Say I have this integral $\int_{-\infty}^\infty$ $\frac{x^2}{x^6+1}$ dx .
Now I know that it has six poles according to this denominator which are the six roots for -1. The question is after I split the denominator up into the 6 brackets which are the poles, is there any simpler way to evaluate the sum of the residues ? So that residue theorem can be used. Does seem like a pain to handle the 5 remaining brackets for each pole that I want to find the residue for.
Duplicate edit: The other question is about finding the poles only. That I already know how to do. I don't see how that is even relevant to my question.
2026-04-12 05:06:22.1775970382
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Conversion into contour integral and poles
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The function $f(z) = \frac {z^2}{z^6+1}$ has six poles of order 1, which means that you can compute the residue for each pole p as follows:
$$Res (f,p) = \lim_{z\to p}f(z)(z-p) $$
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I think you want to use the formula to calculate residue for a fractional function $f(z)$ defined as $$f(z) = \frac{g(z)}{h(z)}.$$ The residue at a simple pole $z_0$ is given by $$Res(f(z),z_0) = \frac{g(z_0)}{h'(z_0)}.$$ Essentially it is the same formula, as mentioned by @Dustin, but with an application of L'Hopital rule. You can follow this to get better idea of how it works.
As shown in many many places throughout this site, one can limit the number of residues to evaluate by using the symmetry of the integrand and making a wise choice of contour that exploits this symmetry. In this case, consider
$$\oint_C dz \frac{z^2}{z^6+1} $$
where $C$ is a wedge-shaped contour in the upper-half plane of radius $R$ and of angle $\pi/3$. The reason why the wedge has an angle of $\pi/3$ will become apparent as we carry out the calculation.
The contour integral is equal to
$$\int_0^R dx \frac{x^2}{1+x^6} + i R \int_0^{\pi/3} d\theta \, e^{i \theta} \frac{R^2 e^{i 2 \theta}}{1+R^6 e^{i 6 \theta}}+ e^{i \pi/3} \int_R^0 dt \, \frac{(e^{i \pi/3})^2 t^2}{1+(e^{i \pi/3})^6 t^6}$$
As $R \to \infty$, the magnitude of the second integral is bounded by
$$\left | i R \int_0^{\pi/3} d\theta \, e^{i \theta} \frac{R^2 e^{i 2 \theta}}{1+R^6 e^{i 6 \theta}} \right | \le \frac{\pi}{3} \frac{R^3}{R^6-1}$$
which clearly vanishes in this limit.
In this limit, the first integral becomes what we are looking for and the third integral becomes a multiple of what we are looking for. The sum of these two is equal to the contour integral which is
$$2 \int_0^{\infty} dx \frac{x^2}{1+x^6} = \int_{\infty}^{\infty} dx \frac{x^2}{1+x^6} $$
By the residue theorem, this is equal to $i 2 \pi$ times the sum of the residues of the poles inside $C$. Note that we have the advantage of having only one pole inside $C$ at $z=e^{i \pi/6}$ instead of three had we carried out the computation with a semicircle. Thus,
$$\int_{\infty}^{\infty} dx \frac{x^2}{1+x^6} = i 2 \pi \frac{(e^{i \pi/6})^2}{6 (e^{i \pi/6})^5}= \frac{\pi}{3}$$
Note that the wedge angle of $\pi/3$ made the integrands of the first and third integrals essentially the same within a constant factor.