Compute Residues for Periodic Function with Multiple Poles?

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Discussion Overview

The discussion focuses on computing the residues of the function \( f(z) = \frac{z-1}{1+\cos(\pi z)} \) at the points \( z_k = 2k+1 \) for \( k \neq 0 \). Participants explore the nature of the poles and the methods for calculating the residues, including the use of series expansions and derivative limits.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants propose that the poles \( z_k \) are simple poles, while others later correct this to indicate that \( z_0 \) is a simple pole and the others are double poles.
  • It is noted that \( z_k \) are zeros of order two of the denominator, and \( z_0 = 0 \) is a zero of the numerator, leading to the classification of the poles.
  • A method for calculating residues at second-order poles is suggested, involving the limit of the derivative of a modified function.
  • Participants discuss using a series expansion to analyze the function near the poles, leading to a specific form for the residue calculation.
  • One participant concludes that the residue at each pole \( z_k \) is \( \frac{2}{\pi^2} \), suggesting that this value is consistent across all poles due to the periodicity of the cosine function.
  • Another participant notes that the coefficient \( A_{-1} \) in the Laurent series expansion does not depend on \( k \), reinforcing the idea of uniformity in the residues.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the classification of the poles initially, with some claiming they are simple while others assert they are double. However, there is agreement on the residue value being the same for all poles, attributed to the periodic nature of the cosine function.

Contextual Notes

There are unresolved aspects regarding the assumptions made about the nature of the poles and the dependence on the series expansion used for residue calculation.

pantboio
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How can i compute $Res(f,z_k)$ where
$$f(z)=\frac{z-1}{1+cos\pi z}$$
and $z_k=2k+1, k\neq 0$?
 
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I think it's not too difficult to show that the $z_{k}$'s are simple poles. [EDIT] This is incorrect. $z_{0}$ is simple, but the others are double.
 
Last edited:
pantboio said:
$z_k$ are zeros of order two of denominator, but $z_0=0$ is also a zero of numerator. So $z_0=0$ is a simple pole, but all the others $z_k=2k+1$ with $k\neq 0$ are 2-poles.

Whoops. You're right. So you're going to need the next order formula, assuming that works. You could try
$$ \text{Res}(f,z_{k})= \lim_{z \to z_{k}} \frac{d}{dz} \left[(z-z_{k})^{2}f(z) \right]$$
for the second-order poles. That would come out to
$$ \text{Res}(f,2k+1)= \lim_{z \to 2k+1} \frac{d}{dz} \left[(z-2k-1)^{2} \, \frac{z-1}{1+ \cos( \pi z)} \right]$$
$$= \lim_{z \to 2k+1} \frac{d}{dz} \left[ \frac{(z-1)(z-2k-1)^{2}}{1+ \cos( \pi z)} \right]$$
$$= \lim_{z \to 2k+1} \frac{d}{dz} \left[ \frac{z^{3}-(4k+3)z^{2} +(4k^{2}+8k+3) z-(2k+1)^{2}}{1+ \cos( \pi z)} \right].$$
Looks like a fair amount of algebra. Hmm. You might be better off going for the series expansion.
 
Using a series expansion: $1+\cos \pi z=\ldots=\dfrac{\pi^2}{2}[z-(2k+1)]^2+\ldots$. Now,

$\dfrac{z-1}{1+\cos \pi z}=\dfrac{2k+[z-(2k+1)]}{\dfrac{\pi^2}{2}[z-(2k+1)]^2+\ldots}=\ldots +\dfrac{A_{-2}}{[z-(2k+1)]^2}+\dfrac{2/\pi^2}{z-(2k+1)}+A_0+\ldots$

So, $\mbox{Res }(f,2k+1)=\mbox{coef }\left(\dfrac{1}{z-(2k+1)}\right)=\dfrac{2}{\pi^2}$
 
Fernando Revilla said:
Using a series expansion: $1+\cos \pi z=\ldots=\dfrac{\pi^2}{2}[z-(2k+1)]^2+\ldots$. Now,

$\dfrac{z-1}{1+\cos \pi z}=\dfrac{2k+[z-(2k+1)]}{\dfrac{\pi^2}{2}[z-(2k+1)]^2+\ldots}=\ldots +\dfrac{A_{-2}}{[z-(2k+1)]^2}+\dfrac{2/\pi^2}{z-(2k+1)}+A_0+\ldots$

So, $\mbox{Res }(f,2k+1)=\mbox{coef }\left(\dfrac{1}{z-(2k+1)}\right)=\dfrac{2}{\pi^2}$
so the residue is the same for all poles, maybe because of $\cos$ periodicity
 
pantboio said:
so the residue is the same for all poles, maybe because of $\cos$ periodicity

More general: the coefficient $A_{-1}$ in the Laurent series expansion of $f$ does not depend on $k$.
 

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