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It follows that t m G sX , that is, event e1 at node k q 1 can never occur later than projected according to the queue model. The equality holds only when . w . X x kq1 t s R for t g s y , t m . If event e1 could happen in s , t m , node k would simply repeat its previous operations when it receives the corresponding feedback signal 1.. Buffer overflow will never occur at node k q 1. It can be proven that the backlog in both the fictitious model and the real queue of node k q 1 is upper bounded by the buffer size Bkq1 derived from 7.12.. Suppose that node k q 1 stays in the buffer overflow state SO such that sX G s q . Since it follows from assumptions A2 and A3 that for t g w s q , sX . we have k t y . F R F kq1 t ., only during s y , s q x could the maximum backlog accumulate in both the model and the real queue. Since, according to assumption A1, node k should enforce the peak service rate S at any time, A kq1 s y , s q . F 2 S , it follows from 7.21., 7.22., and 7.12. that for t g s y , s q x,

The only difference is that include() merely raises a PHP warning if the file to be included can t be found, whereas require() raises a fatal error and stops running the script. Use require() if you re including library files that are essential to the running of your application.

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We now consider a classical approach to the numerical solution of (12.9) that we call the nite-difference (FD) method. Note that the method to follow is by no means the only approach. Indeed, the FDTD method to be considered in Section 12.5 is an alternative, and there are still others. Following (12.5) u(xk , tn+1 ) 2u(xk , tn ) + u(xk , tn 1 ) 2 4 u(xk , n ) 2 u(xk , tn ) = (12.93) 12 t 2 2 t 4 for some n [tn 1 , tn+1 ], and u(xk+1 , tn ) 2u(xk , tn ) + u(xk 1 , tn ) h2 4 u( k , tn ) 2 u(xk , tn ) = 2 12 x h2 x 4 for some k [xk 1 , xk+1 ], where xk = kh, tn = n (12.95) (12.94)

The Dynamic option of ZOOM enables you to pan and zoom in one operation. The Aerial View (discussed in the next section) offers more sophisticated options, but the simplicity of ZOOM Dynamic is sometimes just what you need. When you start ZOOM Dynamic, you see the virtual screen area of the drawing in a blue dashed rectangle; this view box represents the drawing extents or limits, whichever is greater. Your current view is bounded in a green, dashed rectangle. Your mouse cursor changes, based on the two modes of ZOOM Dynamic. Each time you click the left mouse button, you switch modes. Here s how the two modes work: Pan mode: The view box contains an X and can move freely around any displayed area of the drawing. Zoom mode: The view box contains an arrow. The left side of the box is fixed at the point where you changed to Zoom mode. As you move the cursor, the box expands or shrinks, letting you zoom to any magnification. When the view box displays the view that you want, click the right mouse button and choose Enter (or press Enter). The command pans and zooms to show that view. Figure 8-3 shows the screen during a ZOOM Dynamic operation.

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This current is small enough not to be dangerous for the cables and transformers, although it can be prejudicial to rotating machines (see section 10.1.2).

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The capability to remesh a patch of elements has been prototyped in the Sierra framework. This capability is planned to enable applications that have large mesh motion, such as Lagrangian explicit dynamics, to remesh severely distorted patches of elements. For example, in Figure 11.20 a patch containing ve severely distorted triangles is remeshed with eight acute triangles.

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