Solving series with complex exponentials.

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The forum discussion centers on solving the series involving complex exponentials, specifically the equation: 1 + Σ(n=1 to ∞) (r/a)^n e^(jn(θ-φ)) + Σ(n=1 to ∞) (r/a)^n e^(-jn(θ-φ)). The contributors explore the manipulation of geometric series and the conditions under which the series converges, particularly noting that r ≤ a and |e^(j(θ-φ))| ≤ 1. The final expression derived is (a^2 - r^2) / (a^2 - 2ar cos(θ-φ) + r^2), confirming the validity of the geometric series approach for convergence.

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  • Understanding of complex exponentials and Euler's formula.
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  • Knowledge of series manipulation techniques in calculus.
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  • #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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