Title: Hyperspectral Imaging Systems
1Hyperspectral Imaging Systems Atmospheric
Effects
Dr. Richard B. Gomez, Instructor School of
Computational Sciences George Mason University
2Outline
- Atmospheric Structure
- Atmospheric Composition
- Solar/Earth Energy Distribution
- Atmospheric Radiative Transfer Theory
3Basic Forms of Electromagnetic Energy
- Electromagnetic energy exists in many forms
besides visible light (400 - 700 nm). Among
these are - Radio Waves gt100 m
- Microwaves 0.1
100 cm - Millimeter Waves 1 mm 0.1 cm
- Terahertz Frequencies 30 ?m 3 mm
- Thermal Infrared (Heat) 3 5
?m 8 14 ?m - Ultraviolet Rays 3
400 nm - X Rays
0.03 3 nm - Gamma Rays
lt 0.03 nm
4Radiometric Quantities
Quantity Radiant Energy (J) - Q Radiant Energy
Density (J/m3) U Radiant Flux (W) Power
P Radiant Exitance (W/m2) M Irradiance (W/m2)
E Radiance (W/m2-sr) L Radiant Intensity (W/sr)
- I
Definition ?Pdt dQ/dV dQ/dt dP/dA dP/dA d2P/dAd?
dP/d?
5Atmospheric Structure
CompositionNitrogen 78 Oxygen 21 Argon
nearly 1 Others HydrogenHelium, Neon, Carbon
Dioxide, etc.
The greatest error and uncertainty in deriving
reflectance factors usually comes from the
atmospheric modeling component.
6Image from the NASA Langley Research Center,
Atmospheric Sciences Division. http//asd-www.larc
.nasa.gov/erbe/ASDerbe.html
7Background Radiometry
Image courtesy of Digital Imaging and Remote
Sensing (DIRS) Laboratory
8Atmospheric Continuum
9Background SEBASS Sensor
10Background Thermal Spectrum
11What is a Photon?
- ?E h?
- ?E E2 E1 Energy of photon in joules (J).?
Frequency of the photon in hertz. h Planck's
constant 6.625 1034 joule-seconds - Wavelength ? c/? hc/?E
- A light wave that is emitted with a single
quantum of energy ?E h? is called a photon
12Photomultiplier
13Absorption of Light
14Molecular Spectra
15Space Reference System
16 Solid Angle
d? dS / r2 (in steradians, sr)
17Basic Components of Remote Sensing System
- Energy Source
- Transmission Path
- Target
- Background
- Sensor
18Hyperspectral Imaging General Concept
19Hyperspectral Reflectance Measurements
20Key Characteristics of Surface Reflectance
- Range of values of ?
- Spatial variability
- Degree of departure from Lambertian surface
- Surface polarization
- Water and vegetated surfaces have
non-Lambertianreflectance characteristics for
reasons due to specular reflection,
backscattering, shadows, backgrounds, or other
reasons
21Object Information Derived From Signal
22Atmospheric Effects (Richards Fig. 2.1)
23Spectral Windows
Photons falling between the spectral windows
highlighted above are severely attenuated (either
absorbed, scattered, or both) by the Earths
atmosphere.
24Upward Radiance Components
- L L1 L2 L3 L4
- L1 Path Radiance independent of surface
reflectance - L2 Attenuated Signal depends only on the
surface reflectance in the field of view.
Provides Surface information. - L3 Scattered by atmosphere to the surface and
reflected to the sensor. Affected by
non-Lambertian surface light. - L4 Light radiance reflected by the surface
with at least one scattering in the atmosphere
before reaching the sensor. Affectedby
nonuniform surface and by non-Lambertian surface
reflectionthat may be out of the field of view
of the sensor.
25Total Radiance Available to Sensor
- Total Irradiance EG at Earths Surface
- EG E??T?cos ? ?? ED (Path Irradiance
ED) - The Radiance LT Due to Global Irradiance EG of
the pixel - LT (R/?)E??T?cos ? ?? ED
- Total Radiance Available to Sensor
- LS (RT?/?)E??T?cos ? ?? ED LP
- See John Richards Book Page 42, Equation 2.4
26John Richards Equations
27John Richards Reflectance Calculation
28Atmospheric Compensation (continue)
29Luminescence
- Luminescence the emission of light by a
substance. It occurs when an electron returns to
the electronic ground state from an excited state
and loses it's excess energy as a
photonDifferent Types - Fluorescence
- Phosphorescence
- Chemiluminescence
- Bioluminescence
30Atmospheric Compensation
31Remote Sensing Electromagnetic Spectrum
Solar Radiance Back-Scattered from Earths Surface
VIS
Black Body Radiation of the earth (300K)
Energy
3u
10u
0.3u
1u
1 mm
500
a
0.4u
0.7u
VIS
MIR
FIR
MW
SWIR
100
NIR
Blocked
Transmission
500
50
100
5
1
10
500
20
300
5
3
10
2
1.0
0.5
1.5
0.3
0
b
(mm)
um
Wavelength
Human Eye
Photography
Radiometers Imaging Systems
Radars
Passive microwave Radiometers
Laser Sensors
32Atmospheric Transmission Characteristics
33Surface Emissions
34 Absorption Lines
When light from a luminous source passes through
a gas, the gas may extract certain specific
energies from the continuous spectrum. We then
see dark lines where the energy has been removed.
These dark lines are called absorption lines.
35Linewidth Full Width at Half Maximum
Airborne Hyperspectral Systems
36Solar/Earth Energy Distribution
37 Plancks Radiation Law
L? gives the energy per unit volume per unit
wavelength interval for blackbody radiation
38Kirchhoffs Law
- Absorptivity ? Emissivity ?
- A good Absorber is a good emitter of radiation
- This law generally holds for each spectral
component of the blackbody field and for each
direction of the incident radiation
39Stefan-Boltzmann Law
The total power per unit area radiated by a
blackbody is given by the Stefan-Boltzmann law.
? Stefan-Boltzmann constant.
40Beers Law
41Limitations of the Beer-Lambert law
- The linearity of the Beer-Lambert law is limited
by chemical and instrumental factors. These
include -
- absorptivity coefficients deviations at high
concentrations (gt0.01M) due to electrostatic
interactions between molecules in close proximity
- scattering of light due to particulates in the
path - fluorescence or phosphorescence of the sample
- changes in refractive index at high
concentrations - non-monochromatic radiation
- stray light
42Wien's Displacement Law
The wavelength at which a blackbody has its peak
emittance is given by Wien's Displacement
Law
43RTE for Plane-Parallel Atmospheres Model
44Instrument Response Accountability
45Source Function
46Solar Backscatter Radiance
Reflection characteristics of a surface are
provided by the bidirectional reflectance
distribution function (BRDF)
47Weighing Function
p atmospheric pressure? optical thickness
48EOSAEL