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The additive function can be somewhat cumbersome as the years of life of depreciable asset increase. Both methods determine the denominator, which represents 100 percent of the amount to be depreciated. The letter n in the equation represents the number of years in a depreciable asset s life: n(n 2 1) 5(5 2 1) 5 2 6 30 2 15 is the denominator
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(Hint: Write pn as the average of n empirical mass functions with each of the n samples deleted in turn.) 3.13 Calculation of typical set . To clarify the notion of a typical set (n) A(n) and the smallest set of high probability B , we will calculate the set for a simple example. Consider a sequence of i.i.d. binary random variables, X1 , X2 , . . . , Xn , where the probability that Xi = 1 is 0.6 (and therefore the probability that Xi = 0 is 0.4). (a) Calculate H (X). (b) With n = 25 and = 0.1, which sequences fall in the typical set A(n) What is the probability of the typical set How many elements are there in the typical set (This involves computation of a table of probabilities for sequences with k 1 s, 0 k 25, and nding those sequences that are in the typical set.) (c) How many elements are there in the smallest set that has probability 0.9 (d) How many elements are there in the intersection of the sets in parts (b) and (c) What is the probability of this intersection
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Thus, the lemma is satis ed for x = 1. By examination, it is clear that the inequality is also satis ed for x = 0. By differentiation, it is easy to see that gy (x) = (1 xy)n is a convex function of x, and hence for 0 x 1, we have (1 xy)n = gy (x) (1 x)gy (0) + xgy (1) = (1 x)1 + x(1 y) 1 x + xe
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 Input voltage transient L(di/dt) response to HBM and MM pulse;  CDM transient response (precharged VDD power rail) leads to voltage overshoot and resonance oscillation of cancellation network. As a second alternative ESD network, the inductor can be substituted for the ESD diode to the ground reference (Figure 2.20); In the rst case, the ESD inductor element is placed between the input node and the VDD power supply node. The advantages of the diode/ inductor implementation are as follows [27 29]:  Elimination of the ESD diode (e.g., diode to VSS) reducing the total capacitance load and design area.  Elimination of ESD diode capacitance requires larger shunt impedance with reduced impact on RF performance. The disadvantages of this network are as follows:  Inductor area;  ESD robustness limited to the inductor coil ESD robustness;  Input voltage transient L(di/dt) response to HBM and MM pulse;  CDM transient response (precharged VSS power rail) initiates voltage undershoot and resonance oscillation. An ESD RF design practice, known as the cancellation method, is as follows:  In an RF application, an ESD inductor element can be chosen such that the combined capacitance load of an input pad and the ESD diodes form an LC resonance cancellation circuit.
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Illustrated TCP/IP by Matthew G. Naugle Wiley Computer Publishing, John Wiley & Sons, Inc. ISBN: 0471196568 Pub Date: 11/01/98
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Measurement and Methodological Issues
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