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Simulation and Modelling



                      Notes         The curves for Eqs. (3) and (4) are shown in Figure 7.4. These are the curves for the exponential
                                    distribution. The curve in Figure 7.4(b) gives the probability that the next customer arrives by
                                    time t, given that the preceding customer arrived at time zero. Customarily the inverse of the
                                    average interarrival time is denoted by , which is nothing but the average number of customers
                                    arriving at the system per unit time.

                                                          Figure 7.4  : Interarrival  Time of  Customers























                                    Having found that the interarrival time is governed by exponential distribution, we will now
                                    find the probability that exactly k customers have arrived during the time interval t (assuming
                                    that no customer had arrived by time t = 0).

                                    Let q (t) be the probability that exactly k arrivals take place between the start time zero and t, for
                                        k
                                    k = I, 2, 3, .... Then we can write
                                    q (t + h) = (Probability that no arrivals take place between time zero and t). (probability that one
                                     l
                                    arrival takes place during time h) + (probability that one arrival takes place between time zero
                                    and t) . (probability that no arrivals take place during time h)

                                         h         h 
                                       f(t).    q (t). 1   
                                                 
                                             1
                                                   
                                    where f(t), as previously determined, is e  –t/ .
                                    Therefore,
                                            
                                        
                                     q (t h) q (t)  1
                                      1       1
                                                   [f(t) q (t)]
                                                        
                                                          1
                                          h        
                                    as h  0 this expression becomes
                                     dq (t)    1  [f(t) q (t)]
                                       1
                                                
                                      dt          1
                                    The solution of this differential equation can easily be seen to be
                                          1      1
                                     q (t)   e   t /a    f(t)
                                      1
                                                
                                    Extending the same argument (since at most one arrival can take place in the interval h) we get
                                             2
                                            t   1
                                     q (t)       .f(t)
                                      2
                                               2!
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