4.1 Radiometric and geometric corrections Flashcards
Remote sensing data pre-processing
• Remote sensing data are often radiometrically degraded
•Radiometric corrections
–Cosmetic corrections: Line dropouts, Line striping, Random noises
–Sun elevation
–Haze removal
–Atmospheric correction
Radiometric correction
Radiometric correction improve radiometrically degraded remote sensing
– Correcting for imperfections of the sensor
– Correcting for scene peculiarities and atmospheric disturbances
– Image enhancement
Radiometric calibration and correction
• There are visible errors and noises in the raw data that need to be corrected
[DN]
- Sensor dependent
- Re scaling factors often found in the metadata
[At sensor radiance]
- Requires additional information such as Solar zenith angle, Earth-sun distance, solar irradiance
- Often provided in the metadata
[TOA radiance and reflectancce]
• Requires knowledge of atmospheric conditions and aerosol properties at the time of image acquisition
[Surface reflectance]
Cosmetic corrections
• Correcting visible errors and noise in the image data.
– Missing lines: caused by failure of one of the detectors
– N Line striping: caused by the missing calibration of one of n detectors
– Random noise (spikes)
Missing lines
• Missing lines caused by failure of one of the detectors
– Random or periodic
• Defective lines are detected by comparing the average of each line with the scene average
• Defective lines are replaced with average of proceeding or exceeding lines.
N-Line striping
- The response of some detectors might drift with time. Therefore, every line may be brighter or darker than the other lines.
- Line striping is usually corrected using histogram matching or filters in Fourier domain.
• Histogram matching.
– Separate histograms corresponding to each detector.
– One detector response is taken as reference.
– Other responses are matched to the reference.
Spike noise
- Individual pixels with values much higher or lower than surrounding pixels.
- Caused by temporary disturbance or errors during data transmission.
- Identify spikes: each pixel is compared with its neighboring pixels.
- Pixels deviating more than a specific threshold from their neighbors are spikes.
- Spikes are replaced by interpolated values.
Sun elevation correction (1/2)
- Sun elevation changes depending on time of day and day of year.
- Solar irradiance varies with the seasonal changes in solar elevation angle and the distance between the Earth and sun.
- For comparison of images acquired at different time of day or different days of year, sun elevation correction is important.
- note:
- Irradiance that is received by the target is higher in summer compared to winter
- higher sun elevation gives better contrast
Sun elevation correction (2/2)
• Sun angle normalization DN' = DN/sin(a) where DN = raw pixel value DN' = Corrected pixel value a = sun elevation angle
• Sun elevation is usually provided in the metadata
• Relative sun angle correction
– Stable land cover is used as reference
– Radiometric values of the image with lower sun elevation are adjusted to the other image
Haze removal
• Haze correction removes sky radiance from the remote sensing data
– Sky radiance reduces image contrast.
– It has an additive effect, resulting in higher DN values (makes the image brighter but lower contrast).
– Sky radiance depends on wavelength.
– Haze removal is done for each band independently.
• Estimating the correction constant from the image
– When there is areas that should have zero reflectance (e.g. water in Infrared band)
– Smallest value in each band is taken as the correction constant
• From external information
– Additional information e.g. aerosol distribution and gas composition needed
Atmospheric correction -Relative atmospheric correction
– Based on ground reflectance – Approximate – Assume an empirical linear relationship between TOA and ground radiance. – Methods • Two reflectance measurements • Two reference surfaces
Atmospheric correction -Relative atmospheric correction
Method: Two reflectance measurements
Procedure
– The image is corrected based on field radiance measurements.
– The output is an absolute atmospherically corrected image.
• Some bright and dark targets, each covering a few pixels in the image, are selected.
• During the satellite pass, the reflectance of targets is measured in the field, using a reflector-meter device.
• Surface reflectance is measured using portable radiometers at spectrum bands similar to those of the sensor.
• A linear equation between TOA radiance and surface reflectance is built for each band.
• The linear equation is applied to each band to obtain corrected image
Atmospheric correction -Relative atmospheric correction
Method: Two reference surfaces (we want to compare the image from the same area but at a different time of atmospheric circumstances)
– The atmosphere of a reference image is imposed to another image.
– Relies on reflective invariant (the reflection of the target does not change through time) bright and dark areas in the image.
– Any difference in the reflectance of bright and dark areas are attributed to atmospheric conditions.
– The output is an image corrected relative to a reference image.
– Valid for comparing images.
Procedure
• At least one dark and one bright invariant areas in the image are selected (e.g. deep reservoir lakes, big asphalt areas, sandy beaches).
• The radiance difference between the areas in two images are calculated
• Based on the differences, a linear function is calculated.
• The linear function is applied to the second image.
Atmospheric correction -Absolute atmospheric correction
• Radiative transfer models
– Can be used for computing either radiances (intensities) or irradiances (fluxes) for a variety of atmospheric and surface
– Use detailed scattering models of atmosphere from physically based models.
– They need a full description of atmospheric components at fixed altitudes e.g. MODTRAN ® and 6S
– A variety of input parameters are required:
§ Geometric conditions (sun elevation and sensor altitude)
§ Atmospheric model for gaseous components (Rayleigh scattering) e.g. H2O and O3
§ Aerosol models (Mie Scattering) e.g. type and concentration of aerosols like dust, salt, etc
§ Spectral bands and bandwidth