Difference between revisions of "Gaussian integral"
(Replaced content with "sdfih") |
|||
| Line 1: | Line 1: | ||
| − | + | {{move|Gaussian integral}} (The current version uses quotation marks in the title!) | |
| + | {{Template:Math-h}} | ||
| + | The '''Gaussian integral''' is the integral: | ||
| + | |||
| + | :<math> \int_{-\infty}^{\infty} e^{-x^2}dx. </math> | ||
| + | |||
| + | It has a value of <math>\sqrt\pi</math>. The value is needed to normalize the [[Normal distribution]]. | ||
| + | |||
| + | ==Derivation== | ||
| + | |||
| + | First look at the [[Double integral|double integral]] | ||
| + | |||
| + | <math>\int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-x^2-y^2}dxdy.</math> | ||
| + | |||
| + | Separating it, | ||
| + | |||
| + | <math>\int_{-\infty}^{\infty} e^{-x^2}dx \int_{-\infty}^{\infty} e^{-y^2}dy = (\int_{-\infty}^{\infty} e^{-x^2}dx)^2 </math> | ||
| + | |||
| + | So, the double integral is merely the square of the Gaussian integral. | ||
| + | |||
| + | 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: | ||
| + | |||
| + | <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> | ||
| + | |||
| + | <math> = (\int_{0}^{2\pi}d\theta)(\int_{0}^{\infty} e^{-r^2}rdr)</math> | ||
| + | |||
| + | <math> = 2\pi \int_{0}^{\infty} e^{-r^2}rdr.</math> | ||
| + | |||
| + | Substituting <math>z=r^2</math> into the integral, | ||
| + | |||
| + | <math> = 2\pi \int_{0}^{\infty} e^{-z}(z^{1/2})(\frac{dz}{2z^{1/2}})</math> | ||
| + | |||
| + | <math> = \pi \int_{0}^{\infty} e^{-z}dz = \pi \left[-e^{-z} \right]_0^{\infty} = \pi.</math> | ||
| + | |||
| + | Therefore, | ||
| + | |||
| + | <math>(\int_{-\infty}^{\infty} e^{-x^2}dx)^2 = \pi </math> | ||
| + | |||
| + | <math>\int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt\pi.</math> | ||
| + | |||
| + | |||
| + | [[category:mathematics]] | ||
Revision as of 23:36, October 31, 2011
- It has been proposed that this page, :Gaussian integral, be titled, "Gaussian integral".
(The current version uses quotation marks in the title!)
| Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{d}{dx} \sin x=?\,} | This article/section deals with mathematical concepts appropriate for late high school or early college. |
The Gaussian integral is the integral:
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-\infty}^{\infty} e^{-x^2}dx. }
It has a value of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sqrt\pi} . The value is needed to normalize the Normal distribution.
Derivation
First look at the double integral
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-x^2-y^2}dxdy.}
Separating it,
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-\infty}^{\infty} e^{-x^2}dx \int_{-\infty}^{\infty} e^{-y^2}dy = (\int_{-\infty}^{\infty} e^{-x^2}dx)^2 }
So, the double integral is merely the square of the Gaussian integral.
Now, do the double integral in polar co-ordinates. Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle -x^2-y^2= -(x^2+y^2) = -r^2} and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle dxdy=rdrd\theta} , so:
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-x^2-y^2}dxdy = \int_{0}^{2\pi}\int_{0}^{\infty} e^{-r^2}rdrd\theta}
Substituting into the integral,
Therefore,
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle (\int_{-\infty}^{\infty} e^{-x^2}dx)^2 = \pi }
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt\pi.}