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A model for partitioning the light absorption coefficient of natural waters into phytoplankton, nonalgal particulate, and colored dissolved organic components: A case study for the C hesapeake B ay
Author(s) -
Zheng Guangming,
Stramski Dariusz,
DiGiacomo Paul M.
Publication year - 2015
Publication title -
journal of geophysical research: oceans
Language(s) - English
Resource type - Journals
eISSN - 2169-9291
pISSN - 2169-9275
DOI - 10.1002/2014jc010604
Subject(s) - absorption (acoustics) , colored dissolved organic matter , attenuation coefficient , parameterized complexity , phytoplankton , particulates , biological system , exponential function , chesapeake bay , environmental science , chemistry , mathematics , physics , optics , mathematical analysis , algorithm , geology , organic chemistry , nutrient , oceanography , estuary , biology
We present a model, referred to as Generalized Stacked‐Constraints Model (GSCM), for partitioning the total light absorption coefficient of natural water (with pure‐water contribution subtracted), a nw (λ), into phytoplankton, a ph (λ), nonalgal particulate, a d (λ), and CDOM, a g (λ), components. The formulation of the model is based on the so‐called stacked‐constraints approach, which utilizes a number of inequality constraints that must be satisfied simultaneously by the model outputs of component absorption coefficients. A major advancement is that GSCM provides a capability to separate the a d (λ) and a g (λ) coefficients from each other using only weakly restrictive assumptions about the component absorption coefficients. In contrast to the common assumption of exponential spectral shape of a d (λ) and a g (λ) in previous models, in our model these two coefficients are parameterized in terms of several distinct spectral shapes. These shapes are determined from field data collected in the Chesapeake Bay with an ultimate goal to adequately account for the actual variability in spectral shapes of a d (λ) and a g (λ) in the study area. Another advancement of this model lies in its capability to account for potentially nonnegligible magnitude of a d (λ) in the near‐infrared spectral region. Evaluation of model performance demonstrates good agreement with measurements in the Chesapeake Bay. For example, the median ratio of the model‐derived to measured a d (λ), a g (λ), and a ph (λ) at 443 nm is 0.913, 1.064, and 1.056, respectively. Whereas our model in its present form can be a powerful tool for regional studies in the Chesapeake Bay, the overall approach is readily adaptable to other regions or bio‐optical water types.

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