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138                    Fundamentals of Probability and Statistics for Engineers

           determination of the distribution Y  when all X j , j ˆ  1, 2, ... , n, are continuous
           random variables. Consider the transformation

                                    Y ˆ g…X 1 ; ... ; X n †             …5:40†

           where the joint distribution of X 1 , X 2 ,. . . , and X n  is assumed to be specified in
           term  of their  joint  probability density function  (jpdf),  f  (x 1 ,..., x n ),  or
                                                            X 1 ...X n
                                                               (x 1 ,..., x n ).  In  a
           their  joint  probability distribution  function  (JPDF), F X 1 ...X n
           more compact notation, they can be written as f ( x) and F X ( x), respectively,
                                                     X
           where X is an n-dimensional random vector with components X 1 , X 2 ,..., X n .

             The starting point of the derivation is the same as in the single-random-
           variable  case;  that  is,  we  consider  F Y   (y) ˆ  P(Y    y).  In  terms  of  X, this
           probability is equal to P[g( X)    y]. Thus:
                              F Y …y†ˆ P…Y   y†ˆ P‰g…X†  yŠ
                                                                        …5:41†
                                   ˆ F X ‰x : g…x†  yŠ:

           The final expression in the above represents the JPDF of X for which the
           argument x  satisfies g( x)      . In terms of  f ( x), it is given by
                                  y
                                                X
                                             Z    Z
                             F X ‰x : g…x†  yŠˆ       f …x†dx           …5:42†
                                                     X
                                            …R n : g…x† y†

           where the limits of the integrals are determined by an n-dimensional region R n
           within  which  g( x)    y is satisfied. In  view of Equations (5.41) and  (5.42), the
           PDF of Y , F Y   (y), can be determined by evaluating the n-dimensional integral in
           Equation (5.42). The crucial step in this derivation is clearly the identification
               n
           of  R , which must be carried out on a problem-to-problem basis. As n becomes
           large, this can present a formidable obstacle.
             The procedure outlined above can be best demonstrated through examples.
             Example 5.11. Problem: let Y ˆ  X 1 X 2 . Determine the pdf of Y  in terms of




           f   (x 1 , x 2 ).
            X 1 X 2
             Answer: from Equations (5.41) and (5.42), we have
                                       Z Z
                            F Y …y†ˆ        f   …x 1 ; x 2 †dx 1 dx 2 :  …5:43†
                                             X 1 X 2
                                     2
                                    …R : x 1 x 2  y†
           The equation  x 1 x 2 ˆ  y is graphed  in  Figure 5.16 in  which  the shaded  area
                      2
           represents  R , or x 1 x 2    y.  The  limits  of  the  double  integral  can  thus  be
           determined and Equation (5.43) becomes






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