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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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30.5 PROPERTIES OF DISTRIBUTIONS|x − µ| ≥c. From (30.48), we find that∫∫σ 2 ≥ (x − µ) 2 f(x) dx ≥ c 2|x−µ|≥c|x−µ|≥cf(x) dx. (30.49)The first inequality holds because both (x − µ) 2 <strong>and</strong> f(x) are non-negative <strong>for</strong>all x, <strong>and</strong> the second inequality holds because (x − µ) 2 ≥ c 2 over the range ofintegration. However, the RHS of (30.49) is simply equal to c 2 Pr(|X − µ| ≥c),<strong>and</strong> thus we obtain the required inequalityPr(|X − µ| ≥c) ≤ σ2c 2 .A similar derivation may be carried through <strong>for</strong> the case of a discrete r<strong>and</strong>omvariable. Thus, <strong>for</strong> any distribution f(x) that possesses a variance we have, <strong>for</strong>example,Pr(|X − µ| ≥2σ) ≤ 1 4<strong>and</strong> Pr(|X − µ| ≥3σ) ≤ 1 9 .30.5.4 MomentsThe mean (or expectation) of X is sometimes called the first moment of X, sinceit is defined as the sum or integral of the probability density function multipliedby the first power of x. By a simple extension the kth moment of a distributionis defined by{∑µ k ≡ E[X k j]=xk j f(x j) <strong>for</strong> a discrete distribution,∫x k f(x) dx <strong>for</strong> a continuous distribution.(30.50)For notational convenience, we have introduced the symbol µ k to denote E[X k ],the kth moment of the distribution. Clearly, the mean of the distribution is thendenoted by µ 1 , often abbreviated simply to µ, as in the previous subsection, asthis rarely causes confusion.A useful result that relates the second moment, the mean <strong>and</strong> the variance ofa distribution is proved using the properties of the expectation operator:V [X] =E [ (X − µ) 2]= E [ X 2 − 2µX + µ 2]= E [ X 2] − 2µE[X]+µ 2= E [ X 2] − 2µ 2 + µ 2In alternative notations, this result can be written= E [ X 2] − µ 2 . (30.51)〈(x − µ) 2 〉 = 〈x 2 〉−〈x〉 2 or σ 2 = µ 2 − µ 2 1.1147

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