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For Web applications, data-source design is just as important as page design. A well-designed data source may have a tremendous impact on Web site performance and scalability. Generally, the more a database is divided into discrete tables, the more flexible it is; the goal is to force the user to download only the necessary data. Although you may not have complete control over how the site s databases and the like are structured, you should have a complete understanding of the fields used and the type of data stored within them. For example, if the links to product images are in URL format, such as http://www.idest.com/images/logoanim/ logoanim.gif, the code calling the dynamic link is different than if the same field stored data as plain text, such as logoanim.gif.

Suppose you know that while this projection formula is accurate overall, you would get a more accurate projection for the Pants category if you were to use a factor of 1.4 instead of 1.2. All you need to do is move the pointer to cell D10, where the calculated projection for Pants is located, press F2 to edit the formula, and make the desired change. However, this kind of ad hoc change to a PivotTable is generally considered to be bad practice because it is so hard to trace.

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Mixed mode usage, which includes Polygon functionality, is available when the Lasso Tool is in Freeform Mode. To work in Freeform Mode, the Polygon option must be in the off position. While drawing with the Freeform Lasso, press the Alt (Option) key to temporarily invoke Polygon Mode. (Polygon Mode continues only as long as the Alt (Option) key is pressed.) Now, straight polygonal lines can be described between selection points that are created by a mouse click. That is, as long as the Alt (Option) key is pressed, a straight selection line extends between mouse clicks. To return to Freeform Mode, simply sneeze or release the Alt (Option) key. Release the mouse to close the selection.

where the generalized momentum p conjugate to q is p = a L / a q . Differentiation of (2.6) leads to Hamilton s equations of motion,

The result is reasonably nice, as shown in Figure 5-5.

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2-512 Large Eddy Simulation The second approach is to use large eddy simulations The limitations of this method are much less severe The large scale motions are computed in a manner similar to DNS but on a much coarser grid The scale might be as coarse as 1 : 30 The computational domain would then be 303 = 27 104 , which would not be dif cult with current machines A grid several times as ne as this would not be out of the question, and initial LES simulations in stirred tanks have recently been reported (Bakker et al, 1998; Revstedt et al, 1998; Derksen and van den Akker, 1999; Roussinova et al, 2001) This modeling approach computes the larger scales of turbulence directly as they vary in time and models the ner scales of turbulence.

\ = -5 X, p(/) i=t+\

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