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I'm trying to find
\int\limits_0^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}dx}
Since the function is even, I can compute it as
\frac{1}<br /> {2}\int\limits_{ - \infty }^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}dx}
To use the residue theorem, I construct a large semi-circle C with center O and radius R. To avoid the real singularity at x = 0, we construct another (small) semi-circle c with radius r. The closed path is then given by C + [-R,-r] + c + [r,R]. We then let R go to infinity and r to 0. So we have:
\oint {\frac{{\sin x}}<br /> {{x^3 + x}}dx} = \int\limits_C {\frac{{\sin x}}<br /> {{x^3 + x}}dx} + \int\limits_c {\frac{{\sin x}}<br /> {{x^3 + x}}dx} + \int\limits_{ - R}^{ - r} {\frac{{\sin x}}<br /> {{x^3 + x}}} dx + \int\limits_r^R {\frac{{\sin x}}<br /> {{x^3 + x}}} dx
From the residue theorem, I found the LHS to be \pi \sinh 1, by applying the theorem to the only enclosed pole i.
Then, taking the limits or R and r to inf and 0, I found the integral over C to be 0 and over c to be -\pi which results in:
\int\limits_{ - \infty }^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}} dx = \pi \sinh 1 + \pi
Now that appears to be too large, does anyone know what mistake(s) I made or what I should do? Thanks!
\int\limits_0^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}dx}
Since the function is even, I can compute it as
\frac{1}<br /> {2}\int\limits_{ - \infty }^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}dx}
To use the residue theorem, I construct a large semi-circle C with center O and radius R. To avoid the real singularity at x = 0, we construct another (small) semi-circle c with radius r. The closed path is then given by C + [-R,-r] + c + [r,R]. We then let R go to infinity and r to 0. So we have:
\oint {\frac{{\sin x}}<br /> {{x^3 + x}}dx} = \int\limits_C {\frac{{\sin x}}<br /> {{x^3 + x}}dx} + \int\limits_c {\frac{{\sin x}}<br /> {{x^3 + x}}dx} + \int\limits_{ - R}^{ - r} {\frac{{\sin x}}<br /> {{x^3 + x}}} dx + \int\limits_r^R {\frac{{\sin x}}<br /> {{x^3 + x}}} dx
From the residue theorem, I found the LHS to be \pi \sinh 1, by applying the theorem to the only enclosed pole i.
Then, taking the limits or R and r to inf and 0, I found the integral over C to be 0 and over c to be -\pi which results in:
\int\limits_{ - \infty }^{ + \infty } {\frac{{\sin x}}<br /> {{x^3 + x}}} dx = \pi \sinh 1 + \pi
Now that appears to be too large, does anyone know what mistake(s) I made or what I should do? Thanks!