Abstract
The average cosine of the underwater light field (µ̄) is a simple quantity that describes the angular distribution of radiance at a given point. A model of the rate of vertical change of µ̄ in the ocean was developed in order to examine the influences of light absorption and scattering. We made calculations of radiative transfer based on invariant imbedding theory assuming an optically homogeneous ocean with a typical scattering phase function and the simple boundary conditions of the sun overhead in a black sky and a flat ocean surface. Under such conditions, the decrease of µ̄ throughout the water column is well approximated by a single exponential function. The dependence of the parameter Pτ, which describes the rate of change of µ̄ with optical depth, on the single‐scattering albedo ωo, is well approximated by a quadratic function. By applying a linearization technique to the Pτ vs. ωo relationship, we identified the contributions of absorption and scattering to Pτ. Our results indicate that scattering is the more important process, contributing > 50% to Pτ for typical situations when ωo > 0.1. Absorption dominates Pτ when ωo < 0.1, which occurs only in very clear oceanic water at long wavelengths (>650 nm). Our analysis of the effect of scattering phase function shows that the scattering into the middle angles, approximately between 20° and 45°, largely determines the magnitude of Pτ. Using spectral bio‐optical models with several Chl concentrations, we also examined the rate of change in µ̄ with geometric depth Pz for various water types with realistic values of the absorption and scattering coefficients. This analysis shows large variations in both the magnitude and the spectral behavior of Pz with varying Chl concentration.
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