Mathematics · Ch 2 — Trigonometry - I
Trigonometric functions with the help of a circle (trigonometric ratios of any angle)
Trigonometric functions with the help of a circle (trigonometric ratios of any angle)
Trigonometric functions with the help of a circle
Recovering the right-triangle ratios geometrically. Take a right triangle with the right angle at the foot of a perpendicular, and an acute angle θ. Writing the sides as before, and — this is just the familiar definition, set up so it can be generalised.
The general definition. Let θ be any angle, placed in standard position: its vertex at the origin O, and its initial ray OA along the positive x-axis. Consider a circle of radius r centred at O, and let OB be the terminal ray of θ. Let P(x, y) be the point where OB meets the circle. Drop a perpendicular from P to OA, meeting it at M. Then in the right triangle PMO, , , and , so
This matches the right-triangle definition exactly when θ is acute — but now nothing in the construction requires θ to be acute, or even positive. So for any θ ∈ ℝ, we simply define
Because every angle θ determines a unique point P on the circle (and every point on the circle determines a unique angle up to full revolutions), these six ratios really are functions of θ — hence the name trigonometric functions.
Two important consequences.
- Independent of r. If we chose a bigger or smaller circle, P's coordinates would scale by the same factor as r, so the ratios x/r and y/r are unchanged. The trigonometric functions depend only on the angle θ, never on which circle we drew.
- Coterminal angles agree. Angles that differ by a whole number of revolutions (360°, 720°, −360°, ...) have the same terminal ray, hence the same point P, hence identical trigonometric function values.
Why . Since P(x, y) lies on the circle of radius r centred at O, Pythagoras' theorem on triangle PMO gives . As θ varies, the pair traces out the whole circle.
The unit-circle special case. If we choose (the unit circle), the formulas collapse to their simplest form: and directly, i.e. . This is the form used throughout the rest of the chapter, since it is the cleanest to work with. …
What this figure shows. A circle of radius r centred at the origin O, with OA as the initial ray along the positive x-axis and OB as the terminal ray of angle θ. The point P(x, y) lies on the circle and on ray OB; PM is drawn perpendicular to OA, showing OM = x, PM = y, OP = r. …
What this figure shows. Two concentric-style rays from O at the same angle θ: P(x, y) lies on a circle of radius r while Q(x', y') lies on the unit circle on the same ray, illustrating (by similar triangles) that y = r·sinθ and x = r·cosθ, with x' = cosθ, y' = sinθ. …
What this figure shows. A companion diagram to Fig. 2.2 showing the two right triangles formed by dropping perpendiculars from P and Q to the x-axis, used to justify sinθ = y/r = y'/1 and cosθ = x/r = x'/1 via similar triangles. …