Evaluate by contour integration $$\int_{0}^1\frac{dx}{(x^2-x^3)^{1/3}}$$
I am not getting any idea as to how to solve this using contour integration in complex analysis. Can some one please help me?
Evaluate by contour integration $$\int_{0}^1\frac{dx}{(x^2-x^3)^{1/3}}$$
I am not getting any idea as to how to solve this using contour integration in complex analysis. Can some one please help me?
On
Such integral can be evaluated through Euler's Beta function:
$$ \int_{0}^{1}x^{-2/3}(1-x)^{-1/3}\,dx = B\left(\tfrac{1}{3},\tfrac{2}{3}\right) = \Gamma\left(\tfrac{1}{3}\right)\,\Gamma\left(\tfrac{2}{3}\right)\stackrel{\text{reflection f.}}{=}\frac{\pi}{\sin\frac{\pi}{3}} =\color{red}{\frac{2\pi}{\sqrt{3}}}.\tag{1} $$ As an alternative, by letting $x=\sin^2\theta$ the LHS is converted into
$$ 2\int_{0}^{\pi/2}\left(\cot\theta\right)^{1/3}\,d\theta=2\int_{0}^{+\infty}\frac{dt}{t^{1/3}(1+t^2)}=6\int_{0}^{+\infty}\frac{t}{1+t^6}\,dt=3\int_{0}^{+\infty}\frac{dt}{1+t^3}.\tag{2}$$ The last integral can be evaluated through standard contours, or just via $$ \int_{0}^{+\infty}\frac{dt}{(1+t)(1-t+t^2)}=\int_{1}^{+\infty}\frac{dt}{t(t^2-t+1)}=\int_{0}^{1}\frac{t\,dt}{t^2-t+1}=\left[\frac{1}{\sqrt{3}}\arctan\frac{2t-1}{\sqrt{3}}+\frac{1}{2}\log(t^2-t+1)\right]_{0}^{1}=\frac{2\pi}{\sqrt{3}}.\tag{3}$$
Of course we can evaluate this as a Beta function, but that is not the question. Points $0$ and $1$ are singularities of the integrand, which is a hint that contour integration may work on it.
The hint is this. The integrand $$ \frac{1}{(z^2-z^3)^{1/3}} $$ has a single-valued branch in the complement of the interval $[0,1]$. Let $f(z)$ be the branch that looks like $$ \frac{1-i\sqrt{3}}{2}\;\frac{1}{z} + O\left(\frac{1}{z^2}\right) \tag{1}$$ near $z=\infty$. There are no poles in the finite plane outside $[0,1]$.
Integration of $f(z)$ around a circle of large radius $R$ gives us the same answer as integration around a contour $\Gamma_\varepsilon$ described like this:
Go just below the real axis from $0-i\varepsilon$ to $1-i\varepsilon$, go around the point $1$ in a counterclockwise semicircle, go just above the real axis from $1+i\varepsilon$ to $0+i\varepsilon$, go around the point $0$ counterclockwise in a semicircle.
The limit (as $R \to +\infty$) of the integral around the large circle is found from (1). The limit (as $\varepsilon \to 0$) of the integral around the contour $\Gamma_\varepsilon$ is found in terms of the real integral you want to compute. You get a linear equation to solve for your integral.