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By R. A. F. Williams

ISBN-10: 0750611065

ISBN-13: 9780750611060

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Soc, Faraday Trans. 2, 1987, 83, 221. J. , 1989. M. Z. Akcasu and M. Daoud, Macromolecules, 1980, L3, 1703. G. , 1979. 10 A. Lips, C. Smart and E. , 1971, 67, 2979. A. Sack, Nature, 1953, 171, 310. 12 13 V. O. Dalton and K. E. van Holde, Biopolymers, 1967, 5, 135. P. ,Interscience Publ. 1954. 14 M. Z. , 1916, ±7, 557. 15 R. Botet, R. Julien and M. A, 1984, 17 ,L75. C. A. , 1984, 29, 2966. A. Wietz and M. Lett. 1984, 52, 1433. 18 P. Lett. A. Weitz and M. , 1984, 52, 1433. 49 19 A. M. Soc, Faraday Trans.

1st Intn. Mineral Process. Fleming (ed), 1974, pp66-73. 6. R. , 31 (1982) 255-262. 7. J. A. Hamza, Application of flocculants in hydrocyclone separation, Can. Instn. Min. Metall. , 66 (1973) 78-85. 32 1 Stream ΔΡ 50 70 90 10 Q 1 /m s~ U 0 F F* U 0 F F* U 0 F F* 6 . 83 /kg nr 3 /g 6 5 dm~ Wt. 5 29. 9 — 82. 9 - 100. 46 22345 20358 22345 1 0 0 . l); column 8 relates to performance of a single hydrocy clone, columns 1-6 refer to 6 x hydrocyclones in the manifold unit, Figure 2). 72 - Γ 8 12874 15400 12874 Body Re == 4 3 6 8 100.

It is of interest that the inorganic sols give higher values for d (see Table 1) than would be expected for DLA. This may be the result of two effects. Firstly, as these suspensions are slightly polydisperse, smaller particles will be able to pack into gaps between the larger particles resulting in a higher fractal dimension. Secondly, and more importantly in the case of Agl, is the possibility of rearrangement. Because the particles are lozenge shaped, particles initially sticking obliquely will tend to be forced by hydrodynamic forces into face-face configurations.

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Advances in Measurement and Control of Colloidal Processes by R. A. F. Williams


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