Page 60 - A First Course In Stochastic Models
P. 60

THE FORMULA OF LITTLE                      51

                       D n = the amount of time spent by the nth customer in the queue
                            (excluding service time),

                       U n = the amount of time spent by the nth customer in the system
                            (including service time).

                Let us assume that each of the stochastic processes {L q (t)}, {L(t)}, {D n } and {U n }
                is regenerative and has a cycle length with a finite expectation. Then there are
                constants L q , L, W q and W such that the following limits exist and are equal to
                the respective constants with probability 1:


                     1     t
                 lim     L q (u) du = L q  (the long-run average number in queue),
                t→∞ t
                       0
                     1     t
                  lim     L(u) du = L  (the long-run average number in system),
                 t→∞ t  0
                            n
                         1
                     lim      D k = W q  (the long-run average delay in queue per customer),
                     n→∞ n
                           k=1
                            n
                         1
                      lim     U k = W  (the long-run average sojourn time per customer).
                     n→∞ n
                           k=1
                Now define the random variable
                            A(t) = the number of customers arrived by time t,
                It is also assumed that, for some constant λ,

                                       A(t)
                                   lim     = λ   with probability 1.
                                   t→∞  t
                The constant λ gives the long-run average arrival rate of customers. The limit
                λ exists when customers arrive according to a renewal process (or batches of
                customers arrive according to a renewal process with independent and identically
                distributed batch sizes).
                  The existence of the above limits is sufficient to prove the basic relations

                                             L q = λW q                      (2.3.1)

                and
                                              L = λW                         (2.3.2)

                These basic relations are the most familiar form of the formula of Little. The reader
                is referred to Stidham (1974) and Wolff (1989) for a rigorous proof of the formula
                of Little. Here we will be content to demonstrate the plausibility of this result. The
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