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end of the nite line is given by [19] q n 1 XXX Z0 n n 1 j ! Vfin ; t 2Vinf ; t 2VS e r= 2l t 1 i n i j Z0 RS i!j! n i ! n 1 i 0 j 0 ( ! i j =2 p q ! p t 2n 1 lc 1 p Ii j s t2 2n 1 lc 2 1 t 2n 1 lc p ! i j k =2 q ! 1 X t 2n 1 lc p p Ii j k s t2 2n 1 lc 2 t 2n 1 lc k 1 ) p 4 1 2 k 1 u0 t 2n 1 lc 3:8:20 where q, de ned earlier as the maximum re ection number for a given time, can be written as a function of time as ( ) t 1:0 3:8:21 q 0:5 p 1:0 x lc with the notation hxi representing the decimal truncation of x, that is, h2:3i h2:8i 2: For the special case when the driving source resistance RS is equal to the characteristic impedance of the lossless line Z0 and the re ection coef cient becomes zero, the voltage at the end of the nite line is given by q X Vfin ; t 2Vinf ; t VS e r= 2l t 1 n p !n=2 q ! p t 2n 1 lc p In s t2 2n 1 lc 2 t 2n 1 lc p ! n k =2 1 X t 2n 1 lc p : t 2n 1 lc k 1 ) q ! n p p o 2 2n 1 lc 2 4 0k 1 In k s t u0 t 2n 1 lc 3:8:22 Comparisons of the normalized end-of-line voltages obtained by the compact expression (3.



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One needs Cage(h) to be able to catch all properly placed HSs with up to h hexagons However, it turns out that the beasts are not that wild Almost all hexagonal systems with h hexagons appear in Cage(h 1) This allows a signi cant speedup due to the reduction in the search space Those HSs that cannot be properly placed in Cage(h 1) can easily be enumerated (see Exercise 3) Therefore, we can restrict our attention to Cage(h 1), when dealing with hexagonal systems with h hexagons Let p and q be the smallest x- and y-coordinates (respectively) of all (centers of) hexagons of an HS that is properly placed in Cage(h 1) Hexagons with coordinates (p, 0) and (0, q) (with respect to the coordinate system of the cage) are named key hexagons.





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Taking the limit n -+ 00, we find S(n) + (1 - a)- . This result is known as Amdahl s law and states that the speed-up gained when using multiple processors is limited by the inverse of the fraction of the task that can only be performed sequentially. As an example, we consider Q = 90%. We then find that the best we can do is to reduce the completion at most lim,,, time with a factor 10, i.e., lim,,, T(n) = t/10, and the speed-up is 0 S(n) = 10.

820) with those obtained by HSPICE with 1, 10, 50, and 500 lumped RLC elements are shown in Fig 385 [19] For these comparisons, the interconnection metal is assumed to be copper surrounded by a low-k dielectric The various interconnection parameters are as follows: Interconnection length 36 cm Interconnection cross section 21 mm 21 mm Resistance per unit length 379 /cm (.

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Let H(p, q) denote the set of all HSs with h hexagons that are properly placed in Cage(h 1) and their key hexagons on x- and y-axes have coordinates (p, 0) and (0, q), respectively Figure 25 shows one element of H(4, 2) The family {H(p, q) : 0 p h 2, 0 q h 2} is a partition of the set of all hexagonal systems that are well placed in Cage(h 1) Because of symmetry, it can be veri ed that |H(p, q)| = |H(q, p)|, for all p, q {0, 1, , h 2} Thus, the job of enumeration of all properly placed hexagons is reduced to determining |H(p, q)| for all p q Given the numbers 0 p q h 2 and Cage(h 1), determining |H(p, q)| reduces to generating all hexagons systems from H(p, q) We do that by generating their boundary line.

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FIGURE 4.2.8 (a) Crosstalk waveforms for different values of signal source resistance Rs . (b) Crosstalk amplitude versus Rs . (From [5]. # 1984 by IEEE.)

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