Integral Resulting in Arcsine
Contents |
Theorem
- $\displaystyle \int \frac 1{\sqrt{a^2 - x^2}} \ \mathrm dx = \arcsin{\frac x a} + C$
where $a$ is a strictly positive constant and $a^2 > x^2$.
Proof
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \int \frac 1 {\sqrt{a^2 - x^2} } \ \mathrm dx\) | \(=\) | \(\displaystyle \int \frac {\mathrm dx}{\sqrt{a^2 \left({1 - \frac {x^2}{a^2} }\right)} }\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | factor $a^2$ out of the radicand | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int \frac {\mathrm dx}{\sqrt{a^2} \sqrt{1 - \left({\frac x a}\right)^2} }\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \frac 1 a \int \frac {\mathrm dx}{\sqrt{1 - \left({\frac x a}\right)^2} }\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
- $\sin \theta = \dfrac x a \iff x = a \sin \theta$
for $\theta \in \left({-\dfrac \pi 2 .. \dfrac \pi 2}\right)$.
From Boundedness of Sine and Cosine and Shape of Sine Function, this substitution is valid for all $x/a \in \left(-1..1\right)$.
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle a^2\) | \(>\) | \(\displaystyle x^2\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \iff\) | \(\displaystyle \) | \(\displaystyle 1\) | \(>\) | \(\displaystyle \frac{x^2}{a^2}\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | dividing both terms by $a^2$ | ||
| \(\displaystyle \) | \(\displaystyle \iff\) | \(\displaystyle \) | \(\displaystyle 1\) | \(>\) | \(\displaystyle \left({\frac x a} \right)^2\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | Powers of Group Elements | ||
| \(\displaystyle \) | \(\displaystyle \iff\) | \(\displaystyle \) | \(\displaystyle 1\) | \(>\) | \(\displaystyle \left \vert{\frac x a}\right \vert\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | taking the square root of both terms | ||
| \(\displaystyle \) | \(\displaystyle \iff\) | \(\displaystyle \) | \(\displaystyle -1\) | \(<\) | \(\displaystyle \left({\frac x a}\right) < 1\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | Negative of Absolute Value |
... so this substitution will not change the domain of the integrand.
Then:
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle x\) | \(=\) | \(\displaystyle a \sin \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | from above | ||
| \(\displaystyle \) | \(\displaystyle \implies\) | \(\displaystyle \) | \(\displaystyle 1\) | \(=\) | \(\displaystyle a \cos \theta \frac {\mathrm d \theta}{\mathrm dx}\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | differentiate WRT $x$, Derivative of Sine Function, Chain Rule | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \frac 1 a \int \frac 1 {\sqrt{1 - \left({\frac x a}\right)^2 } } \ \mathrm dx\) | \(=\) | \(\displaystyle \frac 1 a \int \frac {a \cos \theta} {\sqrt {1 - \sin^2 \theta} } \frac{\mathrm d \theta} {\mathrm d x} \ \mathrm d x\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | from above | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \frac a a \int \frac{\cos \theta} {\sqrt {1 - \sin^2 \theta} } \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | Integration by Substitution | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int \frac {\cos \theta} {\sqrt {\cos^2 \theta} } \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | Sum of Squares of Sine and Cosine | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \ \int \frac {\cos \theta} {\left \vert \cos \theta \right \vert} \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
We have defined $\theta$ to be in the open interval $\left({-\dfrac \pi 2 .. \dfrac \pi 2}\right)$.
From Sine and Cosine are Periodic on Reals, $\cos \theta > 0$ for the entire interval. Therefore the absolute value is unnecessary, and the integral simplifies to:
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \int \mathrm d \theta\) | \(=\) | \(\displaystyle \theta + C\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
As $\theta$ was stipulated to be in the open interval $\left({-\dfrac \pi 2 .. \dfrac \pi 2}\right)$:
- $\sin \theta = \dfrac x a \iff \theta = \arcsin \dfrac x a$
The answer in terms of $x$, then, is:
- $\displaystyle \int \frac 1 {\sqrt{a^2 - x^2}} \ \mathrm dx = \arcsin \frac x a + C$
$\blacksquare$
Also see
Sources
- For a video presentation of the contents of this page, visit the Khan Academy.