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Absorption properties of marine particles and CDOM:

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Title: Absorption properties of marine particles and CDOM:


1
Absorption properties of marine particles and
CDOM
  • Use of special measurement devices Ultrapath and
    PSICAM
  • Marcel Babin
  • Annick Bricaud
  • Edouard Leymarie
  • Antoine Sciandra

2
Motivations (1)
- The relative contributions of CDOM,
phytoplankton and non-algal particles (NAP) to
light absorption have to be known for
predicting/interpreting the inherent and apparent
optical properties of the ocean.

- In open ocean waters, especially in ultra-clear
waters, these relative contributions are
difficult to quantify and poorly known. We
believe that these relative contributions are
highly variable.

3
Motivations (2)
  • - Some of our previous observations (aNAP/ap is
    largest in the Med Sea, and lowest in the
    Pacific, Bricaud et al. 1998) suggest that iron
    could contribute to non-algal absorption in some
    open ocean waters

- Iron could also play a role in light absorption
by CDOM (e.g. Emmenegger et al. 2001)
4
Objectives for the BIOSOPE cruise
  • - To quantify the relative contributions of
    phytoplankton, CDOM and NAP to light absorption
    in the BIOSOPE area, using new (highly sensitive)
    measurement devices

- To study the variability of these contributions
in the various areas explored during the cruise
(contrasted wrt. iron limitation) -gt role
of iron in light absorption by NAP and CDOM?
- To extend our database of phytoplanktonic
absorption to ultra-oligotrophic waters, and
check the validity of the previously developed
parameterizations (af(l) vs. chl)
5
Methods
  • - Classical methods
  • Particulate absorption concentration of
    particles on a GF/F filter, spectrophotometric
    analysis
  • CDOM absorption spectrophotometric measurements
    using 10 cm cells

These methods are adequate for mesotrophic waters
(will be used as often as possible as reference)
but not for ultra-oligotrophic waters (CDOM
absorption too low large seawater volume needed
for particulate absorption)
two alternative (complementary) methods -
Ultrapath (commercial instrument, pathlength 2
m) - PSICAM (prototype in development,
pathlength gt 5 m)
6
Ultrapath system
Peristaltic pump
Spectrophotometer TIDAS 1
Light source
Optical fiber
Ultrapath cell
Sample
7
Ultrapath tests on natural samples and algal
cultures(DEA Maria Vlachou, 2003)
Phytoplanktonic culture
Dyfamed, 40 m
  • Sensitive method for CDOM absorption
    measurements
  • Can be used also for particulate absorption
    measurements (needs accurate scattering
    correction gt ac-9)
  • The rinsing protocol is being automatized to
    provide reproducible measurements (A. Sciandra,
    G. Malara)

8
Methodological Development PSICAM (Point Source
Integrating Cavity Absorption Meter)
  • Theoretical concept formulated by Elterman
    (1970), developed by Kirk (1995)
  • Advantages
  • Extremely sensitive (pathlengths up to more than
    10 meters)
  • Insensitive to scattering by particles

9
Agenda of the PSICAM development
  • Dec 2003 Feb 2004 Development of a 3-D Monte
    Carlo code to optimize the design of the sphere
  • Feb 2004 Visit to JTO Kirks lab
  • March-April Building of the system
  • May-June Tests in lab and calibration protocol
  • July-October Tests at sea
  • ? BIOSOPE

10
Supplementary measurements needed
  • HPLC pigment concentrations
  • In situ absorption/ attenuation (ac-9)
    measurements (correction of Ultrapath ap
    measurements)
  • Particle dry weight (filtration of 7 L of
    seawater)
  • Iron concentration (particulate and dissolved),
    and ionic (ferric/ferrous) composition if
    possible

11
Methodological Development PSICAM (Point Source
Integrating Cavity Absorption Meter)
  • Theoretical concept formulated by Elterman
    (1970), developed by Kirk (1995)
  • Advantages
  • Extremely sensitive (pathlengths up to more than
    10 meters)
  • Insensitive to scattering by particles

12
SimulO Forward 3-D Monte-Carlo Simulation Program
13
Surface / Volume properties
  • Snell Fresnel Laws
  • (example parallel plate)

14
Simulation of the Point Source
  • Water sample a 5 m-1 , b 2 m-1 (Petzold)
  • Ideal and Simulated Sources (Number of photons
    3.5 108)

?
99 Lambertian surface
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