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Consider an rv X with mean \({\rm{\mu }}\) and standard deviation \({\rm{\sigma }}\), and let g(X) be a specified function of X. The first-order Taylor series approximation to g(X) in the neighborhood of \({\rm{\mu }}\) is \({\rm{g(X)}} \approx {\rm{g(\mu ) + g'(\mu ) \times (X - \mu )}}\) The right-hand side of this equation is a linear function of X. If the distribution of X is concentrated in an interval over which is approximately linear (e.g., \(\sqrt {\rm{x}} \) is approximately linear in (1, 2)), then the equation yields approximations to E(g(X)) and V(g(X)).

a. Give expressions for these approximations. (Hint: Use rules of expected value and variance for a linear function \({\rm{aX + b}}\).)

b. If the voltage v across a medium is fixed but current, I is random, then resistance will also be a random variable related to I by \({\rm{R = v/I}}\). If \({{\rm{\mu }}_{\rm{I}}}{\rm{ = 20}}\) and \({{\rm{\sigma }}_{\rm{I}}}{\rm{ = }}{\rm{.5}}\), calculate approximations to \({{\rm{\mu }}_{\rm{R}}}\) and \({{\rm{\sigma }}_{\rm{R}}}\).

Short Answer

Expert verified

(a) \({\rm{E(g(x)) = g(\mu )}}\) and \({\rm{V(g(x)) = }}{\left( {{\rm{g'(\mu )}}} \right)^{\rm{2}}}{\rm{ \times }}{{\rm{\sigma }}^{\rm{2}}}\) is expressions for these approximately.

(b) \({{\rm{\mu }}_{\rm{R}}}{\rm{ = }}\frac{{\rm{v}}}{{{\rm{20}}}}\) and \({{\rm{\sigma }}_{\rm{R}}}{\rm{ = }}\frac{{\rm{v}}}{{{\rm{800}}}}\).

Step by step solution

01

Definition of Standard deviation

The standard deviation is a measurement of a set of values' variation or dispersion. A low standard deviation implies that the values are close to the set's mean (also known as the anticipated value), whereas a high standard deviation shows that the values are spread out over a larger range.

02

Determining expression for the approximation

(a) X is a rv with a mean of \({\rm{\mu }}\) and a standard deviation of \({\rm{\sigma }}\). By definition, we may then write

\({\rm{\mu = E(X)}}\)

\({{\rm{\sigma }}^{\rm{2}}}{\rm{ = E}}\left( {{{{\rm{(X - \mu )}}}^{\rm{2}}}} \right)\)

It's also assumed that g(X) is a defined function of X, with an approximation near \({\rm{\mu }}\) as:

\({\rm{g(X) = g(\mu ) + g'(\mu ) \times (X - \mu )}}\)

This expression is comparable to \({\rm{aX + b}}\) because \({\rm{g(\mu )}}\) and \({\rm{g'(\mu )}}\) are constants. The mean can thus be expressed as:

\({\rm{E(g(X)) = E(g(\mu )) + E}}\left( {{\rm{g'(\mu ) \times (X - \mu )}}} \right)\)

\({\rm{ = g(\mu ) + g'(\mu ) \times E((X - \mu ))}}\)

\({\rm{ = g(\mu ) + g'(\mu ) \times (E(X) - E(\mu ))}}\)

\({\rm{ = g(\mu ) + g'(\mu ) \times (\mu - \mu )}}\)

\({\rm{E(g(X)) = g(\mu )}}\)

03

Determining representation of g(X) variance

\({\rm{E}}\left( {{\rm{g(X}}{{\rm{)}}^{\rm{2}}}} \right){\rm{ = E}}\left( {{{\left( {{\rm{g(\mu ) + g'(\mu ) \times (X - \mu )}}} \right)}^{\rm{2}}}} \right)\)

\({\rm{ = E}}\left( {{{{\rm{(g(\mu ))}}}^{\rm{2}}}{\rm{ + 2 \times g(\mu ) \times g'(\mu ) \times (X - \mu ) + }}{{\left( {{\rm{g'(\mu )}}} \right)}^{\rm{2}}}{{{\rm{(X - \mu )}}}^{\rm{2}}}} \right)\)

\({\rm{ = E}}\left( {{{{\rm{(g(\mu ))}}}^{\rm{2}}}} \right){\rm{ + E}}\left( {{\rm{2 \times g(\mu ) \times g'(\mu ) \times (X - \mu )}}} \right){\rm{ + E}}\left( {{{\left( {{\rm{g'(\mu )}}} \right)}^{\rm{2}}}{{{\rm{(X - \mu )}}}^{\rm{2}}}} \right)\)

\({\rm{ = (g(\mu )}}{{\rm{)}}^{\rm{2}}}{\rm{ + 2 \times g(\mu ) \times g'(\mu ) \times E((X - \mu )) + }}{\left( {{\rm{g'(\mu )}}} \right)^{\rm{2}}}{\rm{E}}\left( {{{{\rm{(X - \mu )}}}^{\rm{2}}}} \right)\)

\({\rm{ = (g(\mu )}}{{\rm{)}}^{\rm{2}}}{\rm{ + 0 + }}{\left( {{\rm{g'(\mu )}}} \right)^{\rm{2}}}{\rm{ \times }}{{\rm{\sigma }}^{\rm{2}}}\)

\({\rm{E}}\left( {{\rm{g(X}}{{\rm{)}}^{\rm{2}}}} \right){\rm{ = (g(\mu )}}{{\rm{)}}^{\rm{2}}}{\rm{ + }}{\left( {{\rm{g'(\mu )}}} \right)^{\rm{2}}}{\rm{ \times }}{{\rm{\sigma }}^{\rm{2}}}\)

As a result, g(X) variance can be represented as:

\({\rm{V(g(x)) = E}}\left( {{\rm{g(X}}{{\rm{)}}^{\rm{2}}}} \right){\rm{ - E(g(X)}}{{\rm{)}}^{\rm{2}}}\)

\({\rm{ = }}\left( {{{{\rm{(g(\mu ))}}}^{\rm{2}}}{\rm{ + }}{{\left( {{\rm{g'(\mu )}}} \right)}^{\rm{2}}}{\rm{ \times }}{{\rm{\sigma }}^{\rm{2}}}} \right){\rm{ - (g(\mu )}}{{\rm{)}}^{\rm{2}}}\)

\({\rm{V(g(x)) = }}{\left( {{\rm{g'(\mu )}}} \right)^{\rm{2}}}{\rm{ \times }}{{\rm{\sigma }}^{\rm{2}}}\)

04

Calculating approximation for \({{\rm{\mu }}_{\rm{R}}}\) and  \({{\rm{\sigma }}_{\rm{R}}}\)

(b) Assume that I denote the current flowing through a medium, and that:

\({{\rm{\mu }}_{\rm{I}}}{\rm{ = 20}}\)

\({{\rm{\sigma }}_{\rm{I}}}{\rm{ = 0}}{\rm{.5}}\)

R represents the medium's resistance, and

\({\rm{R = }}\frac{{\rm{v}}}{{\rm{I}}}\)

I is equivalent to X, and R is equivalent to g(X), therefore

\({\rm{g(I) = R = }}\frac{{\rm{v}}}{{\rm{I}}}\)

\({\rm{g'(I) = }}\frac{{{\rm{ - v}}}}{{{{\rm{I}}^{\rm{2}}}}}\)

The mean and variance of R can be approximated using the data from the preceding section:

\({{\rm{\mu }}_{\rm{R}}}{\rm{ = g}}\left( {{{\rm{\mu }}_{\rm{I}}}} \right){\rm{ = g(20)}}\)

\({{\rm{\mu }}_{\rm{R}}}{\rm{ = }}\frac{{\rm{v}}}{{{\rm{20}}}}\)

\({{\rm{\sigma }}_{\rm{R}}}{\rm{ = g'(\mu ) \times \sigma = g'(20) \times (0}}{\rm{.5)}}\)

\({{\rm{\sigma }}_{\rm{R}}}{\rm{ = }}\frac{{\rm{v}}}{{{\rm{2}}{{\rm{0}}^{\rm{2}}}}}{\rm{ \times (0}}{\rm{.5)}}\)

\({{\rm{\sigma }}_{\rm{R}}}{\rm{ = }}\frac{{\rm{v}}}{{{\rm{800}}}}\)

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Most popular questions from this chapter

As in the case of the Weibull and Gamma distributions, the lognormal distribution can be modified by the introduction of a third parameter \({\rm{\gamma }}\) such that the pdf is shifted to be positive only for \({\rm{\chi > \gamma }}\)The article cited in Exercise \({\rm{4}}{\rm{.39}}\)suggested that a shifted lognormal distribution with shift (i.e., threshold) \({\rm{ = 1}}{\rm{.0}}\), mean value \({\rm{ = 2}}{\rm{.16, }}\), and standard deviation \({\rm{ = 1}}{\rm{.03}}\) would be an appropriate model for the \({\rm{rv X = }}\) maximum-to-average depth ratio of a corrosion defect in pressurized steel.

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\({\rm{f(x;\theta ,\tau ) = }}\left\{ {\begin{array}{*{20}{c}}{\frac{{\rm{\theta }}}{{\rm{\tau }}}{{{\rm{(1 - x/\tau )}}}^{{\rm{\theta - 1}}}}}&{{\rm{0}} \le {\rm{x < \tau }}}\\{\rm{0}}&{{\rm{ otherwise }}}\end{array}} \right.\)

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