Difference between revisions of "Gaussian integral"

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{{move|Gaussian integral}} (The current version uses quotation marks in the title!)
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{{Template:Math-h}}
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The '''Gaussian integral''' is the integral:
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:<math> \int_{-\infty}^{\infty} e^{-x^2}dx. </math>
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It has a value of <math>\sqrt\pi</math>. The value is needed to normalize the [[Normal distribution]].
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==Derivation==
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First look at the [[Double integral|double integral]]
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<math>\int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-x^2-y^2}dxdy.</math>
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Separating it,
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<math>\int_{-\infty}^{\infty} e^{-x^2}dx \int_{-\infty}^{\infty} e^{-y^2}dy = (\int_{-\infty}^{\infty} e^{-x^2}dx)^2 </math>
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So, the double integral is merely the square of the Gaussian integral.
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Now, do the double integral in polar co-ordinates. <math>-x^2-y^2= -(x^2+y^2) = -r^2</math> and <math>dxdy=rdrd\theta</math>, so:
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<math>\int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-x^2-y^2}dxdy = \int_{0}^{2\pi}\int_{0}^{\infty} e^{-r^2}rdrd\theta</math>
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<math> = (\int_{0}^{2\pi}d\theta)(\int_{0}^{\infty} e^{-r^2}rdr)</math>
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<math> = 2\pi \int_{0}^{\infty} e^{-r^2}rdr.</math>
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Substituting <math>z=r^2</math> into the integral,
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<math> = 2\pi \int_{0}^{\infty} e^{-z}(z^{1/2})(\frac{dz}{2z^{1/2}})</math>
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<math> = \pi \int_{0}^{\infty} e^{-z}dz = \pi  \left[-e^{-z} \right]_0^{\infty} = \pi.</math>
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Therefore,
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<math>(\int_{-\infty}^{\infty} e^{-x^2}dx)^2 = \pi </math>
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<math>\int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt\pi.</math>
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[[category:mathematics]]

Revision as of 00:08, December 25, 2011

  • It has been proposed that this page, :Gaussian integral, be titled, "Gaussian integral".
    (The current version uses quotation marks in the title!)
This article/section deals with mathematical concepts appropriate for late high school or early college.

The Gaussian integral is the integral:

It has a value of . The value is needed to normalize the Normal distribution.

Derivation

First look at the double integral

Separating it,

So, the double integral is merely the square of the Gaussian integral.

Now, do the double integral in polar co-ordinates. and , so:

Substituting into the integral,

Therefore,