Page 377 - A First Course In Stochastic Models
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372             ALGORITHMIC ANALYSIS OF QUEUEING MODELS

                Thus we have a computationally useful algorithm for the waiting-time distribution
                when the probabilities π j can be efficiently computed. These probabilities are the
                unique solution to the equilibrium equations

                                          ∞

                                    π j =   π k p kj ,  j = 0, 1, . . .      (9.5.2)
                                         k=0
                together with the normalizing equation    j=0 j = 1, where the p ij are the one-step
                                                 ∞
                                                    π
                transition probabilities of the Markov chain {X n }. The p ij are easily found. Since
                service completions of phases occur according to a Poisson process with rate µ as
                long as the server is busy, it is readily seen that for any i ≥ 0
                              m                    i+k−j
                                        ∞  −µt  (µt)
                     p ij =         q k   e             a(t) dt,  1 ≤ j ≤ i + m,
                                       0      (i + k − j)!
                          k=max(j−i,1)
                where a(t) denotes the probability density of the interarrival time. The geometric
                tail approach from Section 3.4.2 can be used to reduce the infinite system of linear
                equations (9.5.2) to a finite system of linear equations. To see that

                                        π j+1
                                             ∼ η  as j → ∞                   (9.5.3)
                                         π j
                for some constant 0 < η < 1, note that for any i ≥ 0 the one-step transition
                probability p ij equals 0 for j > i + m and depends on i and j only through the
                difference j − i for j ≥ 1. Next we can apply a general result from Section 3.4.2
                to obtain (9.5.3). Using the expression for p ij , the equation (3.4.9) reduces after
                some algebra to
                                                        m
                                      ∞

                               m         −µ(1−w)t             m−i
                              w −       e       a(t) dt   q i w  = 0.        (9.5.4)
                                     0
                                                       i=1
                The decay factor η is the largest root on (0,1) of this equation. By replacing π j
                for j ≥ M by π M η j−M  for an appropriately chosen integer M, we obtain a finite
                system of linear equations.

                9.5.2 Coxian-2 Services

                Suppose that the service time S of a customer has a Coxian-2 distribution with
                parameters (b, µ 1 , µ 2 ). That is, S is distributed as U 1 with probability 1 − b and
                S is distributed as U 1 + U 2 with probability b, where U 1 and U 2 are indepen-
                dent exponentials with respective means 1/µ 1 and 1/µ 2 . Then the waiting-time
                distribution function W q (x) allows for the explicit expression
                                1 − W q (x) = a 1 e −η 1 x  + a 2 e −η 2 x ,  x ≥ 0,  (9.5.5)
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