Integral Resulting in Arcsine

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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          
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \int \frac {\mathrm dx}{\sqrt{a^2} \sqrt{1 - \left({\frac x a}\right)^2} }\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(=\) \(\displaystyle \frac 1 a \int \frac {\mathrm dx}{\sqrt{1 - \left({\frac x a}\right)^2} }\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    

Substitute:

$\sin \theta = \dfrac x a \iff x = a \sin \theta$

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 $x/a \in \left(-1..1\right)$.

By hypothesis:

\(\displaystyle \) \(\displaystyle \) \(\displaystyle \) \(\displaystyle a^2\) \(>\) \(\displaystyle x^2\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)                    
\(\displaystyle \) \(\displaystyle \iff\) \(\displaystyle \) \(\displaystyle 1\) \(>\) \(\displaystyle \frac{x^2}{a^2}\) \(\displaystyle \) \(\displaystyle \) \(\displaystyle \)          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.
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