Plass G N, Humphreys T J, Kattawar G W
Appl Opt. 1981 Mar 15;20(6):917-31. doi: 10.1364/AO.20.000917.
The influence of the ocean-atmosphere interface on the radiance distribution in both the ocean and atmosphere is investigated. At visible wavelengths in the real ocean just below the surface, the downwelling radiance is a maximum within the critical angle and drops off by 1 or 2 orders of magnitude toward the horizon. The usual explanation that this is due to the sky radiation concentrated within the critical angle and the total internal reflection of the weak upward radiance at the ocean surface at angles outside the critical angle is too simplistic. There are two other important factors: (1) the atmosphere must have sufficient optical thickness so that appreciable sky (multiple scattered) radiation develops at all angles in the downward direction; (2) the water must have appreciable absorption so that the upwelling radiance just below the ocean surface is only a small fraction of the downwelling radiance entering the ocean. Examples show that, if either one of these conditions is not satisfied, an entirely different radiance distribution develops. The variation of the following quantities with depth is studied: radiance; vector and scalar irradiance; distribution function; reflectance; and heating rate. The radiance distribution in a homogeneous medium is compared with that in the same medium with an atmosphere-ocean interface at various depths within the medium. Most of the calculations are done for Rayleigh scattering centers, but some results are given for Mie-type scattering.
研究了海洋 - 大气界面对海洋和大气中辐射亮度分布的影响。在实际海洋中,恰好在海面下方的可见波长处,下行辐射亮度在临界角内达到最大值,并朝着地平线方向下降1或2个数量级。通常的解释是,这是由于天空辐射集中在临界角内,以及在临界角以外角度处海洋表面弱向上辐射亮度的全内反射,这种解释过于简单。还有另外两个重要因素:(1)大气必须具有足够的光学厚度,以便在向下的所有角度都产生可观的天空(多次散射)辐射;(2)水体必须具有可观的吸收,以便海洋表面下方的向上辐射亮度仅为进入海洋的下行辐射亮度的一小部分。示例表明,如果这两个条件中的任何一个不满足,就会产生完全不同的辐射亮度分布。研究了以下量随深度的变化:辐射亮度;矢量和标量辐照度;分布函数;反射率;以及加热率。将均匀介质中的辐射亮度分布与在介质内不同深度处具有海洋 - 大气界面的相同介质中的辐射亮度分布进行了比较。大多数计算是针对瑞利散射中心进行的,但也给出了一些米氏型散射的结果。