The optical pathlength amplification (p factor), induced by multiple scattering in glass-fibre filters used for light absorption measurements of aquatic particles, has been measured by the trans- mittance-reflectance (T-R) method for algal species with cell diameter in the range from 1 to 5 um. The p factors obtained showed a much lower dispersion than that observed in similar measurements carried out by the standard transmittance method, suggesting that this could be due, at least in part, to the incomplete account of the scattering losses taken by the latter method. An experimental test has verified that the (3 factor expression derived from measurements carried out by the T-R method on an algal culture is also applicable to detrital particles. Introduction The light-transmission measurement of particles retained on glass-fibre filters (Yentsch, 1962) is now the most frequently used method for determination of the light absorption spectrum of particles sampled from aquatic environments. The measurement is normally performed by dual-beam spectrophotometers, where the light transmitted through the particle-retaining filter is compared with the light transmitted through an unused 'reference' filter. In the following, this procedure is referred to as the 'standard transmittance' method. The experi- mental raw data are expressed in terms of the dimensionless optical density (OD), also called absorbance, which is equal to the base 10 logarithm of the inverse transmittance. The spectral range in these measurements covers the visible region, and it often extends to the UV and near-IR. The use of glass-fibre filters offers one major advantage and one major disadvantage. The advantage is that the filtration allows one to concentrate particles that are naturally too dilute to measure with standard spectrophoto- meters. The disadvantage is that the particles are embedded within a highly scat- tering medium, which causes an increase in the optical pathlength, resulting in a considerable enhancement of the measured optical density (often referred to as the p factor, following the terminology of Butler (1962)). Conversion of the optical density of the filter-retained particles, OD{, to the optical density of the particle suspension with the same geometrical pathlength, ODSUS, is carried out using empirical relationships. The uncertainty of these relationships probably represents the largest error source affecting the light-transmission measurements of particles retained on glass-fibre filters. Once ODSUS corresponding to a given measured ODf is determined, the volume absorption coefficient of the particle suspension, a (in m1), is obtained from the equation: a = 2.3 ODS11S/X, where X is the ratio of the filtered volume to the
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