From a fraction with infinite sum in denominator to partial fractions?

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SUMMARY

The discussion focuses on the transformation of an integral involving a fraction with an infinite sum in the denominator into a form suitable for partial fraction decomposition. The integral in question is \(\int_{0}^{\frac{\pi}{4}} \frac{d\theta}{\epsilon^2 + \sin^2 \theta}\), which, after applying the Taylor expansion of \(\sin\) and substituting \(\theta = \epsilon u\), leads to the expression \(\frac{1}{\epsilon^2 + \epsilon^2 u^2 - \frac{1}{3} \epsilon^4 u^4 + \cdots}\). This is simplified to \(\frac{1}{\epsilon^2}\left( \frac{1}{1+u^2} + \frac{\epsilon u^4}{3(1+u^2)^2} + \cdots \right)\), demonstrating the equivalence through the manipulation of series expansions and factoring techniques.

PREREQUISITES
  • Understanding of Perturbation Methods
  • Familiarity with Taylor series expansions
  • Knowledge of partial fraction decomposition
  • Basic calculus, particularly integration techniques
NEXT STEPS
  • Study Taylor series and their applications in perturbation theory
  • Learn about partial fraction decomposition techniques in calculus
  • Explore the properties of integrals involving trigonometric functions
  • Investigate the convergence of series and their implications in mathematical analysis
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Students and researchers in mathematics, particularly those studying perturbation methods, integral calculus, and series expansions. This discussion is beneficial for anyone looking to deepen their understanding of mathematical transformations and series manipulations.

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From a fraction with infinite sum in denominator to partial fractions??

I am currently studying a course on Perturbation Methods and in particular an example considering the following integral \int_{0}^{\frac{\pi}{4}} \frac{d\theta}{\epsilon^2 + \sin^2 \theta}.

There's a section of the working where, having used the Taylor expansion of sin near 0 and using sin θ ≈ θ together with substitution θ=εu, we get the following fraction for the integrand
\frac{1}{\epsilon^2 + \epsilon^2 u^2 - \frac13 \epsilon^4 u^4 + \cdots}.
This then in both my lecture notes and a book I'm following becomes
\frac{1}{\epsilon^2}\left( \frac{1}{1+u^2} + \frac{\epsilon u^4}{3(1+u^2)^2} + \cdots \right).

Can anyone see how these are equal?
 
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It looks like using a variation on 1/(1-x) = 1 + x + x2 + ... after factoring out 1/{ε2(1+u2)}.

Also second term numerator should be (εu)4
 

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