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You don t need to be in Expanded Tables mode to see the table outlines. If the Mouse-Over option is enabled, the outlines appear when you re in Standard mode when you hold down the Ctrl (Command) key and move over the table.

public void g l o b a l P r e d i c a t e T r u e ( i n t v [ I ) { Systcni , out . p r i n t l n ( * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * ) ; S y s t e m . o u t . p r i n t l n ( P r e d i c a t e t r u e a t : Util . writeArray ( v ) ) ;

The support for the inverse rule is exactly the same as the support for the original rule, because the two rules have the same combination of products. Perhaps more surprising, the lift for the two rules is the same as well. This is not a coincidence; it comes from the definition of lift. The formula simplifies to:

To split an open path, use the Scissors tool and move the cross-hairs pointer over a path, then click and release the mouse button. You can click an open portion of a segment (that is, between anchor points) or an anchor point. In both cases, two anchor points endpoints of the two resulting paths are created. To split a closed path, use the Scissors tool and move the cross-hairs pointer over a path and then click and release the mouse button. You can click an open portion of a segment or an anchor point. In both cases, two anchor points endpoints of the two resulting paths are created. Move the cross-hairs pointer to a different position along the same path and then click and release the mouse button. After you split a path, you can switch to either of the selection tools and then select, move, or modify either of the two resulting paths as you want. If you ve split a closed path, you may want to close the two open paths (as described in the previous section). The left side of Figure 16.21 shows a pair of open paths created using the Scissors tool on an open path. The right side of Figure 16.21 shows a closed graphics frame that s been split into two open frames.

ch0601_video.avi video on the companion web site at www.wiley.com/

CA and CB are the concentrations of species A and B. DAB , the diffusion coef cient, and kr , the reaction rate, are constant. The system is assumed incompressible and isothermal, and the scalar eld has no effect on the velocity eld (variations in concentration, for example, do not induce velocity gradients). Reynolds decomposition is used to separate the velocity and concentration elds into an average and uctuating part. When these terms are substituted into eq. (2-4), the resulting equation can be averaged9 to give accumulation of A + mean convection due to mean gradients of A + convection due to cross- uctuations of velocity and concentration = bulk diffusion reaction due to (mean eld + uctuating eld) CA + (U )CA + ( ua) = DAB 2 CA kr (CA CB + ab) t (2-5)

Bill Moschella has contributed a number of Expert Tutorials on sound-related topics. His biographical information can be found (together with his sound advice) in 32, Optimizing Flash Sound for Export. The Flash 5 Publish Settings includes a tab for both Windows and Macintosh Projectors, which publish self-inclusive Stand-alone Players. When published as such, these are actually applications/programs. These players enable viewers to see your Flash movies without worrying about downloading the latest version of the Flash Player. While the default Flash .SWF format is cross-platform, these projectors have either a Macintosh or a Windows version.

1. Choose File Open (or press +O/Ctrl+O). The Open File dialog appears. 2. From the Show pop-up menu /Files of type drop-down list, choose XML Data Source. The Specify XML and XSL Options dialog appears. (See Figure 21-6.)