Calculating integrals using residue & cauchy & changing plan

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SUMMARY

The discussion focuses on calculating the integral \(\int_{0}^{2\pi} \dfrac{d\theta}{3+\tan^2\theta}\) using complex analysis techniques, specifically the residue theorem. Participants emphasize the transformation of trigonometric functions into the complex plane, utilizing \(z = e^{i\theta}\) and \(dz = ie^{i\theta}d\theta\). The integral's evaluation hinges on identifying poles within the unit circle, with some contributors expressing skepticism about the applicability of residue calculus due to the integrand's characteristics. Ultimately, the conversation highlights the necessity of correctly identifying poles to successfully apply the residue theorem.

PREREQUISITES
  • Complex analysis fundamentals
  • Residue theorem application
  • Transformation of trigonometric functions to exponential form
  • Understanding of poles and singularities in integrals
NEXT STEPS
  • Study the residue theorem in detail
  • Learn about contour integration techniques
  • Explore the transformation of trigonometric identities into complex exponentials
  • Investigate the identification and classification of poles in complex functions
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Mathematicians, physics students, and anyone interested in advanced calculus techniques, particularly those focusing on complex analysis and integral evaluation methods.

zhillyz
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Homework Statement


\int_{0}^{2\pi} \dfrac{d\theta}{3+tan^2\theta}

Homework Equations


\oint_C f(z) = 2\pi i \cdot R
R(z_{0}) = \lim_{z\to z_{0}}(z-z_{0})f(z)

The Attempt at a Solution


I did a similar example that had the form
\int_{0}^{2\pi} \dfrac{d\theta}{5+4cos\theta}

where I would change to the complex plane z where z = e^{i\theta} and so dz = ie^{i\theta}d\theta \to d\theta = \dfrac{e^{-i\theta}dz}{i}

The cosine function could also be written in terms of the exponential function as such;

e^{i\theta} = cos(\theta)+isin(\theta)
e^{-i\theta} = cos(\theta)-isin(\theta)
\therefore cos(\theta) = \dfrac{1}{2}\left[e^{i\theta} + e^{-i\theta}\right] = \dfrac{1}{2}\left[z + \dfrac{1}{z}\right]
after you substitute all these back into the formula it gives a denominator that can be factorised to give poles which you can find the residual values for and then calculate the integral using the residue theorem. I get kind of lost though trying to describe tan^2(\theta) in the same way.

tan^2(\theta) = sec^2(\theta) - 1 = \dfrac{sin^2(\theta)}{cos^2(\theta)}
sin^2(\theta) + cos^2(\theta) = 1

Thank you in advance.
 
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I do not think the calculus of residues will be of any help here (the integrand has no poles). Some observations:
  • 1+\tan^{2}\theta=\frac{1}{\cos^{2}\theta}
  • \cos(2\theta)=2\cos^{2}\theta-1, so \cos^{2}\theta=\frac{1+\cos2\theta}{2}
 
Svein said:
I do not think the calculus of residues will be of any help here (the integrand has no poles).
I think you did something wrong. There are three poles inside the unit circle.

zhillyz said:
I get kind of lost though trying to describe tan^2(\theta) in the same way.
You can show that
$$\sin \theta = \frac{e^{i\theta}-e^{-i\theta}}{2i} = \frac{z-\frac 1z}{2i},$$ so
$$\tan \theta = \frac 1i \frac{e^{i\theta}-e^{-i\theta}}{e^{i\theta}+e^{-i\theta}} = \frac 1i \frac{z^2-1}{z^2+1}.$$ Then it's just a matter of doing the algebra.
 

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