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Table 14.10 Technologies Developed for Rapid Identi cation of Postconsumer Plastics by Resin Type [10]

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There have been efforts made to push the speed of Token Ring networks beyond the standard 16 Mbps. High-speed Token Ring has not been fully deployed with the decline in newer Token Ring installations. However, it is

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charging are of particular interest and utilize the simple principle that when dissimilar materials, for example, particles of two different plastics, are rubbed together they transfer electrical charge and the resulting surface electrical charge differences can be used to separate the two plastics in an electric eld [42, 75, 87, 88]. Table 14.17 shows a triboelectric series for some common polymers. Figure 14.21 shows an example of an experimental device that has been used to evaluate the separation of numerous mixed plastic streams. The operating principle is shown schematically in Figure 14.22. Many plastic separations are possible using electrostatics [42, 87 91] including the separation of ABS and HIPS from end-of-life electronics, ABS and PMMA from automotive taillights, PP and PE, PET and nylon, PET and PVC, PVC and PE from wire and cable scrap, and the separation of water bottle PVC and PC. Consistent results require careful cleaning and preconditioning of the mixed plastic feedstocks. Some of the advantages and disadvantages of electrostatic separation methods are summarized here: Electrostatic Separators Advantages Dry process Rather known technology from the mineral processing industry Very few moving parts Rather simple design Demonstrated for several binary mixtures Disadvantages Puri er more than a separator Particles must be small but not too small Particle shape can be important Must control humidity and particle moisture level Surface-sensitive technique: surface cleanliness important Somewhat expensive ($100,000 + range)

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3.7. POINT DIFFRACTION INTERFEROMETER Another interesting common path interferometer is the so-called point diffraction interferometer, rst described by Linnik in 1933, rediscovered by Smartt and Strong (1972), and more fully developed by Smartt and Steel (1975). The principle of this interferometer is shown in Figure 3.22. The wave to be examined is brought to a focus to produce an image, usually aberrated, of a point source. At the plane of that image, an absorbing lm is placed. This lm contains a small pinhole or opaque disk in order to diffract the light and produce a spherical reference wavefront. Figure 3.23(a) shows the amplitude magnitude at the image plane, where the diffracting plate is located and Figure 3.23(b) shows the total amplitude after passing the diffracting plate, which can be considered as the superposition of two images as in Figure 3.23(c). To produce an interferogram with good contrast, the wave passing through the lm and the diffracted spherical wave should have the same amplitude at the

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