Gaussian integral using integration by parts

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mbigras
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Homework Statement


Show in detail that:
[tex] \sigma_{x}^{2} = \int_{-\infty}^{\infty} (x -\bar{x})^{2} \frac{1}{\sigma \sqrt{2 \pi}}e^{-\frac{(x-X)^{2}}{2\sigma^{2}}} = \sigma^{2}[/tex]
where,
[tex] G_{X,\sigma}(x) = \frac{1}{\sigma \sqrt{2 \pi}}e^{-\frac{(x-X)^{2}}{2\sigma^{2}}}[/tex]

Homework Equations


[tex] \int u dv = uv -\int v du[/tex]

The Attempt at a Solution


There are some hints that are given. Replace [itex]\bar{x}[/itex] with [itex]X[/itex] (according to the text, this is because they are equal after many trials). make the substitutions [itex]x-X=y[/itex] and [itex]y/\sigma=z[/itex]. Integrate by parts to obtain the result.

After following the hints I get the following integral:
[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{\infty}^{\infty} z^{2}e^{-\frac{z^{2}}{2}}dz[/tex]
How would one go about using integration by parts for this integral?
 
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If the problem is what you asked, you want to integrate by parts twice, taking down the ##x^2## one degree at each step.
 
D H said:
You only need to integrate by parts once if you know the value of ##\int_{-\infty}^{\infty} \exp(x^2) \, dx## (or of ##\int_{-\infty}^{\infty} \exp(x^2/2) \, dx\,\,##).
as it happens I don't know, altho I think I have done them over and over -- you'd think I would learn.
 
Working with integration by parts I've tried some different combinations of [itex]u[/itex] and [itex]dv[/itex]:

[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{-\infty}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> u=z^{2}\\<br /> du = 2 z dz\\<br /> dv = e^{-\frac{z^{2}}{2}}dz\\<br /> v = 2.5\\<br /> 2.5 z^{2} |_{-\infty}^{\infty} - \int 2.5 *2z dz\\<br /> =0[/tex]

Trying to recognize some symetry:
[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{-\infty}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> \frac{2\sigma}{\sqrt{2\pi}} \int_{0}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> u = z^{2}\\<br /> dv = e^{-\frac{z^{2}}{2}} dz[/tex]
seems to blow up to infinity as does setting [itex]u=z[/itex] and [itex]dv = ze^{-\frac{z^{2}}{2}}dz[/itex]

What I would like is a hint about choosing my [itex]u[/itex] and [itex]dv[/itex]. Or it seems like there's something I'm missing here.
 
[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{-\infty}^{\infty} z^{2} e^{-\frac{z^{2}}{2}}dz\\<br /> u = z\\<br /> du = dz\\<br /> \\<br /> dv = z e^{-\frac{z^{2}}{2}} dz\\<br /> v = ?\\<br /> \\[/tex]
working to find v and using a strange result that I found on the boards mentioned by nicksauce near the middle of the page link
[tex] \int z e^{-\frac{z^{2}}{2}} dz\\<br /> u = z\\<br /> du = dz\\<br /> \\<br /> dv = e^{-\frac{z^{2}}{2}} dz \\<br /> v = \frac{\sqrt{\pi}}{\sqrt{2}}\\<br /> \\<br /> z\frac{\sqrt{\pi}}{\sqrt{2}} - \int \frac{\sqrt{\pi}}{\sqrt{2}} dz = 0\\[/tex]
plugging back into above
[tex] u = z\\<br /> du = dz\\<br /> v = 0\\<br /> dv = z e^{-\frac{z^{2}}{2}} dz\\<br /> \\[/tex]
It seems like everything just keeps going to 0 or infinity.
 
How would I handle [itex]\int e^{-\frac{z^{2}}{2}} dz[/itex] if its an indefinite integral?
 
[tex] \sigma_{x}^{2} = \int_{-\infty}^{\infty} (x-X)^2 \frac{1}{\sigma\sqrt{2\pi}} e^{-(x-X)^{2}/2\sigma^{2}} \\<br /> <br /> = \int_{-\infty}^{\infty} y^2 \frac{1}{\sigma\sqrt{2\pi}} e^{-y^{2}/2\sigma^{2}} \\<br /> <br /> = \frac{\sigma}{\sqrt{2\pi}}\int_{-\infty}^{\infty} \frac{y^2}{\sigma^{2}}e^{-y^{2}/2\sigma^{2}} \\<br /> <br /> = \frac{\sigma}{\sqrt{2\pi}}\int_{-\infty}^{\infty} z^{2}e^{-z^{2}/2} \\[/tex]

then IBP and a u-sub to find [itex]v[/itex] by evaluating [itex]dv[/itex] as an indefinite integral.
[tex] u = z\\<br /> du = dz\\<br /> \\<br /> v = -e^{-\frac{z^{2}}{2}}\\<br /> dv = z e^{-\frac{z^{2}}{2}} dz\\<br /> \\<br /> \\<br /> -ze^{-z^2/2} |_{-\infty}^{\infty} + \int_{-\infty}^{\infty} e^{-z^{2}/2}dz\\<br /> = \sqrt{2\pi}[/tex]
going back up to the top
[tex] \sigma_{x}^{2} = \sigma[/tex]

Can you see where I'm missing the extra [itex]\sigma[/itex]? Also, what is the point of doing integration by parts if I just end up with the integral [itex]\int_{-\infty}^{\infty} e^{-z^{2}/2}dz=\sqrt{2\pi}[/itex], but I had to use wolfram to evaluate it, when at the very beginning I could have used wolfram to get [itex]\int_{-\infty}^{\infty} z^{2}e^{-z^{2}/2}=\sqrt{2\pi}[/itex].

Is there a trick to evaluating [itex]\int_{-\infty}^{\infty} e^{-z^{2}/2}dz[/itex] by hand?
 
mbigras said:
Working with integration by parts I've tried some different combinations of [itex]u[/itex] and [itex]dv[/itex]:

[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{-\infty}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> u=z^{2}\\<br /> du = 2 z dz\\<br /> dv = e^{-\frac{z^{2}}{2}}dz\\<br /> v = 2.5\\<br /> 2.5 z^{2} |_{-\infty}^{\infty} - \int 2.5 *2z dz\\<br /> =0[/tex]

Trying to recognize some symetry:
[tex] \frac{\sigma}{\sqrt{2\pi}} \int_{-\infty}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> \frac{2\sigma}{\sqrt{2\pi}} \int_{0}^{\infty} z^{2} e^{-\frac{z^2}{2}} dz\\<br /> u = z^{2}\\<br /> dv = e^{-\frac{z^{2}}{2}} dz[/tex]
seems to blow up to infinity as does setting [itex]u=z[/itex] and [itex]dv = ze^{-\frac{z^{2}}{2}}dz[/itex]

What I would like is a hint about choosing my [itex]u[/itex] and [itex]dv[/itex]. Or it seems like there's something I'm missing here.

Using ##u = z## and ##dv = z\: \exp(-z^2/2) \, dz## is exactly the way to go. I cannot get it to "blow up" as you claim.
 
D H said:
You left out the dx, dy, and dz in your integrals. Don't do that.
And there is my missing sigma! Thank you DH.