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Figure 6-28 shows changes in these parameters as the vessel volume is increased for several processes. The exponents x and y in Figure 6-28 should be determined experimentally or veri ed even for the processes listed in these plots. Some mixing equipment vendors prefer to use the TQ /V criterion because it has a direct impact on the overall size and cost of the mixer, including the gearbox. When choosing a scale-up method, one must consider changes in other ow and power parameters and their impact on the process result. Table 6-8 shows how these important parameters change on scale-up to 10 times the diameter and 1000 times the volume of laboratory mixing tank. Scale-up methods based on constant blend time require the mixer speed in the commercial vessel to be the same as in the laboratory vessel. This, however, results in a very large increase in the motor power. Such a demanding criterion is necessary for very fast to instantaneous reactions where the reaction lifetime may be a few seconds. Commercial reactors for such systems are, therefore, relatively small in size. Using constant P/V, the mixer speed decreases by 78%, but the blend time increases by a factor of 4.6. If constant P/V is used in scaling up a reacting system, the reactors may need to be sized for longer residence time than the laboratory reactor because of the increase in blend time. It should be noted that the Reynolds number increases by a factor of 21.5, and therefore,



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bei Videoverkehr mit Matrix-geometrischen stochastischen Petrinetzen. In: K. Irmscher (editor), Proceedings of the 9th ITG/GI Workshop on Measurement, Modeling and Evaluation

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A traveling matte (or mask) is a special effect that combines motion and masking. Typically the matte is a shape that moves across the screen. Within the matte is one image; outside the mask is a background image. Figure 14-11 shows an example of the traveling matte effect. Notice that one image is seen through a star-shaped graphic pattern, which is the mask. The matte is simply a star-shaped white graphic created against a black background.

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Doi, M, and S F Edwards Dynamics of concentrated polymer systems Part 2 Molecular motion under flow J Chem SOCFaraday Trans II 74 (1978) 18021817 Doi, M, and S F Edwards Dynamics of concentrated polymer systems Part 3 The constitutive equation J Chem SOC Faraday Trans II 74 (1978) 1818-1832 Doi, M, and S F Edwards Dynamics of concentrated polymer systems Part 4 Rheological properties J Chem SOCFaraday Trans II 75 (1 979) 38-54 Doi, M, and S F Edwards The Theory of Polymer Dynamics International Series of Monographs on Physics, Volume 73 (Clarendon, Oxford, 1986) Doi, M, and T Ohta Dynamics and rheology of complex interfaces I J Chem Phys 95 (1991) 1242-1248 Dorfman, I Dirac Structures and Integrabiliry of Nonlinear Evolution Equations Nonlinear Science: Theory and Applications (Wiley, Chichester, 1993) Dressler, M, and B J Edwards.

The influence of matrix viscoelasticity on the rheology of polymer blends Rheol Acta 43 (2004)257-282 Dressler, M, B J Edwards, and H C Ottinger Macroscopic thermodynamics of flowing polymeric liquids Rheol Acta 38 (1999) 1 17-136 Eckart, C The thermodynamics of irreversible processes 111 Relativistic theory of the simple fluid Phys Rev 58 (1940) 919-924 Edwards, B J An analysis of single and double generator thermodynamic formalisms for the macroscopic description of complex fluids J Non-Equilib Thermodyn 23 (1998) 301-333 Edwards, B J, A N Beris, and V G Mavrantzas A model with two coupled Maxwell modes J Rheol 40 (1 996) 9 17-942 Edwards, B J, A N Beris, and H C Ottinger An analysis of single and double generator thermodynamic formalisms for complex fluids 11 The microscopic description J Non-Equilib Thermodyn 23 ( 1998) 334-350 Edwards, B J, H C Ottinger, and R J.

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