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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#1
Find Closed Form

Find Closed Form:

\sum_{n=1,3,5\ldots} \frac{1}{n}e^{-n\pi x/a}\sin{(n\pi y/a)}

PostPosted: Tue Feb 15, 2005 3:34 pm  Back to top 
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joml88
Birch & Swinnerton Dyer
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#2
Please don't double post in multiple forums...I am going to delete your post in the Intermediate Forum.

PostPosted: Tue Feb 15, 2005 3:58 pm  Back to top 
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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#3
with the 40 thousand forums these days, I never know where to post or what level my question falls under... is this problem too advanced for this forum?

PostPosted: Tue Feb 15, 2005 7:22 pm  Back to top 
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Ravi B
Navier-Stokes Equations
Navier-Stokes Equations

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#4
Hint
You can use the identity
\sin \theta = \frac{e^{i\theta} - e^{-i\theta}}{2i}.


PostPosted: Tue Feb 15, 2005 7:29 pm  Back to top 
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jmerry
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#5
Given the nature of the sum, this belongs somewhere in Calculus-Analysis; this is evaluated by interpreting it as a power series.

It's certainly impossible without at least some calculus material.

PostPosted: Tue Feb 15, 2005 8:21 pm  Back to top 
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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#6
would an admin be so kind as to move this post?

PostPosted: Tue Feb 15, 2005 9:38 pm  Back to top 
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Myth
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#7
Spoon wrote:
would an admin be so kind as to move this post?

You should ask moderators for that Wink
_________________
Myth is out of here

PostPosted: Tue Feb 15, 2005 9:58 pm  Back to top 
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Kent Merryfield
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#8
One observation:

If we let u(x,y)=\sum_{\substack{n=1 \\ n \,\text{odd}}}^{\infty} \frac1ne^{-n\pi x/a} \sin(n\pi y/a) for x>0

then \frac{\partial^2u}{\partial x^2}+\frac{\partial^2u}{\partial y^2}=0.

In other words, this is a harmonic function on the right hand half plane with boundary values equal to a "square wave":

u(0,y)= \frac{\pi}4 for 0<y<a, =-\frac{\pi}4 for -a<y<0, and continued to be periodic of period 2a.

As for a closed form solution, I'll get it started.

Let r=e^{-\pi x/a} and let \theta = \frac{\pi y}a. Then we want to compute

\sum_{\substack{n=1 \\ n \,\text{odd}}}^{\infty} \frac1nr^n\sin(n\theta) = \text{Im}\left(\sum_{\substack{n=1 \\ n \,\text{od...

Let g(z)=\sum_{\substack{n=1 \\ n \,\text{odd}}}^{\infty} \frac1nz^n. Differentiate that to get g(z)=\frac1{1-z^2}.

Integrate that and take the imaginary part. The sum we are looking for is

\frac12\text{Arg}\left(\frac{1+z}{1-z}\right).

Someone else can take over from here and finish this.
Last edited by Kent Merryfield on Wed Feb 16, 2005 11:57 am; edited 2 times in total 
PostPosted: Wed Feb 16, 2005 10:28 am  Back to top 
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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#9
Myth wrote:
Spoon wrote:
would an admin be so kind as to move this post?

You should ask moderators for that Wink


by "admin" I think I meant "anyone with the power to move a post"... I was not being so specific...

Anyway, Kent, good catch on Laplace's Equation... This solution actually resulted from solving laplace's equation to begin with Smile.

PostPosted: Wed Feb 16, 2005 11:48 am  Back to top 
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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#10
ok... so like could the moderator please put my post back where it was? Since it's been moved, nobody has even given it a look.

Thanks

PostPosted: Sun Feb 20, 2005 6:35 pm  Back to top 
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vuhung
Hodge Conjecture
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#11
Ravi B wrote:
Hint
You can use the identity
\sin \theta = \frac{e^{i\theta} - e^{-i\theta}}{2i}.

Yes, this maybe the first proof traightforward....

PostPosted: Sun Feb 20, 2005 7:19 pm  Back to top 
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Spoon
Yang-Mills Theory
Yang-Mills Theory

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#12
I don't see how that leads to the solution...

PostPosted: Tue Feb 22, 2005 4:02 pm  Back to top 
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Kent Merryfield
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#13
Well, I've got an answer for you in #8, but I didn't finish it.

u=\frac12(\arg(1+z)-\arg(1-z)) where

z=re^{i\theta},\, r=e^{-\pi x/a},\,\theta=\frac{\pi y}a.

Of course, there's a long way to go.

The first step after that is the geometry-trigonometry problem of computing \arg(1+re^{i\theta}) and \arg(1-re^{i\theta}).

That should take some time; I would suggest starting by drawing pictures of triangles.

Then you can put in what r and \theta are.

PostPosted: Tue Feb 22, 2005 7:31 pm  Back to top 
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