How can Laurent series be applied to complex analysis problems?

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Homework Help Overview

The discussion revolves around the application of Laurent series in complex analysis, specifically in relation to the function sinh(z) and contour integrals. Participants are exploring how to express sinh(z) using Laurent series and the implications of using residue theory in contour integration.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants attempt to express sinh(z) in terms of its Laurent series and question the presence of negative powers in the series. There are discussions about the relationship between Taylor and Laurent series, particularly in the context of sinh(z). Some participants express confusion regarding the application of residue theory in their contour integral problems.

Discussion Status

There is an ongoing exploration of the differences and similarities between Taylor and Laurent series. Some participants have provided insights into the nature of sinh(z) and its series representation, while others are seeking clarification on the use of residue theory in their calculations. The discussion reflects a mix of attempts to understand the concepts and the application of mathematical techniques.

Contextual Notes

Participants are navigating the constraints of homework guidelines, which may influence their approaches to the problems. There is a noted confusion regarding the distinction between Taylor and Laurent series as presented by their professor.

d3nat
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Homework Statement


Laurent series

Homework Equations



##f(z) = sinh(z)## around origin

The Attempt at a Solution



##sinh(z +\frac{1}{z}) = \sum_{-infty}^\infty A_nz^n##
where
##A_n = \frac{1}{2\pi i} \oint \frac{sinh(z'+\frac{1}{z'})}{z'^{n+1}} d'##

Let c = unit circle, ##z'=e^{i \theta}##
## dz' = ie^{i\theta} d\theta##

using Euler relationships

## = \frac{1}{2\pi i} i \oint \frac{sinh(e^{i\theta}+e^{-i\theta}}{(e^{i\theta})^{n+1}} d\theta'##
Cancel out the ##e^{i\theta}## on top and bottom

## = \frac{1}{2\pi} \oint \frac{sinh(2cos\theta)}{e^{in\theta}} d\theta##

## = \frac{1}{2\pi} \int_0^{2\pi} sinh(2cos\theta) e^{-in\theta} d\theta##

##e^{-in\theta} = cos(n\theta)-isin(n\theta)##

Then I said that only the ## cos(n\theta) ## part mattered because I stated the bounds of the integral were from ##0 to 2\pi##

## = \frac{1}{2\pi} \int_0^{2\pi} sinh(2cos\theta) cos(n\theta) d\theta##

However, I've tried many ways of simplifying this and I can't get an answer. Any suggestions? I'm so stumped... :/

Homework Statement


prove contour integral

##\int_0^{2\pi} \frac\{sin^2{\theta)}{a+bcos(\theta)} d\theta = \frac{2\pi}{b^2} [a-(a^2-b^2)^{frac{1}{2}}]##

Homework Equations



## d\theta = \frac{-i dz}{z}##
## sin^2(\theta) = \frac{-1}{4}(z^2+\frac{1}{z^2}-2)##
## cos(\theta) = \frac{1}{2}(z+\frac{1}{z})##

The Attempt at a Solution



Subst. all in and assuming unit circle:

## = -i \oint \frac{dz}{z} \frac{\frac{-1}{4}(z^2+\frac{1}{z^2}-2)}{a+ \frac{b}{2}(z+\frac{1}{z})} dz##

rearranging

## = \frac{i}{2} \oint \frac{dz}{z} \frac{(z^2+\frac{1}{z^2}-2)}{bz^2+2az+b} dz##

Then I solved this using the quadratic equations, so I had two roots (for the denominator)

I know I have to use residue theory, but I've never had to do it with something in the numerator. Is it still the same method? I'm confused...

 
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d3nat said:

Homework Statement


Laurent series

Homework Equations



##f(z) = sinh(z)## around origin

The Attempt at a Solution



##sinh(z +\frac{1}{z}) = \sum_{-infty}^\infty A_nz^n##
where
##A_n = \frac{1}{2\pi i} \oint \frac{sinh(z'+\frac{1}{z'})}{z'^{n+1}} d'##

Let c = unit circle, ##z'=e^{i \theta}##
## dz' = ie^{i\theta} d\theta##

using Euler relationships

## = \frac{1}{2\pi i} i \oint \frac{sinh(e^{i\theta}+e^{-i\theta}}{(e^{i\theta})^{n+1}} d\theta'##
Cancel out the ##e^{i\theta}## on top and bottom

## = \frac{1}{2\pi} \oint \frac{sinh(2cos\theta)}{e^{in\theta}} d\theta##

## = \frac{1}{2\pi} \int_0^{2\pi} sinh(2cos\theta) e^{-in\theta} d\theta##

##e^{-in\theta} = cos(n\theta)-isin(n\theta)##

Then I said that only the ## cos(n\theta) ## part mattered because I stated the bounds of the integral were from ##0 to 2\pi##

## = \frac{1}{2\pi} \int_0^{2\pi} sinh(2cos\theta) cos(n\theta) d\theta##

However, I've tried many ways of simplifying this and I can't get an answer. Any suggestions? I'm so stumped... :/

Homework Statement


prove contour integral

##\int_0^{2\pi} \frac\{sin^2{\theta)}{a+bcos(\theta)} d\theta = \frac{2\pi}{b^2} [a-(a^2-b^2)^{frac{1}{2}}]##

Homework Equations



## d\theta = \frac{-i dz}{z}##
## sin^2(\theta) = \frac{-1}{4}(z^2+\frac{1}{z^2}-2)##
## cos(\theta) = \frac{1}{2}(z+\frac{1}{z})##

The Attempt at a Solution



Subst. all in and assuming unit circle:

## = -i \oint \frac{dz}{z} \frac{\frac{-1}{4}(z^2+\frac{1}{z^2}-2)}{a+ \frac{b}{2}(z+\frac{1}{z})} dz##

rearranging

## = \frac{i}{2} \oint \frac{dz}{z} \frac{(z^2+\frac{1}{z^2}-2)}{bz^2+2az+b} dz##

Then I solved this using the quadratic equations, so I had two roots (for the denominator)

I know I have to use residue theory, but I've never had to do it with something in the numerator. Is it still the same method? I'm confused...

I don't get where you are going here. sinh(z) has a Taylor series around z=0. It's (e^z-e^(-z))/2. There are no negative powers of z at all.
 
Dick said:
I don't get where you are going here. sinh(z) has a Taylor series around z=0. It's (e^z-e^(-z))/2. There are no negative powers of z at all.


I mean, yah, I can solve it with a Taylor series, but I wasn't sure how to solve using a Laurent series, which is what the problem asks.
 
d3nat said:
I mean, yah, I can solve it with a Taylor series, but I wasn't sure how to solve using a Laurent series, which is what the problem asks.

A Laurent series is just a Taylor series possibly includes term of negative degree. sinh(z) doesn't have any. The Taylor series is the same as the Laurent series.
 
Dick said:
A Laurent series is just a Taylor series possibly includes term of negative degree. sinh(z) doesn't have any. The Taylor series is the same as the Laurent series.

Ohhh. Well then, I feel dumb.
My professor made them out to be completely different, so I thought it was two different methods of solving.
Thanks!
 

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