Parameter) Fine and coarse aerosol AOD and fraction Percentage of spherical and spheroid particles High Accuracy requires some constraints large aerosol signal (e.g., > 0.4 at 0.44 m) large sun angle (Θ0 ≥ 50°) Minimum number of “symmetric” angles (homogenous sky) “Level 2” product is quality controlled Statistics (daily and monthly averages), Error bars