Title: HSI Course
1Hyperspectral Imaging Basics Hyperspectral
Concepts Systems Tradeoffs
Dr. Richard B. Gomez, Instructor George Mason
University
2Outline
- Hyperspectral Concepts System Tradeoffs
- Signal-to-Noise Ratio (SNR)
- Spectral Resolution, Sampling Interval, Range
- Image Acquisition Mode Tradeoffs
- Data Collection Systems
- Classification of Hyperspectral Imaging Systems
- Ground, Airborne, Spaceborne
3Radiometric 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?
4Space Reference System
5Basic Components of Remote Sensing System
- Energy Source
- Transmission Path
- Target
- Background
- Sensor
6Hyperspectral Imaging General Concept
7Hyperspectral Reflectance Measurements
8AURORA Hyperspectral Image of Hawaii, Courtesy of
APTI, Inc.
9Hyperspectral Signatures
10Object Information Derived From Signal
11Atmospheric Effects (Richards Fig. 2.1)
12Atmospheric Compensation (continue)
13Incident Radiation
- Incident Radiation Reflected Radiation
- Scattered Radiation
- Absorbed Radiation
- Transmitted Radiation
14Upward 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.
15Total 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
16John Richards Equations
17John Richards Reflectance Calculation
18Basic System Capabilities
- Field-of-View (FOV) or Swath Width on the Ground
- Spectral Range
- Spectral Sampling Interval
- Spectral Resolution
- Spatial Resolution or Instantaneous FOV or
Ground Sample Distance (GSD) - Dynamic Range or Signal-to-Noise Ratio (SNR)
- Wavelength (Spectral) Calibration
- Radiometric Calibration
- Geometric Calibration
- Figure-of-Merit (indicator of overall system
performance)
19Mission Requirements
- Mass
- Power
- Data Rate
- Altitude
- Ground Coverage
- Timeliness
- Speed (Ground Velocity)
- Platform Stability (Pointing Ability)
- Orbit Characteristics (Inclination, Offset,
Type, etc.) - Costs
20System Parameters
- Mass
- Power
- Data Rate
- Encoding Level
- Spectral Discrimination
- Integration Time
- Detector Technology (Focal Plane Array, Format,
Pixel Size) - Pixel Pitch
- Focal Ratio or F-Number
- Focal Length
- Aperture
- Etendue
21Linewidth Full Width at Half Maximum
Airborne Hyperspectral Systems
22Classification of HSI Systems
- Image Acquisition Modes
- Whiskbroom Imagers
- Pushbroom Imagers
- Staring Imagers
- Spectral Selection Modes
- Dispersion Element (grating, prism)
- Filter-Based Systems
- Interference Filters
- Acoustical-Optical Filters
- Liquid Crystal Tunable Filters (LCTF)
- Interferometer-Based Systems
- Michelson Interferometer
- Fourier Transform Interferometer System
- Other (e.g., Multi-order etalons)
23Image Acquisition Mode Tradeoffs
24Spatial versus Spectral Resolution Tradeoffs
25Spatial versus Spectral Resolution Tradeoffs
26Principle Calibration Needs
- Geometric imaging aspects scan jitter,
platform motion - Relative geometric calibration FOV, IFOV, SSI
- Absolute geometric calibration GPS, INS, DTED
- Spectral (wavelength) spectral response of
each channel - Atomic emission line spectra spectral matching
- A-prior knowledge of sensor spectral
characteristics - Radiometric spectral radiance response
- Input radiance versus output digitized signal
- Dynamic range, quantization level, RMS noise
level
27Radiometric System Parameters
28 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.