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Overview of Optical Oceanography


Page updated: Jun 25, 2015
Principal author: Curtis Mobley
Various reflectances are probably the most commonly used apparent optical properties because they are fundamental to remote sensing of the oceans. In the early days of ocean color remote sensing, algorithms were developed to relate the irradiance reflectance R to quantities such as absorption and backscatter coefficients and chlorophyll concentrations (e.g., Morel and Prieur, 1977; Gordon and Morel, 1983). More recently, the remote-sensing reflectance $ R_{\rm rs}$ has become the AOP of choice for remote sensing of ocean properties (e.g., O'Reilly et al. (1998); Mobley et al. (2005)). We now consider each of these reflectances.

The spectral irradiance reflectance (or irradiance ratio), $ R(z,\lambda)$ , is defined as the ratio of spectral upwelling to downwelling plane irradiances:

$\displaystyle R(z, \lambda )~\equiv ~{\frac{E _{u} (z, \lambda )}{E _{d} (z, \lambda )}} \,\, .

$ R(z,\lambda)$ is thus a measure of how much of the radiance traveling in all downward directions is reflected upward into any direction, as measured by a cosine collector. This is illustrated in Fig. 1. Depth z can be any depth within the water column, or in the air just above the sea surface.

Figure: Fig. 1. Illustration of light rays contributing to the irradiance reflectance R.
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Irradiance reflectance has the virtue that it can be measured by a single, uncalibrated, plane irradiance detector. The downwelling irradiance $ E_d$ can be measured, and then the detector can be turned "upside down" to measure $ E_u$ . The calibration factor needed to convert from detector units (voltage, current, or digital counts) to irradiance units ( $ \rm {W~m^{-2}~nm^{-1}}$ ) cancels out.

The spectral remote-sensing reflectance $ R_{\rm rs}$ is defined as

$\displaystyle R _{\rm rs} (\theta ,\phi ,\lambda )~ \equiv ~{\frac{L _{w} ({\rm in~air} , \theta ,\phi ,\lambda )}{E _{d} ({\rm in~air} , \lambda )}} ~~~~~{\rm (sr ^{-1} )} \,\, .

Here the depth argument of "in air" indicates that $ R_{\rm rs}$ is evaluated using the water-leaving radiance $ L_{w}$ and $ E_d$ in the air, just above the water surface. The remote-sensing reflectance is a measure of how much of the downwelling radiance that is incident onto the water surface in any direction is eventually returned through the surface into a small solid angle $ \Delta \Omega$ centered on a particular direction $ (\theta,\phi)$ , as illustrated in Fig. 2.

Figure: Fig. 2. Illustration of light rays contributing to the remote-sensing reflectance $ R_{\rm rs}$ .
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Although $ R_{\rm rs}$ is often computed for nadir-viewing directions only, in actual remote sensing it is usually an off-nadir direction that is being observed by an airborne or satellite remote sensor. As shown next, $ R_{\rm rs}$ has the virtue that it is less sensitive to environmental conditions such as sun angle or sky conditions than is R. This is the reason that it has replaced R for remote sensing. However, determination of $ R_{\rm rs}$ is more difficult than R. First, the measurements of $ L_{u}$ and $ E_{d}$ require different sensors, which must be accurately calibrated. Second, the water leaving radiance $ L_{w}$ cannot be measured directly. Only the total upwelling radiance $ L_{u}$ above the surface can be measured. This $ L_{u}$ is the sum of the water-leaving radiance $ L_{w}$ and the downward sun and sky radiance that is reflected upward by the sea surface, $ L_{s}$ , as illustrated in Fig. 3. $ L_{w}$ therefore must be estimated either from a measurement of the total upwelling radiance $ L_{u}$ made above the sea surface, or from a measurement of $ L_{u}$ made some distance below the sea surface and extrapolated upward through the surface. Each of these estimation methodologies has arguments for and against its use (e.g., Mobley (1999); Toole et al. (2000)).

Figure: Fig. 3. Illustration of light rays contributing to $ L_{u}$ as measured above the sea surface.
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To illustrate the dependence of R and $ R_{\rm rs}$ on IOPs and external environmental conditions, the HydroLight radiative transfer numerical model was run using an IOP model for Case 1 waters with chlorophyll concentrations of 0.1, 1.0, and $ 10.0~\rm {mg~m^{-3}}$ . For each chlorophyll concentration, runs were made for three sets of sky conditions: (1) a level sea surface (windspeed U = 0) and the sun at the zenith (sun = 0) in a clear sky; (2) a rough sea surface with a wind speed of $ U = 10~\rm {m~s^{-1}}$ and the sun at a 50 deg zenith angle (sun = 50) in a clear sky; (3) a wind speed of $ 10~\rm {m~s^{-1}}$ and a heavily overcast sky (overcast) for which the sun's location cannot be discerned.

Figure 4 shows the resulting R spectra at depth $ z = 0$ , which is in the water just below the mean sea surface. This is the quantity most often used to develop remote-sensing algorithms relating R to IOPs or chlorophyll concentrations. The curves for the different chlorophyll concentrations group together, showing that the shape of the R spectra is determined primarily by the different IOPs associated with the different chlorophyll concentrations. However, there is also a significant effect of the sky conditions on the R spectra within each of the three chlorophyll groups.

Figure: Fig. 4. Dependence of R on chlorophyll concentration, sky condition, and wind speed for selected conditions in Case 1 water.
Image 9026807a1fb85ae3f700ce0c6fd39bfb

Figure 5 shows the nadir-viewing $ R_{\rm rs}$ spectra for the same set of HydroLight runs. The three chlorophyll groups are similar in shape to the corresponding R spectra, but there is much less variability in the $ R_{\rm rs}$ spectra due to the external environmental conditions. $ R_{\rm rs}$ is thus a better AOP than is R, because $ R_{\rm rs}$ is less sensitive to the sky conditions while remaining very sensitive to the different IOPs corresponding to the different chlorophyll concentrations.

Figure: Fig. 5. Dependence of $ R_{\rm rs}$ on chlorophyll concentration, sky condition, and wind speed for selected conditions in Case 1 water.
Image 872a3e4b74ab951269bf955aef8813e4

Figure 6 shows the $ R_{\rm rs}$ spectra for nadir $ (\theta_v = 0)$ vs. various off-nadir $ (\theta_v, \phi_v)$ viewing directions. Azimuthal angle $ \phi_v = 90 \deg$ corresponds to looking at right angles to the sun's azimuthal direction, and $ \phi_v = 135 \deg$ is looking half-way between normal to the sun and away from the sun. This range of $ \phi_v$ values is what is usually observed in remote sensing to avoid sun glint from the sea surface. At the lowest chlorophyll concentration, there is not much difference in the spectra for the different viewing directions. However, the differences increase with increasing chlorophyll concentration, and are quite significant for the $ (\theta_v = 60)$ curves when $ Chl = 10~\rm {mg~m^{-3}}$ . These differences in off-nadir directions for different chlorophyll values are a consequence of the changes in shape and relative importance of the scattering phase functions for the small and large chlorophyll-bearing particles vs. that of water as the chlorophyll concentration increases.

Figure: Fig. 6. Dependence of $ R_{\rm rs}$ on chlorophyll concentration in Case 1 water and viewing direction, for a wind speed of 10 m/s and a sun zenith angle of 50 deg.
Image 2b844b63704c54e43c436d0b0d8256ef

As Figs. 5 and 6 show, $ R_{\rm rs}$ is much more sensitive to water IOPs than to external environmental conditions and viewing direction. However, $ R_{\rm rs}$ still does depend somewhat on solar zenith angle (Fig. 5) and viewing direction (Fig. 6). An even better AOP would be obtained if these remaining dependencies can be removed. The resulting AOP is called the exact normalized water-leaving reflectance, denoted by $ [\rho_w(\lambda)]_N^{ex}$ . This reflectance is based on the concept of the normalized water-leaving radiance, which is defined to be "...the radiance that could be measured by a nadir-viewing instrument, if the Sun were at the zenith in the absence of any atmospheric loss, and when the Earth is at its mean distance from the Sun" (Morel and Gentili (1996), page 4852). (Earlier papers often used phrases like "in the absence of an atmosphere", implying that the atmosphere is completely removed. This was found to be too extreme, so the current definition and calculations are based on a standard but non-attenuating atmosphere.) The computation and interpretation of $ [\rho_w(\lambda)]_N^{ex}$ can be rather subtle. These matters are discussed in detail on the page Normalized Reflectances

When processing satellite ocean color imagery, measured top-of-the-atmosphere radiances are converted by the process of atmospheric correction to $ [\rho_w(\lambda)]_N^{ex}$ spectra, which can then be used in algorithms to retrieve geophysical quantities such as the chlorophyll concentration. However, when running HydroLight, $ [\rho_w(\lambda)]_N^{ex}$ can be obtained by putting the sun at the zenith, in which case $ [\rho_w(\lambda)]_N^{ex}$ is $ \pi$ times the nadir-viewing $ R_{\rm rs}$ :

$\displaystyle [\rho_w]_N^{ex} = \pi R_{\rm {rs}}({\rm {HydroLight}};\theta_s = 0,\theta_v = 0) \,.$ (1)

The remote-sensing reflectance reported by NASA as a standard output for sensors such as MODIS or VIIRS is sometimes described as $ [\rho_w(\lambda)]_N^{ex}/\pi$ , which is equivalent to the HydroLight-computed $ R_{\rm {rs}}(\theta_s = 0,\theta_v = 0)$ .

Although $ [\rho_w]_N^{ex}$ or its equivalent $ R_{\rm {rs}}$ are now used for most remote sensing, R is still sometimes measured in water and has its uses. An example of inverting R spectra to obtain absorption and scattering properties can be seen in Roesler and Perry (1995).