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7. Point Estimation  343

                           from anthropometry and astronomy. The method of moments was introduced
                           by Pearson (1902).
                              The methodology is very simple. Suppose that θθ θθ θ = (θ , ..., θ ). Derive the
                                                                                k
                                                                           1
                           first k theoretical moments of the distribution f(x; θθ θθ θ) and pretend that they are
                           equal to the corresponding sample moments, thereby obtaining k equations in
                           k unknown parameters θ , ..., θ . Next, simultaneously solve these k equa-
                                                      k
                                                1
                           tions for θ , ..., θ . The solutions are then the estimators of ? , ..., ? . Refer
                                    1
                                          k
                                                                               1
                                                                                     k
                           back to the Section 2.3 as needed. To be more specific, we proceed as fol-
                           lows: We write










                           Now, having observed the data X = x, the expressions given in the rhs of
                           (7.2.1) can all be evaluated, and hence we will have k separate equations in k
                           unknown parameters θ , ..., θ . These equations are solved simultaneously.
                                                    k
                                              1
                           The following examples would clarify the technique.

                                Often  is written for an estimator of the unknown parameter θθ θθ θ.
                              Example 7.2.1 (Example 6.2.8 Continued) Suppose that X , ..., X  are iid
                                                                                     n
                                                                               1
                                                                      χ
                           Bernoulli(p) where p is unknown, 0 < p < 1. Here   = {0, 1}, θ = p and Θ =
                           (0, 1). Observe that  η  =  η (θ) =  E [X ] =  p, and let us pretend that
                                                1    1      p  1
                                                the sample mean. Hence,      would be the esti-
                           mator of p obtained by the method of moments. We write       which
                           happens to be sufficient for the parameter p too.!
                              Example 7.2.2 (Example 6.2.10 Continued) Suppose that X , ..., X  are iid
                                                                                     n
                                                                                1
                                                                               2
                           N(µ, σ ) where µ, σ  are both unknown with n ≥ 2, θθ θθ θ = (µ, σ ), θθ θθ θ  = µ, θ  =
                                            2
                                2
                                                                                         2
                                                                                  1
                                                       χ
                           σ , −∞ < µ < ∞, 0 < σ < ∞. Here   = ℜ and Θ = ℜ × ℜ . Observe that η  =
                                                                           +
                            2
                                                                                         1
                           η (θ , θ ) = E [X ] = µ and                          so that (7.2.1)
                            1  1  2   ?  1
                           would lead to the two equations,
                           After solving these two equations simultaneously for µ and σ , we obtain
                                                                                 2
                           the estimators      and                                     .  The
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