Evaluate \[\large \int \limits_0^{\infty}\frac{e^{-x}}{\sqrt{x}} \, dx = \sqrt{\pi} \] @Marki
i found the answer online but i don't get one step, so I won't bring it up :P
ok so far i got 2 methods :)
\[\int\limits_{ }^{ } \frac{e^{-x}}{\sqrt{x}}dx\]\[2\sqrt{x}e^{-x}+2\int\limits_{ }^{ }\sqrt{x}e^{-x}~dx\](differentiated e^-x, integ. by parts) \[2\sqrt{x}e^{-x}+2\int\limits_{ }^{ }\sqrt{x}e^{-x}~dx\]u sub, solving the second integral. u=sqrt{x} -x=-u^2 du= 1/(2sqrt{x}) dx >> 2sqrt{x}du=dx >> 2u du=dx 2 * integ. 2u^2 e^(-2u) du integration by parts twice to reduce the u^2.
Laplace :3
my method, if I haven't made a mistake, is not hard...
Oh nice i have searched a bit in MSE but couldnt find this :O please provide the link @TuringTest :)
Interesting xD f(t) = 1/sqrt(t) and we want L(1) @hartnn ? @((*-*)) im still going thru your method
take your time
yes ganesh, thats the easiest way :P
http://math.stackexchange.com/questions/215352/why-is-gamma-left-frac12-right-sqrt-pi (I am looking at the one using spherical coordinates) I don't get why the bounds change on the u-sub, and why the u-sub is correct shouldn't it lead to 4x in the exponent?
I think, it is necessary integrate by parts, first, as below: \[e ^{-x}*2\sqrt{x}|_{0}^{+\infty}+2\int\limits_{0}^{+\infty}e ^{-x}\sqrt{x}dx=2\Gamma(3/2)=2*\frac{ \sqrt{\pi} }{ 2 }=\sqrt{\pi}\]
lets take indefinite integral as refrence \(\large \int \limits_{-\infty}^{\infty} {e^{-x^2}} \, dx \\=\large 2\int \limits_0^{\infty} {e^{-x^2}} \, dx \) x= sqrt t so we would have \(\large 2\int \limits_0^{\infty} {e^{-x^2}} \, dx =\large 2\int \limits_0^{\infty} \frac{1}{2} {e^{-t}} t^{-\frac{1}{2} } \, dx = \Gamma(1/2) \) now lets proof \(\large \int \limits_{-\infty}^{\infty} {e^{-x^2}} \, dx \) there is several way chose from here to make me explain :P http://en.wikipedia.org/wiki/Gaussian_integral
u know that definite integral from -infinity to infinity give -sqrt pi now only chose any proof in wiki link so i would explain ,till then i'll post next method
sorry indefinite*
that looks very neat xD I can work \(\int_0^{\infty} e^{-x^2}dx\) using polar coordinates.. lm going through that mse link provided by TT surprisingly nobody used the obvious laplace transform there.. is it easy to find the laplace transform of 1/sqrt(t) ?
@hartnn mentioned that laplace was the easy way
@Michele_Laino how did you get \(\Gamma (3/2) = \sqrt{\pi}/2\) only if we can get some integer after doing by parts n times xD
hmm i never used or liked laplace :P my second method is using gama function properties im just writing my notes now , will provide u with it quick
I was like, hey guys, how about an elementary calculus?
@ganeshie8 what I don't understand is why it changes to\(\int_{-\infty}^\infty e^{-x^2}dx\) and *not* \(\int_{0}^\infty e^{-x^2}dx\) could somebody explain that to me? I am dumb
since for a property of the Gamma function, we can write: \[\Gamma (z+1)=z \Gamma (z)\] so: \[\Gamma(3/2)=\Gamma (1+1/2)=\frac{ 1 }{ 2 }\Gamma \left( \frac{ 1 }{ 2 } \right)\] @ganeshie8
well know that \(\Gamma (p)=p\Gamma (p-1)\) so 3/2=1+1/2 \(\Gamma (3/2)=3/2\Gamma (1/2)\) hmm how did u got sqrt pi /2 ?
oh wait my bad :P its p-1 gamma (p-1)
then its true :O
my questions got ignored :P fine, I'll figure it out myself
hey no im still thinking.. it has to do with e^(-x^2) being an converging even function i think
hm i didnt think of that
\[2\int\limits_0^{\infty} e^{-x^2} dx =\int\limits_{-\infty }^{\infty} e^{-x^2} dx \]
specifically\[\int_0^\infty e^{-x}d(2\sqrt x)=\int_{-\infty}^\infty e^{-u^2}du\]
ok first of all where did the 2 go?
sorry @Marki I already deleted my post
well ,this integral is the base of all integrals in complex :P i wuld say its like number 1 in multiplying operation and @Michele_Laino i note that thank u :) , how ever @TuringTest |dw:1420125759817:dw|
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