Jeffrey H. Bowles, Wesley J. Moses, Gia M. Lamela, Richard Mied, Karen W. Patterson, and Ellen J. Wagner
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1 1 Jeffrey H. Bowles, Wesley J. Moses, Gia M. Lamela, Richard Mied, Karen W. Patterson, and Ellen J. Wagner and, Washington, D.C. from Center for Advanced Land Management Information Technologies (CALMIT), University of Nebraska-Lincoln, NE, USA. Southern Scientific Center of the Russian Academy of Sciences, Rostov-on-Don, Russia. Israel Oceanographic and Limnological Research, Kinneret Limnological Laboratory, Migdal, Israel 08 May 2014; HICO Users Meeting, Silver Spring, MD
2 2 Outline Bathymetry/Bottom Type Retrieval Surface Velocity Retrieval Chlorophyll-a Retrieval Sensor Noise Effects Challenges Conclusion
3 Bathymetry/ Bottom Type 3 Lee Stocking Island, the Bahamas HICO image acquired on 16 June 2010 Retrievals made using a LUT-based approach HICO RGB
4 Parameters: Phytoplankton Sediment CDOM Depth Bottom Rrs Calibrated At Sensor Radiance Lee Stocking Island, The Bahamas Coastal Waters Spectral Toolkit (CWST): Look-up Table Approach Input into Radiative Transfer Model Atmospheric Correction 3 Component Radiative Transfer Model (EcoLight) Remote Sensing Reflectance Spectrum (R RS ) Database Extract subset of parameters expected to be found in area [index, parameters, R RS spectra] Compare measured spectrum to selected spectra to find best match - takes time Metric is Euclidean Distance Phytoplankton Sediment CDOM, Depth Bottom Type Bottom Reflectance Sand Pigment Absorption Brown Mud Index Depth Bottom Pigment Chlorophyll Yellow Clay Seagrass Diatom Dinoflagellat Cyanobacteri Depth (m) > 20.0 Courtesy: Jeffrey Bowles, NRL 4
5 Bottom Type Retrieval 5 EL + LSI EL + LSI + 50:50 mixes EL + LSI + 50: :75 mixes Courtesy: Gia Lamela, NRL
6 Effect of Adding Mixed Bottom Types Euclidean Distance Statistics Min Max Mean StDev Points EL+LSI Bottoms ,012,000 EL+LSI+50:50 Bottoms ,012,000 EL+LSI+25:75 Bottoms ,012,000 6
7 Bottom Depth Retrieval 7 WITHOUT PROPER BOTTOMS WITH PROPER BOTTOM TYPES Depth (m) Acoustic Distance Along Transect CWST: Old Bottoms Depth (m) Acoustic Distance Along Transect CWST: New Bottoms Courtesy: Gia Lamela, NRL
8 8 Outline Bathymetry/Bottom Type Retrieval Surface Velocity Retrieval Chlorophyll-a Retrieval Sensor Noise Effects Challenges Conclusion
9 Surface Velocity from Global Optimal Solution (GOS) - Developed at NRL Tracks image features and requires only two images (e.g., May 5, 2007) Model Grid for GOS e.g., v = a+bx+cy+dxy Divides images into blocks & models velocity field in each block C Optimize velocity in all blocks to satisfy tracer conservation equation over image Yields dense, differentiable velocity field suitable for model initiation Uniquely adaptable to 2 or more tracers (e.g. IR & sediment) for improved accuracy 9
10 Surface Velocity from HICO 10 Images taken at 10:05:46 UTC and 11:41:13 UTC on March 22, 2011 Velocities determined using a three-tracer element (R 606, R 674, and R 720 )
11 11 Outline Bathymetry/Bottom Type Retrieval Surface Velocity Retrieval Chlorophyll-a Retrieval Sensor Noise Effects Challenges Conclusion
12 Chl-a Retrieval Test the potential of HICO as an operational tool for estimating chl-a concentration in coastal and estuarine waters 12 Previous studies (e.g., Moses et al. 2012) using MERIS data demonstrated the reliability of NIRred models for estimating chl-a concentration in productive coastal waters Current study using multi-temporal data collected after the demise of MERIS
13 Chl-a Retrieval Taganrog Bay (Russia) 13 UKRAINE Descending View RUSSIA Sea of Azov Taganrog Bay Ascending View HICO and in situ data acquired: July Sep in 2012 and Feb stations in 5 campaigns Units Min Max Median Mean mg m HICO data were atmospherically corrected using Tafkaa.
14 Two-Band NIR-red Model [ 1 ] R R Chl-a Chl-a Retrieval Three-Band NIR-red Model [( 1 1 ) ] R R R Chl-a (Gitelson 1992) (Dall Olmo and Gitelson 2005) Note: R 665 is the average of the reflectances at 662 nm and 668 nm Chl-a = (2-Band) Chl-a = (3-Band)
15 Comparison with MERIS 15 MERIS ( ) HICO ( ) Higher range of chl-a concentrations in the dataset Differences in the radiometric calibration and atmospheric correction Higher spatial and temporal variation in the dataset
16 Chl-a Maps 25 Aug Aug (a) (b) The chl-a estimates were quite accurate in spite of the high spatial and temporal variations of chl-a concentration in the bay (Moses et al. 2013) Changes in the chl-a concentration in the Taganrog Bay between 25 Aug and 27 Aug 2012.
17 Lake Kinneret (Israel) 11 March 2013 Phycoerythrin 0.02 Phycocyanin 17 Rrs (sr -1 ) Wavelength (nm) The presence of phycoerythrin and phycocyanin was confirmed by lab analysis of water samples MODIS R645
18 18 Outline Bathymetry/Bottom Type Retrieval Surface Velocity Retrieval Chlorophyll-a Retrieval Sensor Noise Effects Challenges Conclusion
19 Sensor Noise Effects Why Study? Inherent noise in the data affects everything retrieved from the data 19 The Signal-to-Noise Ratio (SNR) is often specified as a single number (maximum based on a standard target) Prescribed SNR different from effective SNR Characterize the effect of HICO s SNR on the retrieval of biophysical parameters in typical coastal water conditions
20 Noise Study - Approach Generate Rrs spectra using pre-defined biophysical parameters 20 Propagate the spectra through the atmosphere to generate at-sensor radiance Add noise to the at-sensor radiance Convert the noise-added at-sensor radiance to at-surface Rrs Retrieve parameters from noise-added Rrs and compare the results to the original parameters
21 Noise Study Approach Initial Parameters 21 HICO Noise Ecolight Comparison Noise-Added Reflectance Levenberg- Marquardt Minimization Simulated Reflectance 800 nm Adjusted )estimated parameters Parameters ( R( λ )noise R( λ ) λ= 400 nm 2 Final Estimated Parameters Yes Squared Difference Threshold? No
22 120 Noise Study - Results 22 Quasi-SNR Low CDOM High CDOM High TSS Medium TSS Low TSS Wavelength (μm) Estimation Error (%) a CDOM (440) = 0.1 m Chl-a (mg m -3 ) TSS = 1 g/m3 TSS = 4 g/m3 TSS = 8 g/m3 TSS = 14 g/m3 TSS = 20 g/m3 Estimation Error (%) a CDOM (440) = 2 m -1 TSS = 1 g/m3 TSS = 4 g/m3 TSS = 8 g/m3 TSS = 14 g/m3 TSS = 20 g/m Chl-a (mg m -3 ) (Moses et al. 2012)
23 Improving SNR by Sensor Design 23 SNR Nominal HICO Setting D = m f = m λ b = 600 nm Wavelength (μm) Note: D = diameter of the aperture; f = focal length; λ b = blaze wavelength Nominal HICO Setting: D = m; f = m; λ b = 400 nm. 26 Feb 2014; Ocean Sciences Meeting, Honolulu, HI
24 Improving SNR by Changing the Aperture Size 24 F -Stop = [ Focal length Diameter of the aperture]
25 SNR Impact on Retrievals 25 Improvement (%) [Error] = F-stop= 3.5 [Error] [Error] F-stop= 3.5 F-stop=
26 26 Outline Bathymetry/Bottom Type Retrieval Surface Velocity Retrieval Chlorophyll-a Retrieval Sensor Noise Effects Challenges Conclusion
27 Challenges Second order light in the near infrared wavelengths No on-board calibration; vicarious techniques adopted Post-launch spectral shifts shifts corrected for through continual comparison with concurrently acquired MODIS data Spectral etaloning more in the NIR region; data are smoothed with a Gaussian filter to minimize etaloning effects Corrections to HICO data described by Gao et al. (2012) A maximum of only 16 images per day (capacity being increased) Only intermittent temporal coverage; but the pointing capability of HICO helps 27
28 Unprecedented spatial and spectral detail from space Conclusion In spite of the challenges, HICO provides unprecedented spatial and spectral detail from space can be used to accurately retrieve biophysical parameters in coastal waters has potential as a reliable tool for monitoring 0.02 coastal water quality in select high-priority regions 0.01 Remember, Taganrog Bay, Russia HICO is a proof-of-concept mission, not designed to be an operational global ocean color monitoring tool. Rrs (sr -1 ) Phycoerythrin Wavelength (nm) Phycocyanin Chl-a 28
29 29 Contact:
30 References 30 Gao, B. -C., Li, R. -R, Lucke, R. L., Davis, C. O., Bevilacqua, R. M., Korwan, D. R., Montes, M. J., Bowles, J. H., and Corson, M. R. (2012). "Vicarious calibrations of HICO data acquired from the International Space Station", Applied Optics, 51(14): Lucke, R. L., Corson, M., McGlothlin, N. R., Butcher, S. D., Wood, D. L., Korwan, D. R., Li, R. R., Snyder, W. A., Davis, C. O., and Chen, D. T. (2011). Hyperspectral Imager for the Coastal Ocean: instrument description and first images, Applied Optics, 50(11): Moses, W. J., Bowles, J. H., Lucke, R. L., and Corson, M. R. (2011). Impact of signal-tonoise ratio in a hyperspectral sensor on the accuracy of biophysical parameter estimation in case II waters, Optics Express, 20(4): Moses, W. J., Gitelson, A. A., Berdnikov, S., Saprygin, V., and Povazhnyi, V. (2012). "Operational MERIS-based NIR-red algorithms for estimating chlorophyll-a concentrations in coastal waters The Azov Sea case study", Remote Sensing of Environment, 121: Moses, W. J., Gitelson, A. A., Berdnikov, S., Bowles, J. H., Povazhnyi, V., Saprygin, V., and Wagner, E. J. (2014). HICO-Based NIR-red Algorithms for Estimating Chlorophyll-a Concentration in Productive Coastal Waters, IEEE Geoscience and Remote Sensing Letters, 11(6):
31 Comparison with MERIS Results 31 Images acquired over the Taganrog Bay on 13 July (a) 120 (b) In Situ Chl-a (mg m -3 ) r 2 = 0.91 r 2 = 0.98 HICO-Based MERIS-Based In Situ Chl-a (mg m -3 ) HICO-Based MERIS-Based r 2 = 0.98 r 2 = Band NIR-red 3-Band NIR-red Difference in the slope of the regression is a function of, among other factors, the difference in the method used for atmospherically correcting the HICO and MERIS images.
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