Solving series with complex exponentials.

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Homework Help Overview

The discussion revolves around the evaluation of a series involving complex exponentials, specifically the expression involving sums of the form \( \sum_{n=1}^{\infty}\left(\frac{r}{a}\right)^n e^{jn(\theta-\phi)} \) and its counterpart with negative exponentials. Participants are attempting to simplify this expression and relate it to known results from geometric series.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to manipulate the series by multiplying by a specific term to simplify it. Some participants suggest using the geometric series formula as a potential approach. Others note the importance of the starting index of the summation and how it affects the results.

Discussion Status

Participants are actively engaging with the problem, questioning the steps taken by the original poster, and exploring different interpretations of the series. There is a recognition of the need to clarify the impact of the summation's starting index and the conditions under which the geometric series applies. Some guidance has been offered regarding the manipulation of series, but no consensus has been reached on the correct approach.

Contextual Notes

It is noted that \( r \leq a \) and \( |e^{j(\theta-\phi)}| \leq 1 \), which are constraints relevant to the convergence of the series. Participants also discuss the implications of these constraints on the validity of the geometric series formula in this context.

  • #31
montadhar said:
[Acos(θ)+Bsin(θ)] is less than one ?
the entire term being less than 1 is what matters

There is no saying that ##A_n## and ##B_n## are smaller than one. Besides, your assumption will limit the solution to be less than 1, that is not right.
 
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  • #32
yungman said:
There is no saying that ##A_n## and ##B_n## are smaller than one. Besides, your assumption will limit the solution to be less than 1, that is not right.

You seem to think that a solution of Laplace's equation in the open disk ##r < a## must necessarily be continuous on the closed disk ##r \leq a##. There is no reason for anything like that to be true; we often face problems of solving a PDE in the interior of a set ##S##, but with a boundary condition on the boundary ##\partial S## that is not everywhere continuous.

Take the current example: the book gives you a function
U(r,\theta-\phi) = \frac{a^2 - r^2}{a^2 + r^2 - 2 a r \cos(\theta - \phi)}.
Below, let ##t = \theta - \phi## for ease of writing.

It is easy to verify directly that ##U## solves Laplace's equation in the open region ##r < a##. Furthermore, for every point ##(a,t_0)## with ##t_0 \neq 0## the function is continuous at ##(a,t_0)##; that is,
\lim_{(r,t) \to (a,t_0)} = 0 = U(a,t_0).
However, ##U## is not continuous at ##(a,0)## (or at ##(a, \pm 2 \pi n), n = 0, 1, 2, \ldots##). For example, for ##r = a## we have
U(a,t) = 0\; \forall\: t \neq 0,
so ##\lim_{t \to 0} U(a,t) = 0.## However, for ##r \neq a## we have
U(r,0) = \frac{a^2 - r^2}{a^2+r^2 - 2 a r} = \frac{a^2 - r^2}{(a-r)^2} = <br /> \frac{a+r}{a-r} \to +\infty\text{ as } r \to a-.
So, the function given to you in the book does satisfy Laplace's equation in the open disc and is continuous except at a single point on the boundary of the disc.

Exactly the same thing happens in the infinite-series representation of ##U##. The fact that the series fails to converge at a single point with ##r = a## is not problem; the function ##U## is just not continuous there, and that has absolutely nothing to do with the infinite series (or, rather, is reflected properly in the infinite series, as it should be).
 
  • #33
Yes, I agree that there is no guaranty the solution is continuous. BUT if you look at the original equation:
u=A_0+\sum_{n=1}^{\infty} \left(\frac{r}{a}\right)^n[A_n\cos(n\theta)+B_n\sin(n\theta)]

It is continuous at ##r=a##.

But if convert the above formula into this form:

\sum_{n=1}^{\infty}\left(\frac{r}{a}\right)^n e^{jn(\theta-\phi)}\;\Rightarrow\;x=\left(\frac{r}{a}\right) e^{j(\theta-\phi)}\;\Rightarrow\;\frac{1}{1-x}=\frac{a}{a-re^{j(\theta-\phi)}}

You have undefined solution whenever ##x=1##. That is not right!

You convert a continuous solution into one that has undefined solution.
 
  • #34
yungman said:
Yes, I agree that there is no guaranty the solution is continuous. BUT if you look at the original equation:
u=A_0+\sum_{n=1}^{\infty} \left(\frac{r}{a}\right)^n[A_n\cos(n\theta)+B_n\sin(n\theta)]

It is continuous at ##r=a##.

But if convert the above formula into this form:

\sum_{n=1}^{\infty}\left(\frac{r}{a}\right)^n e^{jn(\theta-\phi)}\;\Rightarrow\;x=\left(\frac{r}{a}\right) e^{j(\theta-\phi)}\;\Rightarrow\;\frac{1}{1-x}=\frac{a}{a-re^{j(\theta-\phi)}}

You have undefined solution whenever ##x=1##. That is not right!

You convert a continuous solution into one that has undefined solution.

Stop blaming ME; all I did was expand on what the BOOK says. If you have a problem, take it up with the authors of the book!

Anyway, you cannot just say that your original Fourier series is continuous at r = a; you have to PROVE it. You will have trouble doing this, because such arguments are a lot harder than you might think. Anyway, I suspect you are wrong; I bet the function is NOT continuous on the whole circle r = a, and just saying so or wishing it to be true will not work.
 
  • #35
Ray Vickson said:
Stop blaming ME; all I did was expand on what the BOOK says. If you have a problem, take it up with the authors of the book!

Anyway, you cannot just say that your original Fourier series is continuous at r = a; you have to PROVE it. You will have trouble doing this, because such arguments are a lot harder than you might think. Anyway, I suspect you are wrong; I bet the function is NOT continuous on the whole circle r = a, and just saying so or wishing it to be true will not work.

I am not blaming you or disrespect you at all.

All I am saying is from the original formula where the exponential formula supposing derived from is continuous unless ##A_n## or ##B_n## is infinite.

u=A_0+\sum_{n=1}^{\infty} \left(\frac{r}{a}\right)^n[A_n\cos(n\theta)+B_n\sin(n\theta)]

But the derived formula goes to infinite at ##r=a## no matter what.

This is really a question than disrespecting you. I am an engineer that trying to learn math, I am not in the same league to disrespect you or anyone that is homework helper here! I am desperately trying to derive and making sense of this.

Far as I know, using ##\sum_0^{\infty} x^n=\frac{1}{1-x}## require ##x\neq 1## no matter what. That's the limitation that has to be imposed on this series expansion.
 

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