Salick Academy

Trigonometric Functions, Identities and Equations

No calculator

At CAPE, trigonometry stops being about triangles and becomes about identities. Almost every question is really asking: which identity turns this into something I can solve?

Radians and exact values

π radians=180°\pi \text{ radians} = 180°

so 11 radian ≈57.3°\approx 57.3°. To convert, multiply by π180\frac{\pi}{180} or 180π\frac{180}{\pi}.

60°=60×π180=π33π4=3π4×180π=135°60° = 60 \times \frac{\pi}{180} = \frac{\pi}{3} \qquad \frac{3\pi}{4} = \frac{3\pi}{4} \times \frac{180}{\pi} = 135°

Radians make two formulae beautifully simple. For a sector of radius rr and angle θ\theta in radians:

arc length s=rθsector area=12r2θ\text{arc length } s = r\theta \qquad \text{sector area} = \tfrac12 r^2\theta

A sector of radius 5 and angle 0.8 rad has arc length 5×0.8=45 \times 0.8 = 4; one of radius 6 and angle 0.5 rad has area 12(36)(0.5)=9\frac12(36)(0.5) = 9.

The exact values worth knowing by heart:

θ\theta sin⁡θ\sin\theta cos⁡θ\cos\theta tan⁡θ\tan\theta
00 00 11 00
π6=30°\frac{\pi}{6} = 30° 12\frac12 32\frac{\sqrt3}{2} 13\frac{1}{\sqrt3}
π4=45°\frac{\pi}{4} = 45° 12\frac{1}{\sqrt2} 12\frac{1}{\sqrt2} 11
π3=60°\frac{\pi}{3} = 60° 32\frac{\sqrt3}{2} 12\frac12 3\sqrt3
π2=90°\frac{\pi}{2} = 90° 11 00 undefined

Periods

y=sin⁡xy = \sin x and y=cos⁡xy = \cos x have period 2π2\pi and range [−1,1][-1, 1]. y=tan⁡xy = \tan x has period π\pi and no bound at all, with asymptotes at x=π2+nπx = \frac{\pi}{2} + n\pi.

For y=asin⁡(bx)y = a\sin(bx) the amplitude is ∣a∣|a| and the period is 2πb\dfrac{2\pi}{b}.

The reciprocal functions

sec⁡θ=1cos⁡θcosec⁡θ=1sin⁡θcot⁡θ=1tan⁡θ=cos⁡θsin⁡θ\sec\theta = \frac{1}{\cos\theta} \qquad \operatorname{cosec}\theta = \frac{1}{\sin\theta} \qquad \cot\theta = \frac{1}{\tan\theta} = \frac{\cos\theta}{\sin\theta}

Because ∣sin⁡θ∣≤1|\sin\theta| \le 1, the reciprocal ∣cosec⁡θ∣≥1|\operatorname{cosec}\theta| \ge 1 — these functions never take values strictly between −1-1 and 11.

Pythagorean identities

The fundamental one:

sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1

Dividing through by cos⁡2θ\cos^2\theta:

tan⁡2θ+1=sec⁡2θ\tan^2\theta + 1 = \sec^2\theta

Dividing instead by sin⁡2θ\sin^2\theta:

1+cot⁡2θ=cosec⁡2θ1 + \cot^2\theta = \operatorname{cosec}^2\theta

These are the tools for converting an equation into a single function. 2sin⁡2θ+3cos⁡θ=32\sin^2\theta + 3\cos\theta = 3 becomes, using sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta:

2−2cos⁡2θ+3cos⁡θ−3=0⇒2cos⁡2θ−3cos⁡θ+1=02 - 2\cos^2\theta + 3\cos\theta - 3 = 0 \quad \Rightarrow \quad 2\cos^2\theta - 3\cos\theta + 1 = 0

— a quadratic in cos⁡θ\cos\theta.

Compound angle formulae

sin⁡(A±B)=sin⁡Acos⁡B±cos⁡Asin⁡B\sin(A \pm B) = \sin A\cos B \pm \cos A\sin B cos⁡(A±B)=cos⁡Acos⁡B∓sin⁡Asin⁡B\cos(A \pm B) = \cos A\cos B \mp \sin A\sin B tan⁡(A±B)=tan⁡A±tan⁡B1∓tan⁡Atan⁡B\tan(A \pm B) = \frac{\tan A \pm \tan B}{1 \mp \tan A\tan B}

Find the exact value of sin⁡75°\sin 75°.

sin⁡75°=sin⁡(45°+30°)=sin⁡45°cos⁡30°+cos⁡45°sin⁡30°\sin 75° = \sin(45° + 30°) = \sin45°\cos30° + \cos45°\sin30° =12⋅32+12⋅12=3+122=6+24= \frac{1}{\sqrt2}\cdot\frac{\sqrt3}{2} + \frac{1}{\sqrt2}\cdot\frac12 = \frac{\sqrt3 + 1}{2\sqrt2} = \frac{\sqrt6 + \sqrt2}{4}

Check numerically: 2.449+1.4144=0.966\frac{2.449 + 1.414}{4} = 0.966, and sin⁡75°=0.966\sin 75° = 0.966 ✓

Double angle formulae

Set B=AB = A in the compound formulae:

sin⁡2A=2sin⁡Acos⁡A\sin 2A = 2\sin A\cos A cos⁡2A=cos⁡2A−sin⁡2A=2cos⁡2A−1=1−2sin⁡2A\cos 2A = \cos^2 A - \sin^2 A = 2\cos^2 A - 1 = 1 - 2\sin^2 A tan⁡2A=2tan⁡A1−tan⁡2A\tan 2A = \frac{2\tan A}{1 - \tan^2 A}

The three versions of cos⁡2A\cos 2A are equivalent — pick whichever leaves you with the function you want.

Solve sin⁡2θ=sin⁡θ\sin 2\theta = \sin\theta for 0≤θ<2π0 \le \theta < 2\pi.

2sin⁡θcos⁡θ−sin⁡θ=02\sin\theta\cos\theta - \sin\theta = 0 sin⁡θ(2cos⁡θ−1)=0\sin\theta(2\cos\theta - 1) = 0

sin⁡θ=0\sin\theta = 0 gives θ=0,π\theta = 0, \pi. And cos⁡θ=12\cos\theta = \frac12 gives θ=π3,5π3\theta = \frac{\pi}{3}, \frac{5\pi}{3}.

Four solutions in the interval.

The R-formula

acos⁡θ+bsin⁡θ=Rcos⁡(θ−α)a\cos\theta + b\sin\theta = R\cos(\theta - \alpha)

where

R=a2+b2tan⁡α=baR = \sqrt{a^2 + b^2} \qquad \tan\alpha = \frac{b}{a}

Expanding the right side gives Rcos⁡θcos⁡α+Rsin⁡θsin⁡αR\cos\theta\cos\alpha + R\sin\theta\sin\alpha; comparing coefficients yields Rcos⁡α=aR\cos\alpha = a and Rsin⁡α=bR\sin\alpha = b, which produce the two results above.

Express 3cos⁡θ+4sin⁡θ3\cos\theta + 4\sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha).

R=9+16=5tan⁡α=43⇒α=53.13°R = \sqrt{9 + 16} = 5 \qquad \tan\alpha = \tfrac43 \Rightarrow \alpha = 53.13°

3cos⁡θ+4sin⁡θ=5cos⁡(θ−53.13°)3\cos\theta + 4\sin\theta = 5\cos(\theta - 53.13°)

This form makes maxima and minima immediate: since cos⁡\cos ranges over [−1,1][-1,1], the expression has maximum 5 (at θ=53.13°\theta = 53.13°) and minimum −5-5.

Solve 3cos⁡θ+4sin⁡θ=23\cos\theta + 4\sin\theta = 2 for 0°≤θ<360°0° \le \theta < 360°.

5cos⁡(θ−53.13°)=2⇒cos⁡(θ−53.13°)=0.45\cos(\theta - 53.13°) = 2 \quad \Rightarrow \quad \cos(\theta - 53.13°) = 0.4 θ−53.13°=±66.42°\theta - 53.13° = \pm 66.42° θ=119.6°orθ=−13.3°≡346.7°\theta = 119.6° \quad \text{or} \quad \theta = -13.3° \equiv 346.7°

Solving trigonometric equations

A method that does not lose solutions:

  1. Reduce to one function using an identity.
  2. Solve as an ordinary equation — often a quadratic.
  3. Find every angle in the required interval, not just the calculator's principal value.
  4. Check the interval, especially after a substitution such as 2θ2\theta.

Solve 2cos⁡2θ+cos⁡θ−1=02\cos^2\theta + \cos\theta - 1 = 0 for 0°≤θ<360°0° \le \theta < 360°.

(2cos⁡θ−1)(cos⁡θ+1)=0(2\cos\theta - 1)(\cos\theta + 1) = 0

cos⁡θ=12\cos\theta = \frac12 gives θ=60°\theta = 60° and θ=300°\theta = 300°. cos⁡θ=−1\cos\theta = -1 gives θ=180°\theta = 180°.

Three solutions.