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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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30.16 EXERCISES30.18 A particle is confined to the one-dimensional space 0 ≤ x ≤ a, <strong>and</strong> classicallyitcanbeinanysmallintervaldx with equal probability. However, quantummechanics gives the result that the probability distribution is proportional tosin 2 (nπx/a), where n is an integer. Find the variance in the particle’s positionin both the classical <strong>and</strong> quantum-mechanical pictures, <strong>and</strong> show that, althoughthey differ, the latter tends to the <strong>for</strong>mer in the limit of large n, in agreementwith the correspondence principle of physics.30.19 A continuous r<strong>and</strong>om variable X has a probability density function f(x); thecorresponding cumulative probability function is F(x). Show that the r<strong>and</strong>omvariable Y = F(X) is uni<strong>for</strong>mly distributed between 0 <strong>and</strong> 1.30.20 For a non-negative integer r<strong>and</strong>om variable X, in addition to the probabilitygenerating function Φ X (t) defined in equation (30.71), it is possible to define theprobability generating function∞∑Ψ X (t) = g n t n ,where g n is the probability that X>n.(a) Prove that Φ X <strong>and</strong> Ψ X are related byΨ X (t) = 1 − Φ X(t).1 − t(b) Show that E[X] is given by Ψ X (1) <strong>and</strong> that the variance of X can beexpressed as 2Ψ ′ X (1) + Ψ X(1) − [Ψ X (1)] 2 .(c) For a particular r<strong>and</strong>om variable X, the probability that X>nis equal toα n+1 ,with0

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