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Figure 3-28 The left-hand side of the gure shows the concentration of reactants A and B after the rst three ow periods in the sine ow with T = 1.6. The right-hand side is the corresponding product concentration. See insert for a color representation of this gure.

1 1 1 1

389. W. E. Doering and W. R. Roth, Angew. Chern., Int. Ed. Engl. 2,115 (1963); Tetrahedron, 19, 715 (1963). 390. B. H. Meier and W. L. Earl, J. Arn. Chern. Soc. 107,5553 (1985). 391. P. R. Schreiner, A. Wittkopp, P. A. Gunchenko, A. 1. Yaroshinsky, S. A. Peleshanko, and A. A. Fokin, Chern. Eur. J. 7, 2739 (2001). 392. S. Moss, B. T. King, A. de Meijere, S. 1. Kozhushkov, P. E. Eaton, and J. Michl, Org. Lett. 3, 2375 (2001).

Strong Coupling Expansions Weak coupling expansions correspond to normal perturbation theory On a lattice these are complicated by problems such as the loss of Lorentz invariance, and a lattice offers few advantages as a regularization for weak coupling Lattice theories are most useful for strong coupling situations A strong coupling approximation may be implemented by expanding the measure exp( -/3 C, E p )appearing in a Euclidian path integral in powers of p N l/gz, which is a small number if the coupling is large Strong and weak coupling expansions produce useful results for their respective domains, but it is frequently necessary to determine how these domains are related For example, the question of confinement in QCD turns on whether the field theory exhibits a phase transition between the strong and weak coupling regimes.

The CD-ROM included with this book is a hybrid CD-ROM, which means it contains files that run on more than one computer platform in this case, both Windows and Macintosh computers. Several files, primarily the Macromedia trial programs and the other external programs, are compressed. Double-click these files to begin the installation procedure. Most other files on the CD-ROM are uncompressed, and you can simply copy them to your system by using your file manager. Almost all of the Dreamweaver extensions are also compressed and are installed with the Extension Manager, as described in the Dreamweaver extensions section below. In the Examples folder, the file structure replicates the chapter structure of the Dreamweaver MX 2004 Bible. In the Additional Extensions folder, you ll find the various behaviors, objects, and so on, filed under the author s name.

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The analysis above shows that higher speci c power input is necessary both to prevent impeller ooding and to achieve complete dispersion at the large scale. Also, from the ooding correlation, for constant aeration rate and a xed vessel size, 1 D4.5 N2 and therefore NF D 5/2 (18-40) F NF D3 Since constant pumping capacity implies that N D 3 , eq. (18-40) may be taken to imply that at a xed scale of operation, a constant pumping rate is required to disperse a given ow of gas. Also, the use of large D/T ratios is more economical since PF D 5/2 (18-41) Therefore, lesser power is required to prevent ooding using large D/T ratios, or for the same power input, the gas-handling capacity of the impeller is increased. This would also imply that the drop in aerated power draw would be less when larger D/T ratios are used. Similar analysis using the complete dispersion correlation results in PF N3 D5 and replacing NF using eq. (18-40) results in F PCD D 1 (18-42)