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The first coefficient (on the left) is the first coefficient in the e n ~ o d e r .Thus the coded ~ output streams are

Complexity 0( N ) O(N) 0( N ) 0( N ) 0( N ) 0(g2) Complexity 0 0( N ) 0 1 O(N)

~ e e ~t ~ o is the first example we have met of a class that combines both rol n s ~ c h r o n i ~ access methodsand a thread. We could have implementedit as two ed classes, a purely passive entity which encapsulated the st a t e and se t Speed variables and an active entity with only a run() method. However, this would have been e c e s s a r i l y ~ complex and would lead toadditional methods to set and et the variables. implemented, the class satisfactorily encapsulates the As thread and the methods that control its execution.

The selected table is surrounded by a black border, with sizing handles on the right, bottom, and bottom-right corner (as shown in Figure 13-3), just like a selected graphic.

The operating system for your local development machine may be different from the operating system of your remote server. If so, using the Line Breaks option may cause your HTML to appear incorrectly when viewed through a simple text editor (such as Notepad or vi). The Dreamweaver Code Inspector, however, does render the code correctly.

3. In the Select File dialog box, enter the path and the filename in the File Name text box or click the Browse button to locate the file. Click OK.

2A subgroup H of a group G is normal if g-l H g = H for all g E G. Clearly all Abelian groups are normal. 3 0 r of a normal subgroup in a noncommutative group.

Special dif culties arise in the solution of the ordinary differential equations that arise from the problems discussed in this chapter due to the tendency for modelling cases to be characterised by mixed dynamics. A brief review follows on the nature of the dif culties and their remedies but for more detailed information concerning solution schemes the reader should consult one of the specialist texts on the subject such as Press et al. (2002). In the above, most of the methods have generally reduced to sets of ordinary differential equations or transfer functions each of which, in general, can be expressed in the following form: df = f (t , f ) dt The simplest way to advance a numerical solution over the interval, h, is as follows: f n+1 = f n + hf (tn , f n ) in which n refers to points along the solution continuum. In fact this is Euler s method and is equivalent to the forward-in-space discretisation adopted for the partial discretisation of the distributed heat exchange equations discussed earlier (i.e. Equation. 5.10). In practice, Euler s method is likely to prove insuf ciently accurate as a general method of solution unless a very low value of interval h is used. Additionally, for many of the mixed dynamics problems

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The coef cients a0...j and b0...j in Equation 1.142 are called the weighting factors. Recall that the heat ux at surface 0 of a homogeneous slab of material in response to a unit triangular impulse temperature excitation applied to surface 0 is as given in Equation 1.116, which is reproduced below with the subscripts for the heat ux and temperature dropped for simplicity: q(n) = X (0)T (n) + X (1)T (n - 1) + X (2)T (n - 2) + . . . (1.143)

It is interesting to contrast this update formula with the formula for updating the path metric in the Viterbi algorithm. In the Viterbi algorithm, the path metric is updated by adding the branch metric to the previous path metric. Then the minimum of the path metrics at a state is computed. In the BCJR case, the path metric at ( p ) is multiplied by the branch metric yr ( p , q ) , then the branch metrics are summed at each state. Mapping the operations min + sumsum