Area of a Circle
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Theorem
The area $A$ of a circle is given by the formula $A=\pi r^2$, where $r$ is the radius of the circle.
Proof
We start with the equation of a circle: $x^2 + y^2 = r^2$.
Thus $y = \pm \sqrt{r^2 - x^2}$, so from the geometric interpretation of the definite integral:
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle A\) | \(=\) | \(\displaystyle \int_{-r}^r \left[ \sqrt{r^2 - x^2} - (-\sqrt{r^2 - x^2})\right] \mathrm d x\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int_{-r}^r 2 \sqrt{r^2 - x^2} \ \mathrm d x\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int_{-r}^r 2 r \sqrt{1 - \frac{x^2}{r^2} } \ \mathrm d x\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
Let $x = r \sin \theta$ (note that we can do this because $-r \le x \le r$).
Thus $\theta = \arcsin \left({\dfrac x r}\right)$ and $\mathrm d x = r \cos \theta \ \mathrm d \theta$.
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle A\) | \(=\) | \(\displaystyle \int_{\arcsin(\frac{-r} r)}^{\arcsin(\frac r r)} 2r^2 \sqrt{1-\frac{(r \sin \theta)^2}{r^2} }\cos \theta \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | From Integration by Substitution | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int_{-\frac{\pi} 2}^{\frac{\pi} 2} 2r^2\sqrt{1-\sin^2\theta}\cos\theta \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \int_{-\frac{\pi} 2}^{\frac{\pi} 2} 2r^2\sqrt{\cos^2\theta}\cos\theta \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | From Pythagorean trigonometric identities | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle r^2\int_{-\frac{\pi} 2}^{\frac{\pi} 2} 2\cos^2\theta \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle r^2\int_{-\frac{\pi} 2}^{\frac{\pi} 2} (1+\cos(2\theta)) \ \mathrm d \theta\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | Since $2\cos^2\theta = 1 + \cos(2\theta)$ from the double angle formula for cosine | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle r^2\left[\theta + \frac 1 2 \sin(2\theta)\right]_{-\frac{\pi} 2}^{\frac{\pi} 2}\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | From Integration of a Constant and Integral of Cosine Function | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle r^2\left[\frac{\pi} 2 + \frac 1 2 \sin\left(2\cdot\frac{-\pi} 2\right) - \frac{-\pi} 2 - \frac 1 2 \sin \left(2 \cdot \frac {\pi} 2 \right)\right]\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle r^2\left[2\cdot\frac{\pi} 2 + 2\cdot\frac 1 2 \cdot 0 \right]\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \pi r^2\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
$\blacksquare$
Proof by Shell Integration
The circle can be divided into a set of infinitesimally thin rings, each of which has area $2 \pi t \ \mathrm dt$, since the ring has length $2 \pi t$ and thickness $\mathrm d t$.
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle A\) | \(=\) | \(\displaystyle \int_0^r 2\pi t \ \mathrm d t\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | From the definition of pi | ||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \left[{\pi t^2}\right]_0^r\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | |||
| \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) | \(=\) | \(\displaystyle \pi r^2\) | \(\displaystyle \) | \(\displaystyle \) | \(\displaystyle \) |
$\blacksquare$