Approximations to the guassian integral

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SUMMARY

The discussion focuses on approximating the integral of the form \(\int_{x_1}^{x_2}\exp(-x^2)dx\), particularly when one endpoint is infinite. It highlights the known result that \(\int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt{\pi}\) and emphasizes the calculation of \(\int_0^x e^{-t^2} dt\). Two methods are presented: using the Taylor series expansion to derive a series representation and utilizing the Error function (Erf(x)), which is a well-documented and tabulated function for this integral.

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Euclid
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I assume this is standard but I wouldn't know where to look. How do you approximate an integral of the form
[tex]\int_{x_1}^{x_2}\exp(-x^2)dx[/tex]
where possibly one of the endpoints is infinite?
 
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Taking into account that the integrand is an even function, and the well known result that :[tex]\int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt{\pi}[/tex] It remains only to calculate a integral of the form:

[tex]\int_0^x e^{-t^2} dt[/tex].

You may calculate the taylor series and integrate term by term to get a series for that integral: [tex]\sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{n! (2n+1)} =\left(x-\frac{x^3}{3}+\frac{x^5}{10}-\frac{x^7}{42}+\frac{x^9}{216}-\ \cdots\right)[/tex],

Or alternatively, the Error function ( Erf(x) ) is only a constant multiple of that integral, and its values are well tabulated on the internet. http://en.wikipedia.org/wiki/Error_function
 
Ah... thanks. That is very useful.
 

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