A radian is the angle subtended at the centre of a circle by an arc whose length is exactly equal to the radius of the circle. Consequently, the radian relates an angle directly to the geometry of the circle.
Because a full revolution is \(2\pi\) rad = 360°, the proportion
\[ \frac{\theta_{\text{rad}}}{2\pi}=\frac{\theta_{\deg}}{360} \]
gives the conversion formulae
| Angle (degrees) | Angle (radians) |
|---|---|
| 0° | 0 |
| 30° | \(\dfrac{\pi}{6}\) |
| 45° | \(\dfrac{\pi}{4}\) |
| 60° | \(\dfrac{\pi}{3}\) |
| 90° | \(\dfrac{\pi}{2}\) |
| 120° | \(\dfrac{2\pi}{3}\) |
| 180° | \(\pi\) |
| 270° | \(\dfrac{3\pi}{2}\) |
| 360° | 2\(\pi\) |
For a circle of radius \(r\) and a central angle \(\theta\) (in radians), the length \(s\) of the intercepted arc is
\[ s = r\theta \]
Find the arc length subtended by a \(2\ \text{rad}\) angle in a circle of radius \(5\ \text{cm}\).
Solution: \(s = r\theta = 5\ \text{cm}\times 2 = 10\ \text{cm}\).
Given an arc length of \(12\ \text{cm}\) on a circle of radius \(3\ \text{cm}\), determine the central angle in degrees.
Solution: \[ \theta = \frac{s}{r}= \frac{12}{3}=4\ \text{rad} \qquad\Rightarrow\qquad \theta_{\deg}= \frac{180}{\pi}\times4\approx 229.2^{\circ}. \]
The sector is the region bounded by two radii and the intercepted arc. Its area \(A\) is proportional to the central angle:
\[ A = \frac12\,r^{2}\theta \]
Find the area of a sector with radius \(4\ \text{m}\) and angle \(\dfrac{\pi}{3}\) radians.
Solution: \[ A = \frac12\times4^{2}\times\frac{\pi}{3} = \frac12\times16\times\frac{\pi}{3} = \frac{8\pi}{3}\ \text{m}^{2}. \]
A sector of a circle of radius \(5\ \text{cm}\) has area \(10\ \text{cm}^{2}\). Find the central angle in radians and in degrees.
Solution: \[ \theta = \frac{2A}{r^{2}} = \frac{2\times10}{5^{2}} = \frac{20}{25}=0.8\ \text{rad} \] \[ \theta_{\deg}= \frac{180}{\pi}\times0.8\approx 45.8^{\circ}. \]
All standard trigonometric identities remain valid when the angles are expressed in radians. For example:
These formulas are used throughout Pure Mathematics 1; the only requirement is that the arguments \(\alpha,\beta\) are in radians.
Show that \(\sin(\pi/6)=\frac12\) using the double‑angle identity.
Solution: \[ \sin\frac{\pi}{6}= \sin\!\left(\frac{\pi}{3}\times\frac12\right) = 2\sin\frac{\pi}{12}\cos\frac{\pi}{12} \] Evaluating the known values \(\sin\frac{\pi}{6}=0.5\) confirms the identity (the step illustrates that the identity works with radian arguments).
For sufficiently small angles (typically \(|\theta|<0.1\) rad) the first‑order Maclaurin expansions give:
Maclaurin series (truncated after the first non‑zero term) are:
\[ \sin\theta = \theta - \frac{\theta^{3}}{6}+O(\theta^{5}),\qquad \tan\theta = \theta + \frac{\theta^{3}}{3}+O(\theta^{5}),\qquad \cos\theta = 1 - \frac{\theta^{2}}{2} + \frac{\theta^{4}}{24}+O(\theta^{6}). \]
Approximate \(\sin 0.05\) rad.
Solution: \(\sin 0.05 \approx 0.05\). Calculator value: \(0.0499792\); absolute error \(2.08\times10^{-5}\) (< 0.05 %).
The differentiation formulas for the trigonometric functions are valid only when the angle is measured in radians. In particular:
These results follow from the limit \(\displaystyle \lim_{h\to0}\frac{\sin h}{h}=1\), which holds exclusively for radian measure. (A full proof is given later in the calculus chapter, but the key point for the syllabus is the dependence on radians.)
Find all solutions of \(\sin x = \tfrac12\) in the interval \([0,2\pi)\).
Solution: \(\displaystyle x = \frac{\pi}{6}\) or \(x = \frac{5\pi}{6}\) (both in radians).
| Quantity | Formula (radians) |
|---|---|
| Angle from arc length | \(\displaystyle \theta = \frac{s}{r}\) |
| Arc length | \(\displaystyle s = r\theta\) |
| Sector area | \(\displaystyle A = \frac12\,r^{2}\theta\) |
| Degree–radian conversion | \(\displaystyle \theta_{\text{rad}} = \frac{\pi}{180}\,\theta_{\deg}, \qquad \theta_{\deg} = \frac{180}{\pi}\,\theta_{\text{rad}}\) |
| Small‑angle \(\sin\) | \(\displaystyle \sin\theta \approx \theta\) |
| Small‑angle \(\tan\) | \(\displaystyle \tan\theta \approx \theta\) |
| Small‑angle \(\cos\) | \(\displaystyle \cos\theta \approx 1-\frac{\theta^{2}}{2}\) |
| Derivative of \(\sin\) (rad) | \(\displaystyle \frac{d}{dx}\sin x = \cos x\) |
| Derivative of \(\cos\) (rad) | \(\displaystyle \frac{d}{dx}\cos x = -\sin x\) |
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