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WHAT IS COLLECTED?

The 3 subsections below briefly summarize the set of measurements that are performed offshore either from the ship or from the buoy, and at the coastal site from the sunphotometer.

Summary table of parameters collected (Word doc 185 kB)

Ship measurements

The set of parameters directly derived from the measurements made by the SeaWiFS Profiling Multichannel Radiometer (SPMR) to 200m depth and the SeaWiFS Multichannel Surface Radiometer (SMSR) will be (with Λs meaning the band set, i.e., (380, 411, 443, 456, 491, 510, 532, 560, 620, 665, 683, 705 779 and 865) nm. 

  • Above surface radiometers: Es(Λ); and
  • In-water radiometers: Ed(Λ), Eu(Λ).

From profiling with the CTD rosette to 400m, the parameters collected will be chlorophyll fluorescence, CDOM fluorescence, attenuation and absorption coefficients (412, 440, 488, 510, 532, 555, 630, 676, 715 nm), bb(440), bb(532), bb(650), temperature, conductivity and derived salinity, oxygen concentration, and surface PAR.

Samples are collected and filtered for subsequent determination of the phytoplankton pigments and particulate absorption. Water samples are also collected for subsequent lab measurements of CDOM absorption.

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Buoy measurements

The set of parameters directly derived from the measurements will be (with λ meaning the band set, i.e., 412, 443, 490, 510, 560, 665 and 683 nm) :

  • Above surface : Es(λ);
  • At 4 meters : Ed(λ), Eu(λ), Lu(λ), chlorophyll fluorescence; beam attenuation (660 nm)
  • At 9 meters : Ed(λ), Eu(λ), Lu(λ), chlorophyll fluorescence, beam attenuation (660 nm), bb(443) and bb(560), conductivity, temperature, pressure (CTD), two-axis tilt and compass.

From these measurements, various AOPs or IOPs might be derived, as the diffuse attenuation coefficients for upwelling and downwelling irradiance, Ku and Kd, the attenuation coefficient for upwelling radiance, KL, the diffuse reflectance just below the sea surface, R, the nadir Q-factor, Eu/Lu, the attenuation and backscattering coefficients, c and bb. The absorption coefficient, a, will be tentatively derived through inversion of the AOPs (using for instance Kd and R, assuming that they are accurately derivable from the 2 measurement depths of the buoy; e.g., see Gordon and Boynton, 1997; Leathers and McCormick, 1997, Barnard et al., 1999). Table 1 below shows how the data acquired on the system fits to the band sets of several ocean color sensors.

MERIS
10 nm

POLDER-3
20 nm

SeaWiFS
20 nm

MODIS
10 nm

412nm

0

0

443

0

0

0

490

0

0

-2

510

0

560

+5

-5

-5

665

+5

+5

+2

683

0

Table 1.  The MERIS wavelengths, as acquired on the buoy (leftmost column), and the spectral shift of other satellite bands with respect to those of MERIS . The second row gives the channel bandwidths. This table prepared from the IOCCG (1998) report .

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Coastal measurements

The parameters collected there are the sun and sky radiances, using standard filters at 440, 675, 870, 940, 1020 nm and a polarized filter for 870 nm and are used to derive total column water vapor, ozone and aerosol properties, including Angström coefficients, optical thickness and polarization ratios. These derived parameters can be viewed at http://www-loa.univ-lille1.fr/photons/photosdessites/site_photo_Villefranche.htm and http://aeronet.gsfc.nasa.gov.

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