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首页> 外文期刊>Continental Shelf Research: A Companion Journal to Deep-Sea Research and Progress in Oceanography >Light scattering by particles suspended in the sea: The role of particle size and density
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Light scattering by particles suspended in the sea: The role of particle size and density

机译:悬浮在海中的粒子的光散射:粒子大小和密度的作用

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Optical scattering and particle size measurements are reported at 78 stations along the south and west coast of Britain. The composition of the particles is mainly mineral (70% by mass on average) and the light scattering per unit concentration of suspended particles, the specific scattering coefficient, was observed to vary by over an order of magnitude, from less than 0.1 to over 1 m(2) g(-1). More than 3/4 of this variance is explained by changes in the apparent density (dry weight/'wet' volume) and mean size of the particles. For this data set, the specific scattering coefficient can be written b*(M) = (2.35/rho D-A) where b*(M) is the scattering coefficient per unit concentration of mineral particles, rho the apparent density and D-A the mean particle diameter by area. The standard error of the numerator in this equation is 0.08. In fact, most (64%) of the variance in b*(M) is explained by differences in the apparent density of the particles, with variations in particle diameter alone accounting for only 15% of the variance. Because particles in coastal waters flocculate into aggregates containing mineral and organic material as well as water, the apparent density of the particles is variable and considerably less than solid mineral material. Provided a suitable atmospheric correction for visible-band imagery over shelf seas can be applied, it may be possible to estimate b* using satellite remote-sensing measurements of reflectance at two wavelengths. This work has shown that maps of b* produced in this way will be sensitive to variations in near-surface particle density as well as size. It may, however, be possible to use site-specific empirical relationships between particle size and density to derive both of these parameters from space. (C) 2009 Elsevier Ltd. All rights reserved.
机译:据报道,沿英国南海岸和西海岸的78个站点进行了光散射和粒度测量。颗粒的成分主要是矿物(平均占质量的70%),观察到每单位浓度的悬浮颗粒的光散射(比散射系数)在一个数量级上变化,从小于0.1到大于1。 m(2)g(-1)。表观密度(干重/“湿”体积)和颗粒平均尺寸的变化解释了这种差异的3/4以上。对于此数据集,可以将比散射系数写为b *(M)=(2.35 / rho DA),其中b *(M)是每单位浓度矿物颗粒的散射系数,rho表观密度,DA是平均颗粒直径按面积。该公式中分子的标准误差为0.08。实际上,b *(M)的大部分变化(64%)是由颗粒表观密度的差异来解释的,仅粒径的变化仅占变化的15%。由于沿海水中的颗粒会絮凝成含有矿物质和有机物质以及水的聚集体,因此颗粒的表观密度是可变的,并且远低于固体矿物质。如果可以对架子海上的可见光波段图像进行适当的大气校正,则有可能使用两个波长的反射率的卫星遥感测量来估计b *。这项工作表明,以这种方式产生的b *图将对近表面粒子密度和尺寸的变化敏感。但是,可以使用粒度和密度之间的特定位置的经验关系从空间导出这两个参数。 (C)2009 Elsevier Ltd.保留所有权利。

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