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Above-water measurements of reflectance and chlorophyll-a algorithms in the Gulf of Lions, NW Mediterranean Sea

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Abstract

Above-water reflectance and surface chlorophyll a concentrations (Chl a) were measured in the Gulf of Lions, northwestern Mediterranean Sea in 2000 and 2001 in order to test Chl a inversion algorithms. Surface waters were separated in Case 2 waters in the Rhône River plume and proximal Region of Freshwater Influence (ROFI) stations, and Case 1 waters at all the other stations. Case 2 waters were characterized by R443/R555 < R443/R510 < R490/R555 < R490/R510 < 1. In the first part, we compared the concurrent reflectance measurements made with a scanning polarization radiometer (SIMBAD) and a hyperspectral Ocean Optics radiometer. The comparison of the remote-sensing reflectance (Rrs) values at SIMBAD wavelengths shows excellent agreement for Rrs values higher than 0.01 sr-1. Between the two instruments, reflectance ratios, commonly used in Chl a algorithms, show differences smaller than 2% in the Case 2 waters, and smaller than 20% in the Case 1 waters. In the second part, concurrent measurements of Chl a and of hyperspectral reflectance from 6 cruises were used to analyze the statistical performance of global (OC2, OC4) and regional regression algorithms using mainly SeaWiFS bands. The algorithms were tested first over the entire domain, then separately over the Case 1 and Case 2 waters. Chl a algorithms using band ratios such as the one presented in Bricaud et al. (2002) are suitable for the Case 1 waters. However, taking into account the large dispersion of Chl a for very close reflectance ratios in the Case 2 waters, single band ratios are not suitable for deriving Chl a. The use of a 4-wavelength parameter such as Xc, defined by Tassan (1994), leads to better results in the plume and proximal Rhône ROFI.

©2005 Optical Society of America

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Figures (12)

Fig. 1.
Fig. 1. Map of the Gulf of Lions with isobaths at 100, 1000, and 2000 m. The dotted line indicates the SARHYGOL trajectory. The optical stations are indicated by circles, with black or brown circles when both Ocean Optics and Simbad measurements were collected. Brown and yellow circles correspond to Case 2 waters. The dashed line indicates the approximate boundary between the proximal zone and the distal zone of the Rhône ROFI.
Fig. 2.
Fig. 2. Remote sensing reflectance spectra collected in the Gulf of Lions with the 8 Case 2 stations in red.
Fig. 3.
Fig. 3. Example of concurrent reflectance measurements using SIMBAD and Ocean Optics SD1000 radiometers (Gulf of Lions, 16th February 2001).
Fig. 4.
Fig. 4. SIMBAD and Ocean Optics concurrent remote sensing reflectance values at 3 visible wavelengths.
Fig. 5.
Fig. 5. Comparison of SIMBAD and Ocean Optics concurrent reflectance ratios.
Fig. 6.
Fig. 6. Comparison of Chl a estimates by SIMBAD and by Ocean Optics using the OC2v4 algorithm [11].
Fig. 7.
Fig. 7. Chl a estimates using the OC2v4 and OC4v4 algorithms vs. measured Chl a.
Fig. 8.
Fig. 8. Measured Chl a vs. reflectance ratios in the Gulf of Lions (N=32).
Fig. 9.
Fig. 9. Estimates vs. in situ Chl a by several algorithms on the complete Sarhygol dataset (distal+proximal ROFI).
Fig. 10.
Fig. 10. Estimated vs. in situ Chl a in the distal Rhône ROFI using several algorithms.
Fig. 11.
Fig. 11. Chl a vs. Xcmod in the proximal Rhône ROFI and regression relationship.
Fig. 12.
Fig. 12. Modeled Chl a vs. in situ Chl a in the proximal Rhône ROFI using two algorithms.

Tables (5)

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Table 1. Characteristics of the reflectance measurements performed during SARHYGOL cruises

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Table 2. Characteristics of the two types of waters considered in this study (24 “distal ROFI” or Case 1 waters, and 8 “proximal ROFI” or Case 2 waters).

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Table 3. Global and regional Chl a algorithms used in this study. Chl a is expressed in mg.m-3.

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Table 4. Statistical performance of chlorophyll-a algorithms applied to the SARHYGOL dataset (N=32). The parameters are obtained between modeled and measured Chl a.

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Table 5. Statistical performance of optimized Chl a algorithms at SeaWiFS bands for the SARHYGOL dataset (N=32). The parameters are obtained between modeled and measured Chl a.

Equations (18)

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E d ( λ ) = π R g ( λ ) L d ( λ )
R rs ( λ ) = L w ( λ ) E d ( λ ) = L u ( λ ) ρ L sky ( λ ) E d ( λ )
R rs ( 555 ) = 0.9898 R rs ( 560 ) + 0.1322
R rs ( 555 ) = 0.9845 R rs ( 565 ) + 0.2660
mean ( x ) = x ̅ = 1 n i = 1 n x i
stdev ( x ) = [ 1 n 1 i = 1 n ( x i x ̅ ) 2 ] 1 2
MNB = mean ( y a lg y obs y obs ) . 100
rms = stdev ( y a lg y obs y obs ) . 100
log _ bias = mean ( log ( y a lg y obs ) )
log _ rms = stdev ( log ( y a lg y obs ) )
X c = R 443 R 555 . [ R 412 R 490 ] + n
Chl a = 2.513 [ R 443 R 555 ] + 2.827
Chl a = 6.258 · exp ( 1.344 [ R 443 R 555 ] )
Chl a = 7.113 · exp ( 1.496 [ R 443 R 550 ] )
Chl a = 5.677 · exp ( 1.221 [ R 443 R 560 ] )
X c mod = X ca for 0.025 < Chl a < 1.1 mg . m 3
X c mod = X cb for 1.1 < Chl a < 40 mg . m 3
Chl a = 1.609 X c mod 2.457
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