Diffraction gratings. e.g., CDs and DVDs

Size: px
Start display at page:

Download "Diffraction gratings. e.g., CDs and DVDs"

Transcription

1 Diffraction gratings e.g., CDs and DVDs

2 Diffraction gratings Constructive interference where: sinθ = m*λ / d (If d > λ)

3 Single-slit diffraction 1.22 * λ / d

4

5 Grating, plus order-sorting filters on detector VNIR (Si) IR (HgCdTe) Murchie et al. (JGR, 2007)

6 Diffraction gratings: an example (compare to AVIRIS, most planetary reflectance spectrometers) 27 μm x 16.3 mm Murchie et al. (2007)

7 Putting It All Together: A Typical Flowchart for Remote Sensing Projects Data Collection Raw DN Sensor Calibration Radiance at sensor Atmospheric Correction Ground Radiance

8 Groun d Radian ce Division by solar irrad iance or blackbody at target temp Reflectance or emissvity Spectral "polishing" (optional, h yperspectral only) Refin ed reflectance or emissivity Multi- or hypersp ectral analysis Spectral/composition al map(s)

9 Selection of ground-truth locations Spectral/compositional map(s) (back to multior hyperspectral analysis F ield campaign F ield Observations GPS coordinates G round spectra Rectification, G eoreferencing, and Projection of scene Field Samples Refined Atmospheric Correction Lab analyses Final product (e.g., geologic map)

10 Atmospheric Effects For measurements of reflected sunlight (Vis/NIR): I sensor =!" RJ sun + RL atm _ down # $ (1 2τ atm )+ L atm _ up

11 Atmospheric Effects For measurements of self-emitted light (TIR): I sensor =!" εb surface + RL atm _ down # $ (1 τ atm )+ L atm _ up

12 Atmospheric Correction Model-based corrections: Goal is to remove effects of absorption, emission, and scattering of photons by the atmosphere For the geologic remote sensing analyst, typically involves use of one of several black boxes, e.g. MODTRAN or ATREM.

13 input ATREM input ATREM output

14 Want to model and remove effects of H 2 O, CO 2, O 3, N 2 O, CO, CH 4, O 2

15 DIScrete Ordinates Radiative Transfer (DISORT) McGuire et al. (2008)

16 Other types of atmospheric correction: IARR (Internal Average Relative Reflectance): Calculates the reflectance of every pixel in the scene relative to the average of all pixels in the scene averaged together. Works best when there are a wide variety of mineralogies in scene, but not great with vegetation. Useful when nothing is known about the scene e.g., no ground truth spectra, and no model-based atmospheric correction available. Will mute the spectral contrast of components present in a large fraction of the scene.

17 Other types of atmospheric correction: Empirical Line Calibration Employs spectra collected on the ground from known locations in the scene. By comparing pre-correction remote spectrum to ground spectrum from same location, correction values are derived for each wavelength. Works best when multiple locations used, especially if some have low overall reflectance and others have high overall reflectance. Similar in some ways to volcano scan technique used on Mars (divide by atmospheric spectrum derived from comparing summit and flank of dusty Olympus Mons)

18 Spectral Polishing Goal is to remove any residual atmospheric effects in the spectra EFFORT: Empirical Flat Field Optimized Reflectance Transformation: A purely mathematical technique no physics or geology used. Takes advantage of fact that residual atmospheric effects are usually narrow spectral features, whereas mineralogic features are usually somewhat wider. Fits n-degree polynomial model to spectra from all pixels. For each channel, calculate linear regression of correction factor between data and model. Average correction factors from all pixels

19

20 Continuous vs. Discrete Spectral Mapping Map that highlights a particular composition Map that attempts to classify every pixel in the scene

21 Band Ratios and Color

22

23 Band Ratio 2.10µm / 2.22 µm

24 2.10 µm 2.22 µm

25 2.10 µm 2.22 µm

26 Can go beyond simple band ratios to band depths Pelkey et al. (2007)

27 or even more complex band math Pelkey et al. (2007)

28 Which bands would you ratio?

29 Which bands would you ratio? ASTER

30 Distinguishing H 2 O ice from hydrous minerals BAD GOOD Horgan et al. (2009)

31 Color Composites from Continuous Images Hematite Kaolinite Dolomite Only three compositions can be displayed at once (R,G,B)

CRISM (Compact Reconnaissance Imaging Spectrometer for Mars) on MRO. Calibration Upgrade, version 2 to 3

CRISM (Compact Reconnaissance Imaging Spectrometer for Mars) on MRO. Calibration Upgrade, version 2 to 3 CRISM (Compact Reconnaissance Imaging Spectrometer for Mars) on MRO Calibration Upgrade, version 2 to 3 Dave Humm Applied Physics Laboratory, Laurel, MD 20723 18 March 2012 1 Calibration Overview 2 Simplified

More information

Introduction to Remote Sensing Wednesday, September 27, 2017

Introduction to Remote Sensing Wednesday, September 27, 2017 Lab 3 (200 points) Due October 11, 2017 Multispectral Analysis of MASTER HDF Data (ENVI Classic)* Classification Methods (ENVI Classic)* SAM and SID Classification (ENVI Classic) Decision Tree Classification

More information

Hyperspectral Remote Sensing

Hyperspectral Remote Sensing Hyperspectral Remote Sensing Multi-spectral: Several comparatively wide spectral bands Hyperspectral: Many (could be hundreds) very narrow spectral bands GEOG 4110/5100 30 AVIRIS: Airborne Visible/Infrared

More information

ENVI Classic Tutorial: Introduction to Hyperspectral Data 2

ENVI Classic Tutorial: Introduction to Hyperspectral Data 2 ENVI Classic Tutorial: Introduction to Hyperspectral Data Introduction to Hyperspectral Data 2 Files Used in this Tutorial 2 Background: Imaging Spectrometry 4 Introduction to Spectral Processing in ENVI

More information

CRISM Instrument, Mission, and Data Set Description

CRISM Instrument, Mission, and Data Set Description CRISM Instrument, Mission, and Data Set Description 22 March 2009 Scott L. Murchie and the CRISM team 1 Topics to be Discussed Instrument characteristics Hardware overview Data configuration and characteristics

More information

ENVI Tutorial: Vegetation Hyperspectral Analysis

ENVI Tutorial: Vegetation Hyperspectral Analysis ENVI Tutorial: Vegetation Hyperspectral Analysis Table of Contents OVERVIEW OF THIS TUTORIAL...1 HyMap Processing Flow...4 VEGETATION HYPERSPECTRAL ANALYSIS...4 Examine the Jasper Ridge HyMap Radiance

More information

Hyperspectral Processing II Adapted from ENVI Tutorials #14 & 15

Hyperspectral Processing II Adapted from ENVI Tutorials #14 & 15 CEE 615: Digital Image Processing Lab 14: Hyperspectral Processing II p. 1 Hyperspectral Processing II Adapted from ENVI Tutorials #14 & 15 In this lab we consider various types of spectral processing:

More information

ENVI Tutorial: Basic Hyperspectral Analysis

ENVI Tutorial: Basic Hyperspectral Analysis ENVI Tutorial: Basic Hyperspectral Analysis Table of Contents OVERVIEW OF THIS TUTORIAL...2 DEFINE ROIS...3 Load AVIRIS Data...3 Create and Restore ROIs...3 Extract Mean Spectra from ROIs...4 DISCRIMINATE

More information

SPACEFLIGHT HYPERION DATA RADIATION CALIBRATION PRELIMINARY STUDY

SPACEFLIGHT HYPERION DATA RADIATION CALIBRATION PRELIMINARY STUDY SPACEFLIGHT HYPERION DATA RADIATION CALIBRATION PRELIMINARY STUDY Shufang Tian a, Jianping Chen a, Ming Jiang a a CUGB, School of Geosciences and Resources,10083 Haidian District, Beijing, China-(sftian,3s,jming)@cugb.edu.cn

More information

Infrared Scene Simulation for Chemical Standoff Detection System Evaluation

Infrared Scene Simulation for Chemical Standoff Detection System Evaluation Infrared Scene Simulation for Chemical Standoff Detection System Evaluation Peter Mantica, Chris Lietzke, Jer Zimmermann ITT Industries, Advanced Engineering and Sciences Division Fort Wayne, Indiana Fran

More information

MRO CRISM TRR3 Hyperspectral Data Filtering

MRO CRISM TRR3 Hyperspectral Data Filtering MRO CRISM TRR3 Hyperspectral Data Filtering CRISM Data User's Workshop 03/18/12 F. Seelos, CRISM SOC CRISM PDS-Delivered VNIR TRR3 I/F 3-Panel Plot False Color RGB Composite Composite band distribution

More information

MODULE 3 LECTURE NOTES 3 ATMOSPHERIC CORRECTIONS

MODULE 3 LECTURE NOTES 3 ATMOSPHERIC CORRECTIONS MODULE 3 LECTURE NOTES 3 ATMOSPHERIC CORRECTIONS 1. Introduction The energy registered by the sensor will not be exactly equal to that emitted or reflected from the terrain surface due to radiometric and

More information

LAB EXERCISE NO. 02 DUE DATE: 9/22/2015 Total Points: 4 TOPIC: TOA REFLECTANCE COMPUTATION FROM LANDSAT IMAGES

LAB EXERCISE NO. 02 DUE DATE: 9/22/2015 Total Points: 4 TOPIC: TOA REFLECTANCE COMPUTATION FROM LANDSAT IMAGES LAB EXERCISE NO. 02 DUE DATE: 9/22/2015 Total Points: 4 TOPIC: TOA REFLECTANCE COMPUTATION FROM LANDSAT IMAGES You are asked to perform a radiometric conversion from raw digital numbers to reflectance

More information

TOA RADIANCE SIMULATOR FOR THE NEW HYPERSPECTRAL MISSIONS: STORE (SIMULATOR OF TOA RADIANCE)

TOA RADIANCE SIMULATOR FOR THE NEW HYPERSPECTRAL MISSIONS: STORE (SIMULATOR OF TOA RADIANCE) TOA RADIANCE SIMULATOR FOR THE NEW HYPERSPECTRAL MISSIONS: STORE (SIMULATOR OF TOA RADIANCE) Malvina Silvestri Istituto Nazionale di Geofisica e Vulcanologia In the frame of the Italian Space Agency (ASI)

More information

Correction and Calibration 2. Preprocessing

Correction and Calibration 2. Preprocessing Correction and Calibration Reading: Chapter 7, 8. 8.3 ECE/OPTI 53 Image Processing Lab for Remote Sensing Preprocessing Required for certain sensor characteristics and systematic defects Includes: noise

More information

Atmospheric correction of hyperspectral ocean color sensors: application to HICO

Atmospheric correction of hyperspectral ocean color sensors: application to HICO Atmospheric correction of hyperspectral ocean color sensors: application to HICO Amir Ibrahim NASA GSFC / USRA Bryan Franz, Zia Ahmad, Kirk knobelspiesse (NASA GSFC), and Bo-Cai Gao (NRL) Remote sensing

More information

REMOTE SENSING OF BENTHIC HABITATS IN SOUTHWESTERN PUERTO RICO

REMOTE SENSING OF BENTHIC HABITATS IN SOUTHWESTERN PUERTO RICO REMOTE SENSING OF BENTHIC HABITATS IN SOUTHWESTERN PUERTO RICO Fernando Gilbes Santaella Dep. of Geology Roy Armstrong Dep. of Marine Sciences University of Puerto Rico at Mayagüez fernando.gilbes@upr.edu

More information

ENVI Classic Tutorial: Multispectral Analysis of MASTER HDF Data 2

ENVI Classic Tutorial: Multispectral Analysis of MASTER HDF Data 2 ENVI Classic Tutorial: Multispectral Analysis of MASTER HDF Data Multispectral Analysis of MASTER HDF Data 2 Files Used in This Tutorial 2 Background 2 Shortwave Infrared (SWIR) Analysis 3 Opening the

More information

CRISM 2012 Data Users Workshop. MTRDR Data Analysis Walk-Through. K. Seelos, D. Buczkowski, F. Seelos, S. Murchie, and the CRISM SOC JHU/APL

CRISM 2012 Data Users Workshop. MTRDR Data Analysis Walk-Through. K. Seelos, D. Buczkowski, F. Seelos, S. Murchie, and the CRISM SOC JHU/APL CRISM 2012 Data Users Workshop MTRDR Data Analysis Walk-Through K. Seelos, D. Buczkowski, F. Seelos, S. Murchie, and the CRISM SOC JHU/APL 1 Goals Familiarize CRISM data users with the new MTRDR data set

More information

ENVI Classic Tutorial: Basic Hyperspectral Analysis

ENVI Classic Tutorial: Basic Hyperspectral Analysis ENVI Classic Tutorial: Basic Hyperspectral Analysis Basic Hyperspectral Analysis 2 Files Used in this Tutorial 2 Define ROIs 3 Load AVIRIS Data 3 Create and Restore ROIs 3 Extract Mean Spectra from ROIs

More information

Introduction: Experiment 1: Wave Properties of Light

Introduction: Experiment 1: Wave Properties of Light Natural Order Properties of Light Lab Introduction: In this lab we will explore the wave and particle nature of light. In the first experiment we will measure the diffraction pattern of light as it passes

More information

ENVI Tutorial: Geologic Hyperspectral Analysis

ENVI Tutorial: Geologic Hyperspectral Analysis ENVI Tutorial: Geologic Hyperspectral Analysis Table of Contents OVERVIEW OF THIS TUTORIAL...2 Objectives...2 s Used in This Tutorial...2 PROCESSING FLOW...3 GEOLOGIC HYPERSPECTRAL ANALYSIS...4 Overview

More information

Shallow-water Remote Sensing: Lecture 1: Overview

Shallow-water Remote Sensing: Lecture 1: Overview Shallow-water Remote Sensing: Lecture 1: Overview Curtis Mobley Vice President for Science and Senior Scientist Sequoia Scientific, Inc. Bellevue, WA 98005 curtis.mobley@sequoiasci.com IOCCG Course Villefranche-sur-Mer,

More information

GEOG 4110/5100 Advanced Remote Sensing Lecture 2

GEOG 4110/5100 Advanced Remote Sensing Lecture 2 GEOG 4110/5100 Advanced Remote Sensing Lecture 2 Data Quality Radiometric Distortion Radiometric Error Correction Relevant reading: Richards, sections 2.1 2.8; 2.10.1 2.10.3 Data Quality/Resolution Spatial

More information

Control of Light. Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 2007

Control of Light. Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 2007 Control of Light Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 007 Spectro-radiometry Spectral Considerations Chromatic dispersion

More information

Classify Multi-Spectral Data Classify Geologic Terrains on Venus Apply Multi-Variate Statistics

Classify Multi-Spectral Data Classify Geologic Terrains on Venus Apply Multi-Variate Statistics Classify Multi-Spectral Data Classify Geologic Terrains on Venus Apply Multi-Variate Statistics Operations What Do I Need? Classify Merge Combine Cross Scan Score Warp Respace Cover Subscene Rotate Translators

More information

Hyperspectral Imaging

Hyperspectral Imaging I N T R O Introduction to Introduction to Hyperspectral Imaging T O H Y P E R S P Hyperspectral Imaging with TNTmips page 1 Before Getting Started For much of the past decade, hyperspectral imaging has

More information

10/2/2012 Corporate Headquarters 9390 Gateway Dr, Ste 100 Reno, NV p: f:

10/2/2012 Corporate Headquarters 9390 Gateway Dr, Ste 100 Reno, NV p: f: SRS Project Report 1538 R.I.T. 10/2/2012 Corporate Headquarters 9390 Gateway Dr, Ste 100 Reno, NV 89521 p: 775.329.6660 f: 775.329.6668 Table of Contents 1 Overview 2 Acquisition Summary 3 4 2.1 Collection

More information

Chapter 24. Wave Optics

Chapter 24. Wave Optics Chapter 24 Wave Optics Diffraction Huygen s principle requires that the waves spread out after they pass through slits This spreading out of light from its initial line of travel is called diffraction

More information

Crop Types Classification By Hyperion Data And Unmixing Algorithm

Crop Types Classification By Hyperion Data And Unmixing Algorithm Crop Types Classification By Hyperion Data And Unmixing Algorithm H. FAHIMNEJAD 1, S.R. SOOFBAF 2, A. ALIMOHAMMADI 3, M. J. VALADAN ZOEJ 4 Geodesy and Geomatic Faculty, K.N.Toosi University of Technology,

More information

Spectral imagers for nanosatellites

Spectral imagers for nanosatellites VTT TECHNICAL RESEARCH CENTRE OF FINLAND LTD Spectral imagers for nanosatellites Finnish Satellite Workshop 2018 Antti Näsilä VTT Microspectrometers Fabry-Perot (FPI) technology for miniaturizing optical

More information

Potential of Sentinel-2 for retrieval of biophysical and biochemical vegetation parameters

Potential of Sentinel-2 for retrieval of biophysical and biochemical vegetation parameters Insert the title of your slide Potential of Sentinel-2 for retrieval of biophysical and biochemical vegetation parameters D. Scheffler, T. Kuester, K. Segl, D. Spengler and H. Kaufmann Motivation Insert

More information

A Survey of Modelling and Rendering of the Earth s Atmosphere

A Survey of Modelling and Rendering of the Earth s Atmosphere Spring Conference on Computer Graphics 00 A Survey of Modelling and Rendering of the Earth s Atmosphere Jaroslav Sloup Department of Computer Science and Engineering Czech Technical University in Prague

More information

Dr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD (301) (301) fax

Dr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD (301) (301) fax Dr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD 20723 (301) 953-6871 (301) 953-6670 fax Understand the instrument. Be able to convert measured counts/pixel on-orbit into

More information

A spectral climatology for atmospheric compensation

A spectral climatology for atmospheric compensation Approved for Public Release; Distribution Unlimited. 14-1557 A spectral climatology for atmospheric compensation John H. Powell* a and Ronald G. Resmini a a College of Science, George Mason University,

More information

ACORN, ATREM, ATCOR4, CAM5S, FLAASH

ACORN, ATREM, ATCOR4, CAM5S, FLAASH A comparison between six model-based methods to retrieve surface reflectance and water vapor content from hyperspectral data: A case study using synthetic AVIRIS data E. Ben-Dor *1, B.C. Kindel 2 and Patkin

More information

THE EFFECT OF TOPOGRAPHIC FACTOR IN ATMOSPHERIC CORRECTION FOR HYPERSPECTRAL DATA

THE EFFECT OF TOPOGRAPHIC FACTOR IN ATMOSPHERIC CORRECTION FOR HYPERSPECTRAL DATA THE EFFECT OF TOPOGRAPHIC FACTOR IN ATMOSPHERIC CORRECTION FOR HYPERSPECTRAL DATA Tzu-Min Hong 1, Kun-Jen Wu 2, Chi-Kuei Wang 3* 1 Graduate student, Department of Geomatics, National Cheng-Kung University

More information

Using Adjustable Slits to Reduce Interfering Element Effects

Using Adjustable Slits to Reduce Interfering Element Effects Prodigy ICP Technical Note Using Adjustable Slits to Reduce Interfering Element Effects INTRODUCTION The Inductively Coupled Plasma (ICP) is one of the most widely used emission sources for routine trace

More information

Aardobservatie en Data-analyse Image processing

Aardobservatie en Data-analyse Image processing Aardobservatie en Data-analyse Image processing 1 Image processing: Processing of digital images aiming at: - image correction (geometry, dropped lines, etc) - image calibration: DN into radiance or into

More information

SPICAM Archive Tutorial. Principal Investigator : J.L. Bertaux Archive Manager : A. Reberac

SPICAM Archive Tutorial. Principal Investigator : J.L. Bertaux Archive Manager : A. Reberac SPICAM Archive Tutorial Principal Investigator : J.L. Bertaux Archive Manager : A. Reberac 1 SPICAM Archive Tutorial SPICAM Instrument SPICAM data levels/products SPICAM Archive volume set organization

More information

DIMENSION REDUCTION FOR HYPERSPECTRAL DATA USING RANDOMIZED PCA AND LAPLACIAN EIGENMAPS

DIMENSION REDUCTION FOR HYPERSPECTRAL DATA USING RANDOMIZED PCA AND LAPLACIAN EIGENMAPS DIMENSION REDUCTION FOR HYPERSPECTRAL DATA USING RANDOMIZED PCA AND LAPLACIAN EIGENMAPS YIRAN LI APPLIED MATHEMATICS, STATISTICS AND SCIENTIFIC COMPUTING ADVISOR: DR. WOJTEK CZAJA, DR. JOHN BENEDETTO DEPARTMENT

More information

Lecture 39. Chapter 37 Diffraction

Lecture 39. Chapter 37 Diffraction Lecture 39 Chapter 37 Diffraction Interference Review Combining waves from small number of coherent sources double-slit experiment with slit width much smaller than wavelength of the light Diffraction

More information

INTELLIGENT TARGET DETECTION IN HYPERSPECTRAL IMAGERY

INTELLIGENT TARGET DETECTION IN HYPERSPECTRAL IMAGERY INTELLIGENT TARGET DETECTION IN HYPERSPECTRAL IMAGERY Ayanna Howard, Curtis Padgett, Kenneth Brown Jet Propulsion Laboratory, California Institute of Technology 4800 Oak Grove Drive, Pasadena, CA 91 109-8099

More information

doi: / See next page.

doi: / See next page. S.M. Adler-Golden, S. Richtsmeier, P. Conforti and L. Bernstein, Spectral Image Destriping using a Low-dimensional Model, Proc. Proc. SPIE 8743, Algorithms and Technologies for Multispectral, Hyperspectral,

More information

Comparison of Full-resolution S-NPP CrIS Radiance with Radiative Transfer Model

Comparison of Full-resolution S-NPP CrIS Radiance with Radiative Transfer Model Comparison of Full-resolution S-NPP CrIS Radiance with Radiative Transfer Model Xu Liu NASA Langley Research Center W. Wu, S. Kizer, H. Li, D. K. Zhou, and A. M. Larar Acknowledgements Yong Han NOAA STAR

More information

End-to-End Simulation of Sentinel-2 Data with Emphasis on Atmospheric Correction Methods

End-to-End Simulation of Sentinel-2 Data with Emphasis on Atmospheric Correction Methods End-to-End Simulation of Sentinel-2 Data with Emphasis on Atmospheric Correction Methods Luis Guanter 1, Karl Segl 2, Hermann Kaufmann 2 (1) Institute for Space Sciences, Freie Universität Berlin, Germany

More information

Locating the Shadow Regions in LiDAR Data: Results on the SHARE 2012 Dataset

Locating the Shadow Regions in LiDAR Data: Results on the SHARE 2012 Dataset Locating the Shadow Regions in LiDAR Data: Results on the SHARE 22 Dataset Mustafa BOYACI, Seniha Esen YUKSEL* Hacettepe University, Department of Electrical and Electronics Engineering Beytepe, Ankara,

More information

The Gain setting for Landsat 7 (High or Low Gain) depends on: Sensor Calibration - Application. the surface cover types of the earth and the sun angle

The Gain setting for Landsat 7 (High or Low Gain) depends on: Sensor Calibration - Application. the surface cover types of the earth and the sun angle Sensor Calibration - Application Station Identifier ASN Scene Center atitude 34.840 (34 3'0.64"N) Day Night DAY Scene Center ongitude 33.03270 (33 0'7.72"E) WRS Path WRS Row 76 036 Corner Upper eft atitude

More information

Working with M 3 Data. Jeff Nettles M 3 Data Tutorial at AGU December 13, 2010

Working with M 3 Data. Jeff Nettles M 3 Data Tutorial at AGU December 13, 2010 Working with M 3 Data Jeff Nettles M 3 Data Tutorial at AGU December 13, 2010 For Reference Slides and example data from today s workshop available at http://m3dataquest.jpl.nasa.gov See Green et al. (2010)

More information

Vicarious Radiometric Calibration of MOMS at La Crau Test Site and Intercalibration with SPOT

Vicarious Radiometric Calibration of MOMS at La Crau Test Site and Intercalibration with SPOT Vicarious Radiometric Calibration of MOMS at La Crau Test Site and Intercalibration with SPOT M. Schroeder, R. Müller, P. Reinartz German Aerospace Center, DLR Institute of Optoelectronics, Optical Remote

More information

HYPERSPECTRAL REMOTE SENSING

HYPERSPECTRAL REMOTE SENSING HYPERSPECTRAL REMOTE SENSING By Samuel Rosario Overview The Electromagnetic Spectrum Radiation Types MSI vs HIS Sensors Applications Image Analysis Software Feature Extraction Information Extraction 1

More information

Hydrocarbon Index an algorithm for hyperspectral detection of hydrocarbons

Hydrocarbon Index an algorithm for hyperspectral detection of hydrocarbons INT. J. REMOTE SENSING, 20 JUNE, 2004, VOL. 25, NO. 12, 2467 2473 Hydrocarbon Index an algorithm for hyperspectral detection of hydrocarbons F. KÜHN*, K. OPPERMANN and B. HÖRIG Federal Institute for Geosciences

More information

ENHANCEMENT OF DIFFUSERS BRDF ACCURACY

ENHANCEMENT OF DIFFUSERS BRDF ACCURACY ENHANCEMENT OF DIFFUSERS BRDF ACCURACY Grégory Bazalgette Courrèges-Lacoste (1), Hedser van Brug (1) and Gerard Otter (1) (1) TNO Science and Industry, Opto-Mechanical Instrumentation Space, P.O.Box 155,

More information

Atmospheric / Topographic Correction for Airborne Imagery. (ATCOR-4 User Guide, Version 7.0.3, March 2016)

Atmospheric / Topographic Correction for Airborne Imagery. (ATCOR-4 User Guide, Version 7.0.3, March 2016) Atmospheric / Topographic Correction for Airborne Imagery (ATCOR-4 User Guide, Version 7.0.3, March 2016) R. Richter 1 and D. Schläpfer 2 1 DLR - German Aerospace Center, D - 82234 Wessling, Germany 2

More information

Optics Vac Work MT 2008

Optics Vac Work MT 2008 Optics Vac Work MT 2008 1. Explain what is meant by the Fraunhofer condition for diffraction. [4] An aperture lies in the plane z = 0 and has amplitude transmission function T(y) independent of x. It is

More information

Chemistry Instrumental Analysis Lecture 6. Chem 4631

Chemistry Instrumental Analysis Lecture 6. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 6 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device

More information

Determining satellite rotation rates for unresolved targets using temporal variations in spectral signatures

Determining satellite rotation rates for unresolved targets using temporal variations in spectral signatures Determining satellite rotation rates for unresolved targets using temporal variations in spectral signatures Joseph Coughlin Stinger Ghaffarian Technologies Colorado Springs, CO joe.coughlin@sgt-inc.com

More information

Light and Electromagnetic Waves. Honors Physics

Light and Electromagnetic Waves. Honors Physics Light and Electromagnetic Waves Honors Physics Electromagnetic Waves EM waves are a result of accelerated charges and disturbances in electric and magnetic fields (Radio wave example here) As electrons

More information

Lecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization

Lecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization Lecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization Lens Aberrations - 3 lectures Spherical aberrations Coma,

More information

MODTRAN4 RADIATIVE TRANSFER MODELING FOR ATMOSPHERIC CORRECTION. Spectral Sciences, Inc., Burlington, MA 01803

MODTRAN4 RADIATIVE TRANSFER MODELING FOR ATMOSPHERIC CORRECTION. Spectral Sciences, Inc., Burlington, MA 01803 MODTRAN4 RADIATIVE TRANSFER MODELING FOR ATMOSPHERIC CORRECTION A. Berk a, G. P. Anderson b, L. S. Bernstein a, P. K. Acharya a, H. Dothe a, M. W. Matthew a, S. M. Adler-Golden a, J. H. Chetwynd, Jr. b,

More information

IMAGING SPECTROMETER DATA CORRECTION

IMAGING SPECTROMETER DATA CORRECTION S E S 2 0 0 5 Scientific Conference SPACE, ECOLOGY, SAFETY with International Participation 10 13 June 2005, Varna, Bulgaria IMAGING SPECTROMETER DATA CORRECTION Valentin Atanassov, Georgi Jelev, Lubomira

More information

Radiometric Correction. Lecture 4 February 5, 2008

Radiometric Correction. Lecture 4 February 5, 2008 Radiometric Correction Lecture 4 February 5, 2008 Procedures of image processing Preprocessing Radiometric correction is concerned with improving the accuracy of surface spectral reflectance, emittance,

More information

Interference & Diffraction

Interference & Diffraction Electromagnetism & Light Interference & Diffraction https://youtu.be/iuv6hy6zsd0?t=2m17s Your opinion is very important to us. What study material would you recommend for future classes of Phys140/141?

More information

Spectroscopy techniques II. Danny Steeghs

Spectroscopy techniques II. Danny Steeghs Spectroscopy techniques II Danny Steeghs Conducting long-slit spectroscopy Science goals must come first, what are the resolution and S/N requirements? Is there a restriction on exposure time? Decide on

More information

Testing Hyperspectral Remote Sensing Monitoring Techniques for Geological CO 2 Storage at Natural Seeps

Testing Hyperspectral Remote Sensing Monitoring Techniques for Geological CO 2 Storage at Natural Seeps Testing Hyperspectral Remote Sensing Monitoring Techniques for Geological CO 2 Storage at Natural Seeps Luke Bateson Clare Fleming Jonathan Pearce British Geological Survey In what ways can EO help with

More information

Retrieval of Surface Reflectance and LAI Mapping with Data from ALI, Hyperion and AVIRIS

Retrieval of Surface Reflectance and LAI Mapping with Data from ALI, Hyperion and AVIRIS Retrieval of Surface Reflectance and LAI Mapping with Data from ALI, Hyperion and AVIRIS P. Gong 1, G. Biging 1, R. Pu 1, and M. R. Larrieu 2 1 Center for Assessment and Monitoring of Forest and Environmental

More information

Atmospheric inversion in the presence of clouds: an adaptive ELM approach.

Atmospheric inversion in the presence of clouds: an adaptive ELM approach. Atmospheric inversion in the presence of clouds: an adaptive ELM approach. Brent Bartlett and John R. Schott Rochester Institute of Technology, Rochester, NY, USA ABSTRACT Many algorithms exist to invert

More information

LECTURE 14 PHASORS & GRATINGS. Instructor: Kazumi Tolich

LECTURE 14 PHASORS & GRATINGS. Instructor: Kazumi Tolich LECTURE 14 PHASORS & GRATINGS Instructor: Kazumi Tolich Lecture 14 2 Reading chapter 33-5 & 33-8 Phasors n Addition of two harmonic waves n Interference pattern from multiple sources n Single slit diffraction

More information

Update on Pre-Cursor Calibration Analysis of Sentinel 2. Dennis Helder Nischal Mishra Larry Leigh Dave Aaron

Update on Pre-Cursor Calibration Analysis of Sentinel 2. Dennis Helder Nischal Mishra Larry Leigh Dave Aaron Update on Pre-Cursor Calibration Analysis of Sentinel 2 Dennis Helder Nischal Mishra Larry Leigh Dave Aaron Background The value of Sentinel-2 data, to the Landsat world, will be entirely dependent on

More information

Spectrographs. C. A. Griffith, Class Notes, PTYS 521, 2016 Not for distribution.

Spectrographs. C. A. Griffith, Class Notes, PTYS 521, 2016 Not for distribution. Spectrographs C A Griffith, Class Notes, PTYS 521, 2016 Not for distribution 1 Spectrographs and their characteristics A spectrograph is an instrument that disperses light into a frequency spectrum, which

More information

Quality assessment of RS data. Remote Sensing (GRS-20306)

Quality assessment of RS data. Remote Sensing (GRS-20306) Quality assessment of RS data Remote Sensing (GRS-20306) Quality assessment General definition for quality assessment (Wikipedia) includes evaluation, grading and measurement process to assess design,

More information

Applications of passive remote sensing using emission: Remote sensing of sea surface temperature (SST)

Applications of passive remote sensing using emission: Remote sensing of sea surface temperature (SST) Lecture 5 Applications of passive remote sensing using emission: Remote sensing of sea face temperature SS Objectives:. SS retrievals from passive infrared remote sensing.. Microwave vs. R SS retrievals.

More information

A Fast Smoothing Algorithm for Post-Processing of Surface Reflectance Spectra Retrieved from Airborne Imaging Spectrometer Data

A Fast Smoothing Algorithm for Post-Processing of Surface Reflectance Spectra Retrieved from Airborne Imaging Spectrometer Data Sensors 2013, 13, 13879-13891; doi:10.3390/s131013879 Article OPEN ACCESS sensors ISSN 1424-8220 www.mdpi.com/journal/sensors A Fast Smoothing Algorithm for Post-Processing of Surface Reflectance Spectra

More information

GENESIS Generator of Spectral Image Simulations

GENESIS Generator of Spectral Image Simulations MBT Space Division - GENESIS Generator of Spectral Image Simulations Dr. Yael Efraim, Dr. N. Cohen, Dr. G. Tidhar, Dr. T. Feingersh Dec 2017 1 Scope GENESIS: End-to-end simulation of hyper-spectral (HS)

More information

Linking sun-induced fluorescence and photosynthesis in a forest ecosystem

Linking sun-induced fluorescence and photosynthesis in a forest ecosystem Linking sun-induced fluorescence and photosynthesis in a forest ecosystem COST ES1309 Tagliabue G, Panigada C, Dechant B, Celesti M, Cogliati S, Colombo R, Julitta T, Meroni M, Schickling A, Schuettemeyer

More information

No Brain Too Small PHYSICS

No Brain Too Small PHYSICS Level 3 Physics: Demonstrate understanding of Waves Waves Behaviour - Answers In 03, AS 953 replaced AS 9050. The Mess that is NCEA Assessment Schedules. In AS 9050 there was an Evidence column with the

More information

(0, 1, 1) (0, 1, 1) (0, 1, 0) What is light? What is color? Terminology

(0, 1, 1) (0, 1, 1) (0, 1, 0) What is light? What is color? Terminology lecture 23 (0, 1, 1) (0, 0, 0) (0, 0, 1) (0, 1, 1) (1, 1, 1) (1, 1, 0) (0, 1, 0) hue - which ''? saturation - how pure? luminance (value) - intensity What is light? What is? Light consists of electromagnetic

More information

Lecture 7. Spectral Unmixing. Summary. Mixtures in Remote Sensing

Lecture 7. Spectral Unmixing. Summary. Mixtures in Remote Sensing Lecture 7 Spectral Unmixing Summary This lecture will introduce you to the concepts of linear spectral mixing. This methods is sometimes also called: Spectral Mixture Analysis (SMA: Wessman et al 1997)

More information

Data products. Dario Fadda (USRA) Pipeline team Bill Vacca Melanie Clarke Dario Fadda

Data products. Dario Fadda (USRA) Pipeline team Bill Vacca Melanie Clarke Dario Fadda Data products Dario Fadda (USRA) Pipeline team Bill Vacca Melanie Clarke Dario Fadda Pipeline (levels 1 à 2) The pipeline consists in a sequence of modules. For each module, files are created and read

More information

False Color to NDVI Conversion Precision NDVI Single Sensor

False Color to NDVI Conversion Precision NDVI Single Sensor False Color to NDVI Conversion Precision NDVI Single Sensor Contents 1 Sensor Properties... 2 2 Isolating Bands... 2 3 Calculating NDVI from Original Image Pixel DN... 3 4 Calculating NDVI from AgVault

More information

Motivation. Aerosol Retrieval Over Urban Areas with High Resolution Hyperspectral Sensors

Motivation. Aerosol Retrieval Over Urban Areas with High Resolution Hyperspectral Sensors Motivation Aerosol etrieval Over Urban Areas with High esolution Hyperspectral Sensors Barry Gross (CCNY) Oluwatosin Ogunwuyi (Ugrad CCNY) Brian Cairns (NASA-GISS) Istvan Laszlo (NOAA-NESDIS) Aerosols

More information

ATMOSPHERIC CORRECTION ITERATIVE METHOD FOR HIGH RESOLUTION AEROSPACE IMAGING SPECTROMETERS

ATMOSPHERIC CORRECTION ITERATIVE METHOD FOR HIGH RESOLUTION AEROSPACE IMAGING SPECTROMETERS ATMOSPHERIC CORRECTION ITERATIVE METHOD FOR HIGH RESOLUTION AEROSPACE IMAGING SPECTROMETERS Alessandro Barducci, Donatella Guzzi, Paolo Marcoionni, Ivan Pippi * CNR IFAC Via Madonna del Piano 10, 50019

More information

Interactive comment on Quantification and mitigation of the impact of scene inhomogeneity on Sentinel-4 UVN UV-VIS retrievals by S. Noël et al.

Interactive comment on Quantification and mitigation of the impact of scene inhomogeneity on Sentinel-4 UVN UV-VIS retrievals by S. Noël et al. Atmos. Meas. Tech. Discuss., www.atmos-meas-tech-discuss.net/5/c741/2012/ Author(s) 2012. This work is distributed under the Creative Commons Attribute 3.0 License. Atmospheric Measurement Techniques Discussions

More information

Interactive comment on Quantification and mitigation of the impact of scene inhomogeneity on Sentinel-4 UVN UV-VIS retrievals by S. Noël et al.

Interactive comment on Quantification and mitigation of the impact of scene inhomogeneity on Sentinel-4 UVN UV-VIS retrievals by S. Noël et al. Atmos. Meas. Tech. Discuss., 5, C741 C750, 2012 www.atmos-meas-tech-discuss.net/5/c741/2012/ Author(s) 2012. This work is distributed under the Creative Commons Attribute 3.0 License. Atmospheric Measurement

More information

Airborne Hyperspectral Imaging Using the CASI1500

Airborne Hyperspectral Imaging Using the CASI1500 Airborne Hyperspectral Imaging Using the CASI1500 AGRISAR/EAGLE 2006, ITRES Research CASI 1500 overview A class leading VNIR sensor with extremely sharp optics. 380 to 1050nm range 288 spectral bands ~1500

More information

Full Optical Spectrum Hyperspectral Scene Simulation

Full Optical Spectrum Hyperspectral Scene Simulation Full Optical Spectrum Hyperspectral Scene Simulation Robert L. Sundberg and Steven Richtsmeier Spectral Sciences, Inc. 4 Fourth Avenue Burlington, MA 01803 Abstract-Full optical spectrum (UV to LWIR) hyperspectral

More information

Michelson Interferometer

Michelson Interferometer Michelson Interferometer The Michelson interferometer uses the interference of two reflected waves The third, beamsplitting, mirror is partially reflecting ( half silvered, except it s a thin Aluminum

More information

Chapter 4 - Diffraction

Chapter 4 - Diffraction Diffraction is the phenomenon that occurs when a wave interacts with an obstacle. David J. Starling Penn State Hazleton PHYS 214 When a wave interacts with an obstacle, the waves spread out and interfere.

More information

GODDARD SPACE FLIGHT CENTER. Future of cal/val. K. Thome NASA/GSFC

GODDARD SPACE FLIGHT CENTER. Future of cal/val. K. Thome NASA/GSFC GODDARD SPACE FLIGHT CENTER Future of cal/val K. Thome NASA/GSFC Key issues for cal/val Importance of cal/val continues to increase as models improve and budget pressures go up Better cal/val approaches

More information

Throughput of an Optical Instrument II: Physical measurements, Source, Optics. Q4- Number of 500 nm photons per second generated at source

Throughput of an Optical Instrument II: Physical measurements, Source, Optics. Q4- Number of 500 nm photons per second generated at source Throughput of an Optical Instrument II: Physical measurements, Source, Optics Question- Value Q1- Percent output between 450-550 nm by mass Answer (w/ units) Q2- Energy in J of a 500 nm photon Q3- Flux

More information

Calculation steps 1) Locate the exercise data in your PC C:\...\Data

Calculation steps 1) Locate the exercise data in your PC C:\...\Data Calculation steps 1) Locate the exercise data in your PC (freely available from the U.S. Geological Survey: http://earthexplorer.usgs.gov/). C:\...\Data The data consists of two folders, one for Athens

More information

MET 4410 Remote Sensing: Radar and Satellite Meteorology MET 5412 Remote Sensing in Meteorology. Lecture 9: Reflection and Refraction (Petty Ch4)

MET 4410 Remote Sensing: Radar and Satellite Meteorology MET 5412 Remote Sensing in Meteorology. Lecture 9: Reflection and Refraction (Petty Ch4) MET 4410 Remote Sensing: Radar and Satellite Meteorology MET 5412 Remote Sensing in Meteorology Lecture 9: Reflection and Refraction (Petty Ch4) When to use the laws of reflection and refraction? EM waves

More information

Monte Carlo Ray Tracing Based Non-Linear Mixture Model of Mixed Pixels in Earth Observation Satellite Imagery Data

Monte Carlo Ray Tracing Based Non-Linear Mixture Model of Mixed Pixels in Earth Observation Satellite Imagery Data Monte Carlo Ray Tracing Based Non-Linear Mixture Model of Mixed Pixels in Earth Observation Satellite Imagery Data Verification of non-linear mixed pixel model with real remote sensing satellite images

More information

CRISM File Naming Convention Secret Decoder Ring

CRISM File Naming Convention Secret Decoder Ring CRISM File Naming Convention Secret Decoder Ring Observing Mode Unique Target ID Segment ID Data Type Macro ID or Browse Product Detector Product Type and Version Number Extension Observing Mode 3-letter

More information

Chapter 24 - The Wave Nature of Light

Chapter 24 - The Wave Nature of Light Chapter 24 - The Wave Nature of Light Summary Four Consequences of the Wave nature of Light: Diffraction Dispersion Interference Polarization Huygens principle: every point on a wavefront is a source of

More information

UAV-based Remote Sensing Payload Comprehensive Validation System

UAV-based Remote Sensing Payload Comprehensive Validation System 36th CEOS Working Group on Calibration and Validation Plenary May 13-17, 2013 at Shanghai, China UAV-based Remote Sensing Payload Comprehensive Validation System Chuan-rong LI Project PI www.aoe.cas.cn

More information

EECE5646 Second Exam. with Solutions

EECE5646 Second Exam. with Solutions EECE5646 Second Exam with Solutions Prof. Charles A. DiMarzio Department of Electrical and Computer Engineering Northeastern University Fall Semester 2012 6 December 2012 1 Lyot Filter Here we consider

More information

DEEP LEARNING TO DIVERSIFY BELIEF NETWORKS FOR REMOTE SENSING IMAGE CLASSIFICATION

DEEP LEARNING TO DIVERSIFY BELIEF NETWORKS FOR REMOTE SENSING IMAGE CLASSIFICATION DEEP LEARNING TO DIVERSIFY BELIEF NETWORKS FOR REMOTE SENSING IMAGE CLASSIFICATION S.Dhanalakshmi #1 #PG Scholar, Department of Computer Science, Dr.Sivanthi Aditanar college of Engineering, Tiruchendur

More information

Chapter 25. Wave Optics

Chapter 25. Wave Optics Chapter 25 Wave Optics Interference Light waves interfere with each other much like mechanical waves do All interference associated with light waves arises when the electromagnetic fields that constitute

More information

Overview of the EnMAP Imaging Spectroscopy Mission

Overview of the EnMAP Imaging Spectroscopy Mission Overview of the EnMAP Imaging Spectroscopy Mission L. Guanter, H. Kaufmann, K. Segl, S. Foerster, T. Storch, A. Mueller, U. Heiden, M. Bachmann, G. Rossner, C. Chlebek, S. Fischer, B. Sang, the EnMAP Science

More information