Although not discussed here, any evaluation of instrument calibration or processing algorithm changes is normally preceded by a re-evaluation of the vicarious calibration (Eplee, 2003). This effectively removes any bias on the mission-mean normalized water-leaving radiance retrievals at the MOBY vicarious calibration site. When comparing products from different sensors, any algorithm changes that are applicable to both sensors are applied equally, and both sensors are vicariously recalibrated at MOBY.
The plots and images shown in this document come from various processing and testing events. They are provided as examples only, and thus they do not reflect the current state of product quality. This document is intended to describe the analysis methods. The analysis results are posted elsewhere.
From these global, multi-day composites, a subset of the filled bins is selected and standard ocean products are averaged and trended with time. The analysis is focused on the trends in normalized water-leaving radiances (nLw), but trends in chlorophyll and atmospheric products are also evaluated. For bin selection and averaging, three global subsets are defined, corresponding to clear water, deep water, and coastal water. The deep water subset consists of all bins where water depth is greater than 1000 meters. Clear water is defined as deep water where the retrieved chlorophyll is less than 0.15 mg/m^3. Coastal water is defined as all bins where water depth is between 30 and 1000 meters, as defined by a shallow water mask and the deep water mask.
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A good example of this analysis is the SeaWiFS 5-year annual cycle for nLw shown above. In the absense of any major geophysical events, we expect the trend in global deep-water or global clear-water nLw to repeat from year to year. Low-level differences may be due to geographic sampling biases or real geophysical changes, but on the large-scale these plots tell us that SeaWiFS products are self-consistent over time (i.e., there is no long-term drift).
| Band | SeaWiFS | MODIS | OCTS |
| nLw 1 | 412 | 412 | 412 |
| nLw 2 | 443 | 443 | 443 |
| nLw 3 | 490 | 488 | 490 |
| nLw 4 | 510 | 531 | 520 |
| nLw 5 | 555 | 551 | 565 |
| nLw 6 | 670 | 667 & 678 | 670 |
| Chlor_a | OC4v4 | OC3M | OC4O |
| AOT | 865 | 870 | 865 |
| Epsilon | 765/865 | 750/870 | 765/865 |
With Level-3 composited data products in an equivalent form, the datasets are further reduced to a set of common bins. This means that only those bins for which a retrieval exists for both sensors are included in subsequent averaging and trending. This is critical to the statistics, as some sensors show systematic data gaps even after 8-days of compositing, and this can result in geographic sampling bias if both sensors are not equivalently masked.
Finally, with the products in common bin form, the data are divided into geographic subsets for averaging and trending. The subsets include the global deep, clear, and coastal-water subsets described in Section II, as well as a set of standard regions and a set of latitudinally distributed zones. When comparing the clear-water subsetted data, it should be noted that anomalously high chlorophyll retrievals from either sensor can significantly alter the geographic distribution of selected bins. In contrast, the deep-water and coastal subsets are purely geographic in selection criteria. The coastal subset, however, is more likely to contain regions of significant variability in water structure and atmospheric conditions, as well as case 2 water types, all of which can lead to greater retrieval uncertainty and larger differences between the two sensors. The deep-water subset is, therefore, the most stable subset for cross-sensor comparison of retrieved oceanic optical properties. The geographic extent of all three global subsets will vary, however, with the seasonal change in earth illumination and thus sensor imaging duty cycle.
retrievals Note that no effort is made to force the sensor retrievals to a common bandpass. Some level of difference is expected whan comparing the nLw retrievals between two sensors, particularly in the case where the nominal center wavelengths are not identical. A discussion of inherent differences between SeaWiFS and MODIS is available here. And a discussion of differences in the chlorophyll algorithms can be found here.
Figure 3 presents a sample pair of MODIS and SeaWiFS deep water subsetted chlorophyll images for one 8-day period in May of 2003, after mapping to the more familiar platte carre projection. The images show the geographic extent of the common-binned, deep-water subset, and they provide some insight into the qualitative agreement between the two sensors.
| SeaWiFS |
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MODIS |
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Log10(Chla), 0.01 - 1.0 mg/m^3 |
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The regional and zonal subsets are generally visible at all times of year. The regions were chosen for relative homogeneity (Fougnie, et al., 2002), and they are all in relatively clear water. A region is also included at Hawaii, to verify performance at the point of vicarious calibration (Eplee et al., 2003), where calibration biases should be minimal. The regions are described in Table 2 and shown graphically in Figure 4. The zonal subsets were added to provide a systematic means for investigating latitudinally-dependent differences between the two sensors. These are shown in Table 3 and Figure 5.
| Region ID |
Minimum Latitude |
Maximum Latitude |
Minimum Longitude |
Maximum Longitude |
| Hawaii | 18.0 | 19.9 | -158.5 | -156.5 |
| PacN | 15.0 | 23.0 | -180.0 | -159.4 |
| PacNW | 10.0 | 22.7 | 139.5 | 165.6 |
| PacSE | -44.9 | -20.7 | -130.2 | -89.0 |
| AtlN | 17.0 | 27.0 | -62.5 | -44.2 |
| AtlS | -19.9 | -9.9 | -32.3 | -11.0 |
| IndS | -29.9 | -21.2 | 89.5 | 100.1 |
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| Region ID |
Minimum Latitude |
Maximum Latitude |
Minimum Longitude |
Maximum Longitude |
| PacN50 | 40.0 | 50.0 | -170.0 | -150.0 |
| PacN40 | 30.0 | 40.0 | -170.0 | -150.0 |
| PacN30 | 20.0 | 30.0 | -170.0 | -150.0 |
| PacN20 | 10.0 | 20.0 | -170.0 | -150.0 |
| PacN10 | 0.0 | 10.0 | -170.0 | -150.0 |
| PacS10 | -10.0 | 0.0 | -170.0 | -150.0 |
| PacS20 | -20.0 | -10.0 | -170.0 | -150.0 |
| PacS30 | -30.0 | -20.0 | -170.0 | -150.0 |
| PacS40 | -40.0 | -30.0 | -170.0 | -150.0 |
| PacS50 | -50.0 | -40.0 | -170.0 | -150.0 |
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Taken alone, the comparitive temporal analysis can not be used to determine absolute error, since relative differences may be due to errors in either dataset or real geophysical effects which are not yet understood. However, when taken in concert with the self consistency analyses described in section II and the in situ comparisons of Section I, the sensor-to-sensor comparisons can serve to identify and isolate the likely cause for differences. An example of this is Figure 7, which shows results for the PacN50 zonal subset for two test cases. The plot on the left is before a correction was made to the MODIS/Aqua polarization sensitivity, while the plot on the right is after the correction.
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Campbell, J.W., J.M. Blaisdell, and M. Darzi, 1995: Level-3 SeaWiFS Data Products: Spatial and Temporal Binning Algorithms. NASA Tech. Memo. 104566, Vol. 32, S.B. Hooker, E.R. Firestone, and J.G. Acker, Eds., NASA Goddard Space Flight Center, Greenbelt, Maryland
Gordon, H.R. & M. Wang, "Retrieval of water-leaving radiance and aerosol optical thickness over the oceans with SeaWiFS: a preliminary algorithm," Appl. Opt., vol. 33, pp. 443-452, 1994
Eplee, R.E., Jr., R.A. Barnes, S.W. Bailey, and P.J. Werdell, 2003: "Changes to the vicarious calibration of SeaWiFS." In: Patt, F.S., R.A. Barnes, R.E. Eplee, Jr., B.A. Franz, W.D. Robinson, G.C. Feldman, S.W. Bailey, P.J. Werdell, R. Frouin, R.P. Stumpf, R.A. Arnone, R.W. Gould, Jr., P.M. Martinolich, and V. Ransibrahmanakul, Algorithm Updates for the Fourth SeaWiFS Data Reprocessing, NASA Tech. Memo. 2003--206892, Vol. 22, S.B. Hooker and E.R. Firestone, Eds., NASA Goddard Space Flight Center, Greenbelt, Maryland, (in press).
Fougnie, B., P. Henry, A. Morel, D. Antoine, and F. Montagner, 2002: Identification and Characterization of Stable Homogeneous Oceanic Zones: Climatology and Impact on In-Flight Calibration of Space Sensors over Rayleigh Scattering. Ocean Optics XVI, Santa Fe, NM, November 18-22, 2002.
Morel, A., D. Antoine, and B. Gentilli, 2002: Bidirectional reflectance of oceanic waters: accounting for Raman emission and varying particle scattering phase function. Appl. Opt., 41, 6289-6306
O'Reilly, J., S. Maritorena, M. O'Brien, D. Siegel, D. Toole, D. Menzies, R. Smith, J. Mueller, B. Mitchell, M. Kahru, F. CHavez, P. Strutton, G. Cota, S. Hooker, C. McClain, K. Carder, F. Muller-Karger, L. Harding, A. Magnuson, D. Phinney, G. Moore, J. Aiken, K. Arrigo, R. Letelier and M. Culver (2000). SeaWiFS postlaunch technical report series, Volume 11, SeaWiFS postlaunch calibration and validation analyses, Part 3, NASA Technical Memorandum.
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