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Unit 7: Simulation of Queuing System (I)



            It can be seen that, in general                                                       Notes

                         
            dq (t)  q  (t) q (t)
              k     k 1   k
                     
              dt        
            We have already solved this differential equation for k = 1 and 2 (for k = 0, q (t) = f(t)). Solving
                                                                          o
            it successively for k = 3, 4, ... , we will get
                                           k
                                          t   1
                                  q (t)       e  –t /                            ...(5)
                                   k
                                             k!
            Expression (5) is known as the Poisson distribution formula. It is one of the most important and
            widely  encountered  distributions.  Curves  for  q (t)  for  several  values  of  k  are  shown  in
                                                     k
            Figure 7.5. Note that for k = 0, we get the negative exponential curve,
                                            q (t) = e –t/a  = f(t)
                                             0
                                      Figure  7.5: Poisson  Distribution



















            We have thus seen that if the interarrival  time is distributed exponentially,  the number  of
            arrivals is given by Poisson distribution. Therefore, the two terms negative exponential arrival
            or Poisson arrival are often used interchangeably. It should be emphasized here that Poisson
            arrival pattern is just one of many possible arrival patterns in a queueing situation. It results
            from the three assumptions that (i) the successive arrivals are statistically independent of each
            other, that (ii) there is a long-term inter-arrival time constant ex, and that (iii) the probability of
            an arrival taking place during a time interval h is directly proportional to h.

            Exponential service time: Let us make similar assumptions about the servicing process, namely,
            (i) the statistical independence of successive servicings, (ii) the long-term constancy of service
            time, and (iii) the probability of completing the .service for a customer during a time interval h
            is proportional to h. Therefore, as in the case of interarrival time, we will get
                                  g(t) = e–t/                                       ...(6)

            where g(t) is the probability that a customer's service could not be completed in time t, (given
            that the previous customer's service was completed at time zero) and  is the long-term average
            service  time.
            Operating characteristics: Now we have completely defined the four parameters of the queueing
            system. These are (i) Poisson arrival pattern, (ii) negative exponential service times, (iii) a single
            server, and (iv) the first-come-first-served queue discipline. For this particular queueing system
            we will now derive some interesting and useful statistics about the system:






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