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Fundamentals of Probability and Statistics for Engineers

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Functions <strong>of</strong> R<strong>and</strong>om Variables 123is the inverse function <strong>of</strong> g(x), or the solution <strong>for</strong> x in Equation (5.5) in terms <strong>of</strong>y. Hence,F Y …y† ˆP…Y y† ˆP‰g…X† yŠ ˆP‰X g 1 …y†Š ˆ F X ‰g 1 …y†Š:…5:7†Equation (5.7) gives the relationship between the PDF <strong>of</strong> X <strong>and</strong> that <strong>of</strong> Y , ourdesired result.The relationship between the pdfs <strong>of</strong> X <strong>and</strong> Y are obtained by differentiatingboth sides <strong>of</strong> Equation (5.7) with respect to y. We have:f Y …y† ˆdF Y…y†dyˆ ddy fF X‰g 1 …y†Šg ˆ f X ‰g 1 …y†Š dg 1 …y†: …5:8†dyIt is clear that Equations (5.7) <strong>and</strong> (5.8) hold not only <strong>for</strong> the particulartrans<strong>for</strong>mation given by Equation (5.5) but <strong>for</strong> all continuous g(x) that are strictlymonotonic increasing functions <strong>of</strong> x, that is, g(x 2 )> g(x 1 )whenever x 2 >x 1 .Consider now a slightly different situation in which the trans<strong>for</strong>mation isgiven byY ˆ g…X† ˆ 2X ‡ 1: …5:9†Starting again with F Y (y) ˆ P(Y y), <strong>and</strong> reasoning as be<strong>for</strong>e, the regionY y in the range space R Y is now mapped into the region X > g 1 (y), asindicated in Figure 5.3. Hence, we have in this caseF Y …y† ˆP…Y y† ˆP‰X > g 1 …y†Šˆ 1 P‰X g 1 …y†Š ˆ 1 F X ‰g 1 …y†Š:…5:10†yy =–2x +1yxx = g –1 (y)= 1–y2Figure 5.3 Trans<strong>for</strong>mation defined by Equation (5.9)TLFeBOOK

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