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BSA Flow Software Installation and User's Guide - CSI

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Figure 7-45. The upper panel shows ray traces indicating the three modes<br />

of scattering, reflection <strong>and</strong> first <strong>and</strong> second order refraction, for a water<br />

droplet. In the lower panel, the light intensity (log scale, one decade<br />

between each circle) for each of these modes is shown in a polar plot for<br />

scattering angles from 0° to 180° <strong>and</strong> for two polarizations — the upper half<br />

at 90° to the scattering plane, <strong>and</strong> the lower half parallel to the scattering<br />

plane.<br />

Dependence of geometrical factor on relative refractive index<br />

Refraction by As it appears from equation (For first order refraction (Equation 7-17)) for<br />

first order refraction, the geometrical<br />

a droplet factor, β, for refraction depends on the relative refractive index of the<br />

particle, n rel , in addition to the angles ϑ, ψ <strong>and</strong> ϕ. In many situations the<br />

exact value of n rel is not known.<br />

As shown in Figure 7-46, the geometrical factor, β, becomes less dependent<br />

on n rel as the scattering angle ϕ increases. Clearly, however, there is a limit<br />

to how great a scattering angle can be used, since light scattered by<br />

refraction only exists at scattering angles less than ϕ c1 . Moreover, to get a<br />

linear size-phase relationship regions where two or more modes of scattering<br />

make contributions of the same order of magnitude to the intensity of the<br />

scattered light should be avoided.<br />

7-52 <strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>: Reference guide

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