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The most complete coverage of Illustrator: This book isn t big because I wanted to hog all the retail book space for myself (of course, that s not a bad idea), but it s because I tried to include every possible thing you d ever want to know about Illustrator From learning the basics of drawing to creating outstanding special effects with vectors and rasters, it s all here Fun, original, different artwork to illustrate the techniques and capabilities of Illustrator: When I say different, I m not talking about performance art Instead, I mean that each technique is created with a different piece of artwork Some of it is simple, and some of it is complex with each piece showing not only a particular feature but also other Illustrator capabilities Clean artwork without those annoying jaggies: This is vector software.

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K2 = k2, 0 + k2,1z -1 + . . . k2, n( k ) z - n( k2 )

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When you think of vectors, you probably think of smooth, flowing paths that don t look like someone filled in a bunch of squares on a sheet of graph paper So, instead of using screenshots for paths shown in this book, each path was painstakingly drawn in Illustrator I think you ll appreciate the difference Top-notch technical prowess: Again, the Illustrator CS5 Bible has gotten the best possible people to do a technical review of the book Previous editions were technically reviewed by the lead technical support engineer for Illustrator and UI designers who have worked on the product Perfect for teaching: If you know Illustrator inside and out, you ll find that the Illustrator CS5 Bible is the best teaching tool available for Illustrator, with examples and explanations that perfectly complement a teaching environment Many computer-training companies teaching Illustrator use this book, as do schools and universities.

The Reynolds number characterizes turbulence in any given pipeline ow or mixing device. It is instructive to consider rst the empty or unpacked pipe and look at the classic experiment by Osborne Reynolds (1883). His demonstration consisted of owing water through a clear glass tube with capability to vary the water ow rate to achieve a broad range of uid velocity. At the center of the tube a ne jet of water-soluble dye is introduced through a capillary tube so that a thin lament of dye injected coaxially into the stream of water has a velocity equal to that of the water at the point of introduction. Figure 7-1a shows that at low water velocity the dye lament retains its identity in the water stream, tending to widen very slightly during the downstream passage because of molecular diffusion of the dye into the water. At a slightly higher mean velocity as shown in Figure 7-1b, the dye lament breaks up into nite large eddies. Further downstream the eddies break up further, and the dye that has been introduced tends to become homogeneously dispersed or mixed with the water. At much higher mean velocity (Figure 7-1c) the eddy activity becomes extremely violent, and the region of homogeneous dye color approaches the point of dye entry. From visual observation it is evident that the eddies in normal pipe

Real-world examples and advice: Illustrator doesn t exist in a vacuum Instead, it s often used in conjunction with other programs and in a variety of different environments and situations Some people use Illustrator to create logos, others create full-page advertisements, and still others create entire billboards with Illustrator Throughout this book, I present various real-world situations and examples that add to your understanding of each topic..

uid mixing) have allowed more detailed analysis to be performed of the state of mixing. Early computational studies showed more rapid mixing than experimental studies. This was due to a phenomena called numerical diffusion, where with coarse grids numerical rounding errors cause a smoothing of concentration gradients. With ner grids and the tracking of large number of massless particle tracking, the accuracy of the calculation matches well with the experimental measurements. This has been demonstrated in laminar ow for both the Koch SMX and the Kenics KMS motionless mixers by Zalc et al. (2003) and for turbulent mixing with Kenics HEVs by Bakker and LaRoche (1993).

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