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Scattering by Single Particles General Considerations

In many applications, the most important characteristic of the scattered wave is its intensity, /, expre.ssed in cgs units as erg/cm sec. At large distances from the origin, the energy flowing through a spherical surface element is 7r- sin0 d9 This energy flows radially and depends on 6 and (p but not on r. It is proportional to the intensity of the incident beam In and can be expressed as follows  [Pg.126]

The wavelength of the incident beam. is introduced in the denominator to make the scattering function, F 6, p. X), dimensionless. In general, F 0. A.) depends on the [Pg.126]

scattering function can be determined from theory for certain important special cases as discussed in the following sections. The performance of optical single-particle counters (Chapter 6) depends on the variation of the scattering function with angular position, and much effort has been devoted to the design of such detectors. [Pg.126]

The intensity function, by itself, is not suffleient to characterize the scattered light. Needed also are (he polarization and phase of the scattered light, which are discussed in the [Pg.126]

This defines the scattering cross section which has the dimension of area but is not in general equal to the particle cross-sectional area. Indeed it is customary to define the scattering efficiency [Pg.127]


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