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182                    Fundamentals of Probability and Statistics for Engineers

                     Table 6.2 Comparison of the observed and theoretical
                     distributions of flying-bomb hits, for Example 6.14
                                               k
                    n k
                           0       1        2      3       4       5

                    n o    229     211      93     35      7     1
                     k
                    n p    226.7   211.4    98.5   30.6    7.1   1.6
                     k
           volumes, and if it is reasonable to assume that the probability of finding k flaws in
           any region depends only on the volume and not on the shape of the region.
             Other physical situations in which the Poisson distribution is used include
           bacteria counts on a Petri plate, the distribution of airplane-spread fertilizers
           in a field, and the distribution of industrial pollutants in a given region.

             Example 6.14. A good example of this application is the study carried out by
           Clark (1946) concerning the distribution of flying-bomb hits in one part of London
                                                                        2
           during World War 2. The area is divided into 576 small areas of 0.25 km each.
           In  Table  6.2,  the  number n k  of  areas  with  exactly  k  hits  is  recorded  and
           is compared with the predicted number based on a Poisson distribution, with
            t ˆ  number  of total hits per number  of areas ˆ  537/576 ˆ  0.932. We see an
           excellent agreement between the predicted and observed results.


           6.3.2  THE  POISSON  APPROXIMATION  TO  THE  BINOMIAL
                 DISTRIBUTION


           Let X  be a random variable having the binomial distribution with
                                  n   k     n k

                          p …k†ˆ     p …1   p†  ;  k ˆ 0; 1; ... ; n:    …6:51†
                           X
                                  k
           Consider the case when n !1,and p !  0, in such a way that np ˆ    remains

           fixed. We note that  is the mean of X, which is assumed to remain constant. Then,
                                 n    k       n k

                        p …k†ˆ          1        ;  k ˆ 0; 1; ... ; n:   …6:52†
                         X
                                 k  n       n
           As n !1  , the factorials n! and (n    k)! appearing in the binomial coefficient
           can be approximated by using the Stirling’s formula [Equation (4.78)]. We also
           note that
                                             c n

                                                   c
                                     lim 1 ‡    ˆ e :                    …6:53†
                                    n!1      n
           Using these relationships in Equation (6.52) then gives, after some manipulation,







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