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Mathematics 20 Online
OpenStudy (richyw):

Can someone help me with this power series expansion?

OpenStudy (richyw):

I am trying to evaluate this integral \[\Phi=-2R\mu G\int^\pi_0\frac{d\theta}{\left(r^2+R^2-2Rr\cos\theta\right)^{1/2}}\]

OpenStudy (richyw):

letting \(x=R/r\) I have\[\Phi=-2R\mu x\int\frac{d\theta}{\left(1+x^2-2x\cos\theta\right)^{1/2}}\]

OpenStudy (kainui):

I guess I'm waiting for the power series to come into play.

OpenStudy (richyw):

now my textbook wants me to expand this is a power series making certain to keep all terms of order \(x^2\). How do I do this? the next step shows\[\Phi=-2\mu Gx\int^{\pi}_0\left[\left(1-\frac{x^2}{2}+x\cos\theta\right)+ \frac{3}{8}\left(x^2-2x\cos\theta\right)^2+\dots\right]d\theta\]

OpenStudy (richyw):

I get lost at this step

OpenStudy (kainui):

Wait what? I'm lost too. So it's trying to expand this as a function of x or theta? I was hoping you'd be able to use a trig identity to get rid of the bottom. Maybe if I had more context, what is this? You're trying to do something in physics so perhaps it's an approximation to something that I could understand better, but it looks like the law of cosines essentially.

OpenStudy (richyw):

I am trying to find the potential of a field of a thin ring.

OpenStudy (richyw):

just uploading the page

OpenStudy (kainui):

Alright thanks, this looks fun overall, hopefully we can figure it out haha.

OpenStudy (richyw):

OpenStudy (richyw):

OpenStudy (richyw):

so I understand what happened up to the power series expansion. I am unsure of what math happened there. The rest is straightforwards as well

OpenStudy (kainui):

I guess it comes down to me really just not wanting to take the derivative of these functions to see if this is truly just a substitution of the power series.

OpenStudy (kainui):

Probably should just ask your professor about this, since this seems fairly odd to just sort of bust out the power series like this almost magically. I assume that this is really just a power series of (1+x^2-2xcos(theta))^(-1/2) and when you use the far-field approximation that essentially means that x^3 and higher terms become negligible, so we get rid of them to make the approximation simpler.

OpenStudy (richyw):

alright well thanks for trying!

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