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		<summary type="html">&lt;p&gt;117.216.176.13: /* Example */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Unreferenced|date=December 2009}}&lt;br /&gt;
&amp;lt;!-- ==CDF method== will do this later --&amp;gt;&lt;br /&gt;
In [[probability theory]], it is possible to approximate the [[moment (mathematics)|moments]] of a function &#039;&#039;f&#039;&#039; of a [[random variable]] &#039;&#039;X&#039;&#039; using [[Taylor expansion]]s, provided that &#039;&#039;f&#039;&#039; is sufficiently differentiable and that the moments of &#039;&#039;X&#039;&#039; are finite.  This technique is often used by [[statistics|statisticians]].&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
::{|&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;math&amp;gt;\mu&amp;lt;/math&amp;gt;&lt;br /&gt;
|&amp;lt;math&amp;gt; = \operatorname{E}\left[X\right]&amp;lt;/math&amp;gt;&lt;br /&gt;
|-&lt;br /&gt;
|&amp;lt;math&amp;gt;\sigma^2&amp;lt;/math&amp;gt; &lt;br /&gt;
|&amp;lt;math&amp;gt; = \operatorname{var}\left[X\right]&amp;lt;/math&amp;gt;&lt;br /&gt;
|}--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==First moment==&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
\operatorname{E}\left[f(X)\right] &amp;amp; {} = \operatorname{E}\left[f(\mu_X + \left(X - \mu_X\right))\right] \\&lt;br /&gt;
&amp;amp; {} \approx \operatorname{E}\left[f(\mu_X) + f&#039;(\mu_X)\left(X-\mu_X\right) + \frac{1}{2}f&#039;&#039;(\mu_X) \left(X - \mu_X\right)^2 \right].&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Noting that &amp;lt;math&amp;gt;E[X-\mu_X]=0&amp;lt;/math&amp;gt;, the 2nd term disappears. Also &amp;lt;math&amp;gt;E[(X-\mu_X)^2]&amp;lt;/math&amp;gt; is &amp;lt;math&amp;gt;\sigma_X^2&amp;lt;/math&amp;gt;. Therefore,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\operatorname{E}\left[f(X)\right]\approx f(\mu_X) +\frac{f&#039;&#039;(\mu_X)}{2}\sigma_X^2&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\mu_X&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\sigma^2_X&amp;lt;/math&amp;gt; are the mean and variance of X respectively.&lt;br /&gt;
&lt;br /&gt;
It is possible to generalize this to functions of more than one variable using [[Taylor expansion#Taylor series in several variables|multivariate Taylor expansions]]. For example,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\operatorname{E}\left[\frac{X}{Y}\right]\approx\frac{\operatorname{E}\left[X\right]}{\operatorname{E}\left[Y\right]} -\frac{\operatorname{cov}\left[X,Y\right]}{\operatorname{E}\left[Y\right]^2}+\frac{\operatorname{E}\left[X\right]}{\operatorname{E}\left[Y\right]^3}\operatorname{var}\left[Y\right]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Second moment==&lt;br /&gt;
Analogously,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\operatorname{var}\left[f(X)\right]\approx \left(f&#039;(\operatorname{E}\left[X\right])\right)^2\operatorname{var}\left[X\right] = \left(f&#039;(\mu_X)\right)^2\sigma^2_X.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The above is using a first order approximation unlike for the method used in estimating the first moment. It will be a poor approximation in cases where &amp;lt;math&amp;gt;f(X)&amp;lt;/math&amp;gt; is highly non-linear. This is a special case of the [[delta method]]. For example,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\operatorname{var}\left[\frac{X}{Y}\right]\approx\frac{\operatorname{var}\left[X\right]}{\operatorname{E}\left[Y\right]^2}-\frac{2\operatorname{E}\left[X\right]}{\operatorname{E}\left[Y\right]^3}\operatorname{cov}\left[X,Y\right]+\frac{\operatorname{E}\left[X\right]^2}{\operatorname{E}\left[Y\right]^4}\operatorname{var}\left[Y\right].&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Propagation of uncertainty]]&lt;br /&gt;
*[[WKB approximation]]&lt;br /&gt;
*http://www.stanford.edu/class/cme308/notes/TaylorAppDeltaMethod.pdf&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Taylor Expansions For The Moments Of Functions Of Random Variables}}&lt;br /&gt;
[[Category:Statistical approximations]]&lt;br /&gt;
[[Category:Algebra of random variables]]&lt;/div&gt;</summary>
		<author><name>117.216.176.13</name></author>
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