Page 95 - A First Course In Stochastic Models
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TRANSIENT ANALYSIS                       87

                time between the arrival epochs of the nth and (n + 1)th customer and let C n
                denote the number of customers served during the interarrival time A n . Note that
                X n+1 = X n + 1 − C n . The probability distribution of C n obviously depends on
                X n (= the number of customers seen by the nth arrival). The easiest way to find
                the probability distribution of C n is to use the observation that service completions
                occur according to a Poisson process with rate µ as long as the server is busy.
                This observation is a consequence of the assumption of exponentially distributed
                service times and the relation between the Poisson process and the exponential
                distribution. By conditioning on the interarrival time A n and using the law of total
                probability, we find for each state i that

                    p ij = P {X n+1 = j | X n = i}

                           ∞
                       =     P {i + 1 − j service completions during A n | A n = t}a(t) dt
                          0
                           ∞      (µt)
                                      i+1−j
                       =     e −µt         a(t) dt,  1 ≤ j ≤ i + 1.          (3.1.2)
                          0      (i + 1 − j)!
                This formula does not hold for j = 0. Why not? The probability p i0 is easiest to
                compute from
                                            i+1

                                   p i0 = 1 −  p ij ,  i = 0, 1, . . . .
                                            j=1
                Obviously, p ij = 0 for j > i + 1 for each state i.



                                  3.2   TRANSIENT ANALYSIS

                This section deals with the transient analysis of the Markov chain {X n , n =
                0, 1, . . . } with state space I and one-step transition probabilities p ij for i, j ∈ I.
                We first show how the one-step transition probabilities determine the probability of
                going from state i to state j in the next n steps. The n-step transition probabilities
                are defined by
                                   (n)
                                 p   = P {X n = j | X 0 = i},  i, j ∈ I
                                   ij
                                           (1)
                for any n = 1, 2, . . . Note that p  = p ij . It is convenient to define
                                           ij

                                         (0)   1   if j = i,
                                        p   =
                                         ij    0   if j  = i.
                Theorem 3.2.1 (Chapman–Kolmogoroff equations) For all n, m = 0, 1, . . . ,

                                     (n+m)      (n) (m)
                                   p      =    p  p   ,  i, j ∈ I.           (3.2.1)
                                     ij         ik  kj
                                            k∈I
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