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2. Expectations of Functions of Random Variables  83

                           which was exactly the same integral evaluated in (2.3.13). In other words,
                           from (2.3.14) we can immediately claim that M (t) = exp(1/2t ). Thus, one
                                                                                2
                                                                    Y
                           can rewrite (2.3.15) as follows:


                              Now, log(M (t)) = tµ + 1/2t σ  so that dM (t)/dt = (µ + tσ ) M (t). Hence,
                                                       2
                                                                              2
                                                     2
                                        X
                                                                 X
                                                                                  X
                           dM (t)/dt, when evaluated at t = 0, reduces to η  = µ because one has
                                                                       1
                              X
                           M (0) = 1.
                             X
                              Also, using the chain rule of differentiation we have d M (t)/dt  = σ M (t) +
                                                                                 2
                                                                                     2
                                                                          2
                                                                                       X
                                                                            X
                           (µ + tσ )  M (t) so that d  M (t)/dt , when evaluated at t = 0, reduces to η  = σ 2
                                 2 2
                                               2
                                                       2
                                                                                       2
                                     X
                                                  X
                           + µ . In view of the Theorem 2.3.1, we can say that µ is the mean of X and V(X)
                              2
                                                   2
                                               2
                                2
                           = E(X ) – µ  = σ  + µ  – µ  = σ . These answers were verified earlier in (2.2.30).
                                    2
                                            2
                                        2
                              One can also easily evaluate higher order derivatives of the mgf. In view of
                                                             k
                           the Theorem 2.3.1 one can claim that d  M (t)/dt  with k = 3 and 4, when
                                                                     k
                                                                X
                                                                          4
                                                             3
                           evaluated at t = 0, will reduce to η  or E(X ) and η  or E(X ) respectively. Then,
                             α
                                                                   4
                                                       3
                           in order to obtain the third and fourth central moments of X, one should pro-
                           ceed as follows:
                           by the Theorem 2.2.1. Similarly,
                           Look at the related Exercises 2.3.1-2.3.2.
                              Example 2.3.3 Suppose that Z is the standard normal variable. How should
                           one directly derive the expression for E(|Z|)? Here, the mgf of Z from (2.3.14) is
                           not going to be of much help. Let us apply the Definition 2.2.3 and proceed as
                           follows. As before, we substitute u = –z when z < 0, and express E(|Z|) as
                           In the last step of (2.3.19), one immediately realizes that the two integrals are
                           really the same that is,                                     and
                           hence one has
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