Title: Implementation of Vicarious Calibration for High Spatial Resolution Sensors
1Implementation of Vicarious Calibration for High
Spatial Resolution Sensors
- Stephen J. Schiller
- Raytheon Space and Airborne Systems El Segundo,
CA - Collaborators
- Dennis Helder- South Dakota State University
- Mary Pagnutti and Robert Ryan - Lockheed Martin
Space Operations, Stennis Space Center - Vicki Zanoni NASA Earth Scinece Applications
Directorate, Stennis Space Center
2Overview
- Calibration Considerations for Absolute
Radiometry - Vicarious Calibration and its application to
High Spatial Resolution Sensors - Design of Ground Targets and Ground Truth
Measurements - Top-of-Atmosphere Radiance Estimates Using
MODTRAN and Considering - BRDF Effects
- Adjacency Effect
- Aerosol Modeling
- Evaluating Model Radiance Accuracy
- Error Propagation Model
3Sensor Absolute Calibration
- Absolute Calibration establishes the link to
physical parameters and processes recorded in the
remote sensing image. - Multiple paths to SI units are necessary to
evaluate systematic errors in calibration
coefficients. - Vicarious calibration provides a known at-sensor
radiance independent of on-board calibration
sources - Goal of this presentation is to outline the
process for not just obtaining a gain estimate at
a single radiance level but to generate a
Vicarious Calibration Curve over the operational
dynamic range of the sensor
4Reflectance Based Vicarious Calibration
Methodology
- Measure surface/atmospheric optical properties at
the site containing one or more uniform targets - Constrain input parameters in a radiative
transfer model (MODTRAN 4) to match surface and
atmospheric conditions at the time of the sensor
overpass - Predict the top-of-atmosphere spectral radiance
for the ground target (hyperspectral resolution) - Extract target signal from sensor data for each
band - Integrate the at-sensor radiance spectrum with
the sensors relative spectral response for each
band - Calculate the gain and bias for each band
- Method provides an absolute calibration
established relative to the solar spectral
constant
5Ground-Based Vicarious Calibration of Sensor Gain
and Bias
Measure Target Reflectance
Solar Spectral Constant
Radiative Transfer Calculation of At-Sensor
Radiance (L)
Sensor Signal (S) of Ground Targets
Monitor Atmospheric Transmittance,
Diffuse/Global Ratio
S (dS/dL) L B Sensor Gain and Bias
6Traditional Approach to Vicarious Calibration of
Remote Sensing Systems
(Developed for Large Footprint Sensors Requiring
Natural Targets)
Typical approach has been to characterize a large
bright uniform target at a desert site to provide
a known top-of-atmosphere radiance
level. Provides a gain value based on a single
radiance level Uncertainty is estimated to be
/- 3 (RSS estimate of measurement and modeling
errors)
IKONOS Image of Lunar Lake, Nevada
7Improvement is to Generate a Calibration Curve
Over the Sensors Dynamic Range using Multiple
Sites IKONOS
White Sands
Six Deployments
Lunar Lake Playa
Railroad Valley Playa
Vegetation Cover (Brookings)
Deep Dense Vegetation or Water Bodies (zero
reflectance)
8Calibration Curve Generation From A Single Field
Campaign
(Using Man-made Targets)
Does the tight linear fit imply a better gain
estimate? Does the data resolve detector
non-linearity?
9No! Not Yet. More Data shows There are
Systematic Variations in Gain Estimates Between
Sites and Dates
- However, we now be seeing differences due to
- Stray light,
- Out of band leakage,
- Temperature variations of focal plane and readout
electronics, - Limitations of ground truth data and atmospheric
modeling.
10Enhanced application applied to high spatial
resolution sensors
- Generate a Vicarious Calibration Curve covering
the sensor dynamic range in a single image - Same atmospheric effects, scattered light levels,
adjacency effect, sensor responsivity conditions - Evaluates both gain and bias.
- Potential to evaluate non-linear responsivity.
- Potential to reduce cost compared to multiple
campaigns
11Enhanced Ground Target Design
- Lay out six to eight targets covering 0 to 85
reflectance - Targets include
- - Spectrally flat (gray toned targets for
calibration curve generation) - - Strong spectral contrast (evaluate effects of
spectral banding) - - Sample of surround spectrum (location where
image DN for each band is near the average of the
entire image) - Reflectance of each target is measured at the
site close to the time of the sensor overpass - Use a site that is similar to image sites
collected in operational use. (reproduce
scattered light and out-of-band leakage effects) - Ocean/coastal, vegetation, desert
12DN Histogram Of A Pre-Campaign Image Of The
Target Area Provides Data To Identify A Surround
Spectral Sample Location
Histogram of 11 km by 11 km IKONOS image of
Brookings
Arrow indicates DN value of the surround target
area
13Vicarious Calibration Curve Generation for Push
Broom Sensors 1
Detector Array
- Assumes a flat field image has been acquired for
relative calibration of all detector channels on
the focal plane (i.e. cloud, ice or desert scenes
, side slither image) - Relative gain for each channel is derived from
its response in terms of the average response of
all the channels
Uniform cloud or ground scene
Side slither image
14Vicarious Calibration Curve Generation for Push
Broom Sensors 2
- Next, apply the relative gain to the vicarious
calibration image - Raw signal (DNraw ) of calibration targets are
converted to relative signal (DNrel) and average
over the target area
- Weighted least-squares regression of TOA
Radiance, , vs relative signal
gives absolute gain, with respect
to average responsivity of focal plane,
- This relation defines the vicarious calibration
curve - Absolute gain of each channel, Gchan,band,,is
given by
TOA Radiance (Watts/m2-ster)
Slope
abs
15Achieving Accurate Top of Atmosphere Radiance
Estimates 1
- Radiative transfer model (MODTRAN) must account
for all major atmospheric effects
16Achieving Accurate Top Of Atmosphere Radiance
Estimates 2
- Requires extensive set of field data obtained
with well calibrated radiometers and reference
panels. - BRDF (Bi-directional Reflectance Distribution
Function) of calibration panels and targets - Atmospheric transmittance, upwelling radiance,
diffuse/global ratio, almucantor scans of sky
path radiance (if possible - hyperspectral
resolution) - Verticle profiles of water vapor and aerosols
(altitude of boundary layer) - radiosonde / lidar / aircraft based measurements
17Achieving Accurate Top Of Atmosphere Radiance
Estimates 3
- Requires MODTRAN parameters to be established via
user supplied inputs (using a default atmosphere
or surface reflectance is not adequate) - Target and surround reflectance spectrum
(hyperspectral resolution, user supplied BRDF) - Wavelength characterized aerosol extinction known
below and above the boundary layer (user supplied
from sun photometry) - Surface Range in the boundary layer (adjusted to
reproduce observed transmittance) - Aerosol scattering phase function ( adjust H-G
asymmetry factor or input user-supplied)
18Comments on MODTRAN Model Characterization
- BRDF Considerations
- Adjacency Effect
- Aerosol Vertical Profile
19BRDF Knowledge of calibration panel and ground
targets is essential
BRDF effects are reduced with higher
diffuse-to-global ratio
20Multi-angle images should be collected to verify
atmospheric and BRDF model
Tz7o
Tz19o
21Comments on MODTRAN Model Characterization
- BRDF Considerations
- Adjacency Effect
- Aerosol Vertical Profile
22Measuring Atmospheric Parameters To Characterize
The Adjacency Effect Is Critical
MODTRAN
Target spectrum surround spectrum
Modeling adjacency effect is required to
reproduce measured upwelling radiance off ground
targets
Grass spectrum used for surround
23Surround Spectrums Influence On Sky Path Radiance
Red edge of vegetation observed in the
downwelling sky path radiance
24Comments on MODTRAN Model Characterization
- BRDF Considerations
- Adjacency Effect
- Aerosol Vertical Profile
25Aircraft Measurements Of Extinction At The
Boundary Layer Improve Aerosol Model
Solar radiometer observations at the top of the
boundary layer (altitude defined in the MODTRAN
model) revealed a significantly higher
transmittance than available with MODTRAN model
atmospheres. The 1976 standard atmosphere was
scaled to fit the observations. Aerosol vertical
profile plays a significant role in modeling the
adjacency effect and extinction as a function of
wavelength (composition varies with height).
26Analysis Designed To Uses Multiple Paths to SI
Units for Accuracy Assessment
- MODTRAN parameterization achieved with input of
unitless quantities ties TOA radiance only to
solar spectral constant - Transmittance
- Reflectance
- Diffuse/global ration
- Assymetry factor
- Ground truth validation data from calibrated
radiometers is traceable to NIST standards - Upwelling radiance at surface
- Sky path radiance
- Direct comparison of MODTRAN predicted and
measured upwelling radiance and sky path radiance
evaluates systematic errors
27Comparison of MODTRAN and Measured Upwelling
Radiance Grass Target
28Comparison of MODTRAN and Measured Sky Path
Radiance
29TOA Error Propagation Model
- Apply error propation analysis to the following
radiative transfer equation from ground to
sensor. - is the upwelling target radiance at ground
level - is the transmittance along the path
between the target and the sensor - is the sky path radiance contribution as
seen from the sensor when viewing the target (the
signal produced if looking at a surface of zero
reflectance) - Each component is directly related to calibrated
ground measurements of which their uncertainty is
known based on the measurement errors of the
spectroradiometer and sunphotometer
30Error Propagation Equation Deriving the
Uncertainty in the TOA Radiance
- Ratio of air mass from ground to sun and sensor
- MODTRAN calculated transmittance to sun and
sensor - MODTRAN calculated upwelling radiance at the
ground - Measurement uncertainty in transmittance from
ground to sun - Measurement uncertainty in upwelling radiance
from target - Measurement uncertainty in in sky path radiance
from ground observation - Uncertainty in estimating aerosol extinction at
the MODTRAN input wavelengths from solar
radiometry. A is a fraction of the total
transmittance. - uncertainty in TOA sky path radiance using the
H-G scattering phase function characterized with
ground measurements. B is a fraction of the TOA
path radiance,
Described in Technique for estimating
uncertainties in top-of-Atmosphere radiances
derived by vicarious calibration, S.J. Schiller,
SPIE vol. 5151, 2003
31Conclusion
- Progress made in vicarious claibration techniques
for high spatial resolution sensors. - Natural targets to grey-toned deployed targets
- Single radiance levels at different sites dates
to multiple levels evaluated in a single campaign
event. - Goal is to generate a vicarious calibration curve
over the operational dynamic range of EO sensors
(Vis to SWIR) - Atmospheric model (i.e. MODTRAN) must be
characterized using user supplied parameters - Ground truth must address
- BRDF properties of targets
- Adjacency effect (knowledge of surround spectrum)
- Aerosol vertical profile
- Radiometric accuracy knowledge of ground truth
data for TOA radiance uncertainty estimates - Working toward lt3 absolute accuracy from
environments consistent with operational use