evaluate the integral
|dw:1419165589544:dw|
I actually have no idea, lol. by parts will not work I don't think
Are you sure that the lower limit is zero. ln(0) is -Infinity
Unless this is a Reimann Sum?
there must be problem with limit, ithink
This integral is actually equal to \[- \frac \pi 4 \]
this is also what wolframalpha is giving How to find it out?
type in the function.
Is this a problem in Calculus?
can you give me a hint. I am not able to do it by parts. I
im thinking of substitution \(x = \tan u\)
that gives you a nice bounds and you allows you to use properties of definite integrals
or is this question from complex analysis ?
\[\int_0^{\infty}\left[\frac{1}{(x^2+1)^2}\cdot \ln(x)\right]dx\]Is that how you thought of making \(x=\tan u\)?
I tried a couple things and this is what works! \[\Large I(\alpha) = \int\limits_0^\infty \frac{\ln(\alpha x)}{(x^2+1)^2}dx\] You need to use a parameter, then take the derivative with respect to it to get: \[\Large I'(\alpha) = \int\limits_0^\infty \frac{1}{\alpha} \frac{1}{(x^2+1)^2}dx\] This integral (which is hard but not impossible anymore becomes:
\[\Large I'(\alpha) = \frac{1}{2\alpha} \left( \frac{x}{x^2+1} + \tan^{-1}x\right) |_0^\infty\] Evaluate on the bounds and you get \[\Large I'(\alpha) = \frac{1}{\alpha} \frac{\pi}{4}\] Now let's integrate with respect to alpha: \[\Large I(\alpha) = \ln(\alpha) \frac{\pi}{4} + C\]
To solve for C we set them equal to each other \[\Large I(\alpha) = \ln( \alpha) \frac{\pi}{4} + C = \int\limits_0^\infty \frac{\ln(\alpha x)}{(x^2+1)^2}dx\] And actually I have to go unfortunately but we just need to set alpha so we can solve for the constant which will =0 and then we set alpha to 1 to recover our original integral I believe...
I actually didn't finish solving it yet but I just assumed it was right when I saw the pi/4 but I might have messed up somewhere. Good luck haha.
Ok I'm back let me finish!
Here's where we left off: \[\Large I(\alpha) = \ln( \alpha) \frac{\pi}{4} + C = \int\limits_0^\infty \frac{\ln(\alpha x)}{(x^2+1)^2}dx\] Let's let alpha =e and alpha =1/e to get two equations: \[\Large \frac{\pi}{4} + C = \int\limits\limits_0^\infty \frac{\ln( x)}{(x^2+1)^2}dx \\ \Large -\frac{\pi}{4} + C = -\int\limits\limits_0^\infty \frac{\ln( x)}{(x^2+1)^2}dx\] Add these two together and we have simply \[\Large C=0\]\
Upon looking at it again, I have decided that my answer is wrong. I don't know how to fix it haha.
this parameter stuff is really a very clever method xD
adding them together gives C = -pi/4
@ganeshie8 are you sure? I think I discovered the mistake in this substitution
See we can rewrite this "substitution" as:\[\large I(\alpha) = \int\limits_0^\infty \frac{\ln(\alpha x)}{(x^2+1)^2}dx = \ln(\alpha) \int\limits_0^\infty \frac{1}{(x^2+1)^2}dx+\int\limits_0^\infty \frac{\ln( x)}{(x^2+1)^2}dx\] So there's not really any dependence of the integral on alpha at all.
Oh im getting C = integral, why is that "independence" a reason for C getting equal to the integral in the end ?
nvm i was working on working on wrong stuff so we dont have C yet ?
Here is a solution using earlier trig substitution : \[\begin{aligned} &\int\limits_0^{\infty} \frac{\ln x dx}{(x^2+1)^2} &&\stackrel{u=\tan x}{=} \int\limits_0^{\pi/2}\cos^2 u \ln (\tan u) du = I\\~\\ &&&= -\int\limits_0^{\pi/2}\cos^2(\frac{\pi}{2}- u) \ln (\tan (\frac{\pi}{2}-u)) du \\~\\ &&&= -\int\limits_0^{\pi/2}\sin^2 u \ln (\tan u) du = I\\~\\ \end{aligned}\] Adding both gives \[\begin{aligned} 2I&= \int\limits_0^{\pi/2}\cos(2u) \ln (\tan u) du \\~\\ \end{aligned}\] Evaluating the indefinite integral is trivial by parts \[\begin{aligned} 2I&= \frac{1}{2}\sin(2u) \ln (\tan u) \Bigg|_0^{\pi/2} - \int \limits_0^{\pi/2} 1 du \\~\\ & = -\frac{\pi}{2} \end{aligned}\]
Suppose we try letting \(u=\ln x\) so that \(e^u=x\), and \(dx=e^u~du\). Then the integral becomes \[\int_{-\infty}^\infty \frac{ue^u}{(e^{2u}+1)^2}~du\] which looks ... easier? It seems doable with IBP at first glance.
IBP yields something like \[\frac{1}{2}\left[\arctan e^u+\frac{u e^u}{e^{2u}+1}\right]_{-\infty}^\infty-\frac{1}{2}\int_{-\infty}^\infty \left(\arctan e^u+\frac{e^u}{e^{2u}+1}\right)~du\] which runs into the problem of \[\int_{-\infty}^\infty \arctan e^u~du\] not converging.
Using a little residue theory one can show that (for \(a>0\)) \[\int\limits_{0}^{\infty}\frac{\ln(x)}{(x^2+a^2)^2}dx=\frac{\pi}{4a^3}\ln\left(\frac{a}{e} \right)\] letting \(a=1\) gives the answer to this particular problem
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