Is it to do with \(\color{green}{\textsf{Gamma Function}}\) ?? \[\color{blue}{\int\limits_{-\infty}^{\infty}(e^{-x^2} \cdot x^2) dx}\] How to solve it??
\[\color{red}{\Gamma(n) = \int\limits_0^{\infty} e^{-x} \cdot x^{(n-1)} \cdot dx}\]
Is this right for Gamma Function??
yes @waterineyes
I am here only.. :)
If in my question I put : \(x^2 = t\), then \(2x \cdot dx = dt\) But, then what will be the limits for t ??
I get limits from : Infinity from Infinity, and here I got stuck....
The function is even, so you can do \[ \begin{align} \int_{-\infty}^{\infty}e^{-x^2}x^2dx&=2\int_{0}^{\infty}e^{-x^2}x^2dx \end{align}\]
then using your substitution will be okay :) it will still be bounds of 0 to \(\infty\) and you can use the gamma function
Wow..!!
One more doubt, I have. I have further problem in solving it..
The function is even, so you can do \[ \begin{align} \int_{-\infty}^{\infty}e^{-x^2}x^2dx&=2\int_{0}^{\infty}e^{-x^2}x\cdot dx \\&=2\int_{0}^{\infty}\end{align}\] \(u = x^2\) \(du = 2x dx \implies \dfrac{du}{2}=xdx\)
By substitution, I will get: \[2 \int\limits_{0}^{\infty} e^{-t} \cdot \sqrt{t} \cdot dt = \Gamma(\frac{3}{2})\] Is this right or not?
oops well ipressed enter too soon :)
yeah I get Gamma(3/2)
Then?? \[\Gamma (\frac{3}{2}) = \frac{3}{2} \Gamma(\frac{1}{2})\] ??
\[\implies \frac{3 \sqrt{\pi}}{2}\]
Or I have done it too fast, there must be a mistake.. :(
\(\Gamma \left( \dfrac{3}{2}\right)=\dfrac{1}{2}\Gamma \left( \dfrac{1}{2}\right)=\dfrac{\sqrt{\pi}}{2}\) since \(\Gamma(n)=(n-1)\Gamma(n-1)\)
\[\Gamma(n+1) = n \Gamma(n)\]
Sorry, Okay Okay.. I got it.. \[\Gamma(\frac{3}{2}) = \frac{\sqrt{\pi}}{2}\]
n is half there not 3/2..
\(\Large\checkmark \)
\[\color{green}{\checkmark}\]
@AccessDenied you want to add something??
I had a different route I was writing up. Just checking it over. :P
I did not check for even or odd, that's why it was looking typical to me.. :)
I won't mind, if we can go by that route now.. :)
This one involves the Gaussian integral with a parameter. Basically using the method for differentiation under the integral. \( \displaystyle \begin{align} \int_{-\infty}^{\infty} e^{-tx^2} \cdot x^2 \ dx &= -\int_{-\infty}^{\infty} \frac{\partial}{\partial t} \left( e^{-tx^2} \right) \ dx \\ &= \dfrac{d}{dt} \left(-\int_{-\infty}^{\infty} e^{-tx^2} \ dx \right) \\ &= \dfrac{d}{dt} \left(-\sqrt{\dfrac{\pi}{t}}\right) \\ &= \dfrac{d}{dt} \left(-\sqrt{\pi} \cdot t^{-1/2} \right) \\ &= \sqrt{\pi} \dfrac{1}{2} t^{-3/2} \\ \end{align} \) From there we can substitute t = 1 for the original integral, which gives back sqrt(pi)/2 again It was actually the first thing I thought of before I saw the above.
^nice method =]
Sorry @kirbykirby you content with the 3, this is for @AccessDenied ..
I will keep it in my notes.. :) Thank you both @kirbykirby and @AccessDenied ..
Glad to share! I've always liked that method after reading this online document and seeing some of its real power: http://www.math.uconn.edu/~kconrad/blurbs/analysis/diffunderint.pdf
I will definitely favourite that page
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