Evaluating Contour Integral using Residue Theorem

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Homework Help Overview

The discussion revolves around evaluating the integral ##\int_{0}^{\infty} \frac{\sqrt{x}}{x^3 + 1} dx## using contour integration techniques. Participants explore the implications of the integral's definition over the positive real axis and the appropriate contours to consider in the complex plane.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of a semi-circular contour in the upper half-plane and the implications of poles located within the contour. There are questions about whether to adjust the contour to only include the relevant pole at ##z = e^{i\frac{\pi}{3}##. Some suggest considering different paths and angles to simplify the evaluation. Others propose a substitution to transform the integral into a potentially simpler form.

Discussion Status

The discussion is active, with various participants offering different perspectives on how to approach the integral. Some have provided hints regarding substitutions, while others emphasize the importance of contour integration. There is no explicit consensus on the best method, and multiple interpretations of the problem are being explored.

Contextual Notes

Participants note the challenges posed by the singularity at ##z=0## and the nature of the integrand, which may affect the choice of contour. The original poster's requirement to use contour integration is acknowledged, leading to a debate about the appropriateness of alternative methods.

  • #31
No-one seems to like my approach, but I shall persist anyway.:shy:
##I_1 = \int_{r=0}^\infty f(r).dr##
##I_2 = \lim_{R→\infty} \int_{\theta=0}^{2\pi/3} f(R e^{i\theta}).dR e^{i\theta} = 0##
##I_3 = \int_{r=\infty}^0 f(r e^{2\pi i/3}).d(r e^{2\pi i/3}) = \int_{r=\infty}^0 \frac{(r e^{2\pi i/3})^{\frac 1 2}}{1+(r e^{2\pi i/3})^3}e^{2\pi i/3}.dr= -\int_{r=0}^\infty \frac{\sqrt r e^{\pi i/3}e^{2\pi i/3}}{1+r^3}.dr = \int_{r=0}^\infty \frac{\sqrt r }{1+r^3}.dr = I_1##
Since the residue at the only pole inside the contour is -i/3, 2 I1 = I1+I2 + I3 = 2πi * (-i/3), so I1 = π/3.
 
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  • #32
haruspex said:
No-one seems to like my approach, but I shall persist anyway.:shy:
##I_1 = \int_{r=0}^\infty f(r).dr##
##I_2 = \lim_{R→\infty} \int_{\theta=0}^{2\pi/3} f(R e^{i\theta}).dR e^{i\theta} = 0##
##I_3 = \int_{r=\infty}^0 f(r e^{2\pi i/3}).d(r e^{2\pi i/3}) = \int_{r=\infty}^0 \frac{(r e^{2\pi i/3})^{\frac 1 2}}{1+(r e^{2\pi i/3})^3}e^{2\pi i/3}.dr= -\int_{r=0}^\infty \frac{\sqrt r e^{\pi i/3}e^{2\pi i/3}}{1+r^3}.dr = \int_{r=0}^\infty \frac{\sqrt r }{1+r^3}.dr = I_1##
Since the residue at the only pole inside the contour is -i/3, 2 I1 = I1+I2 + I3 = 2πi * (-i/3), so I1 = π/3.

It's an easier, simpler approach haruspex than what I initially came up with (the keyhole contour). Good though to see it solved several ways. That comes in handy too later on with other more difficult problems. :)
 

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