The inverse trigonometric functions crop up wherever an angle must be computed from a ratio. Three typical examples.

Example 1 — Angle of elevation

An observer sees the top of a tower of height h=30h=30 m, from a horizontal distance d=50d=50 m. The angle of elevation θ\theta with respect to the ground satisfies: tanθ=hd=3050=0,6    θ=arctan(0,6)30,96°.\tan\theta = \frac{h}{d} = \frac{30}{50} = 0{,}6 \;\Rightarrow\; \theta = \arctan(0{,}6) \approx 30{,}96°. At distance d=10d=10 m: θ=arctan371,57°\theta = \arctan 3 \approx 71{,}57°. As one approaches the tower, the angle grows towards 90°90° (vertical asymptote of tan\tan).

Example 2 — Angle between two lines

Given r:y=2x+1r: y = 2x+1 and s:y=12x+3s: y = -\tfrac12 x + 3, with gradients m1=2m_1=2, m2=1/2m_2=-1/2. Since m1m2=1m_1 m_2 = -1, the lines are perpendicular (angle 90°90°). In general the angle α\alpha between two lines is obtained from tanα=m1m21+m1m2,α=arctan ⁣(m1m21+m1m2).\tan\alpha = \frac{m_1 - m_2}{1+m_1 m_2},\qquad \alpha = \arctan\!\left(\frac{m_1-m_2}{1+m_1 m_2}\right). If 1+m1m2=01+m_1m_2 = 0 the denominator vanishes and the angle is π/2\pi/2 (perpendicularity).

Example 3 — Refraction (an outline)

Snell’s law relates the angle of incidence θi\theta_i and of refraction θr\theta_r to the index nn: sinθi=nsinθr\sin\theta_i = n\sin\theta_r. Knowing θi\theta_i and nn, the refracted angle is θr=arcsin ⁣(sinθi/n)\theta_r = \arcsin\!\left(\sin\theta_i/n\right). For water-air n=1,33n=1{,}33 and θi=45°\theta_i=45°: θr=arcsin(0,531)32,1°\theta_r = \arcsin(0{,}531) \approx 32{,}1°.

Topics: Trigonometry
Concepts: Arcsine · Arctangent · Gradient · Line
Functions: Arcsine · Arctangent · Inverse trigonometric functions
Skills: Analytic geometry · Modelling · Using formulae