Trigonometry Toolkit

A2 · P3 · 2 min

P3 trigonometry adds three reciprocal functions and a dozen identities to the two you learnt in P1. The difficulty is rarely the algebra; it is choosing which identity to use. This note collects everything in one place and gives a strategy for picking the right tool.

Every identity you need

Key result

Definitions

sec⁡θ=1cos⁡θ,cosec⁡θ=1sin⁡θ,cot⁡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}

Pythagorean

sin⁡2θ+cos⁡2θ≡1,1+tan⁡2θ≡sec⁡2θ,1+cot⁡2θ≡cosec⁡2θ\sin^2\theta + \cos^2\theta \equiv 1, \qquad 1 + \tan^2\theta \equiv \sec^2\theta, \qquad 1 + \cot^2\theta \equiv \operatorname{cosec}^2\theta

Compound angles

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

Double angles

sin⁡2A≡2sin⁡Acos⁡A,cos⁡2A≡cos⁡2A−sin⁡2A≡2cos⁡2A−1≡1−2sin⁡2A,tan⁡2A≡2tan⁡A1−tan⁡2A\sin 2A \equiv 2\sin A\cos A, \qquad \cos 2A \equiv \cos^2 A - \sin^2 A \equiv 2\cos^2 A - 1 \equiv 1 - 2\sin^2 A, \qquad \tan 2A \equiv \frac{2\tan A}{1 - \tan^2 A}

Harmonic form

asin⁡θ±bcos⁡θ≡Rsin⁡(θ±α),acos⁡θ±bsin⁡θ≡Rcos⁡(θ∓α),R=a2+b2, tan⁡α=baa\sin\theta \pm b\cos\theta \equiv R\sin(\theta \pm \alpha), \qquad a\cos\theta \pm b\sin\theta \equiv R\cos(\theta \mp \alpha), \qquad R = \sqrt{a^2 + b^2},\ \tan\alpha = \frac{b}{a}

Choosing an identity

The expression containsReach for
sec⁡\sec, cosec⁡\operatorname{cosec}, cot⁡\cotrewrite in terms of sin⁡\sin, cos⁡\cos, tan⁡\tan; or the matching Pythagorean identity
tan⁡2\tan^2 and sec⁡2\sec^2 together, or sec⁡\sec and tan⁡\tan1+tan⁡2=sec⁡21 + \tan^2 = \sec^2
an angle and its double (θ\theta and 2θ2\theta)double-angle formulae; pick the cos⁡2A\cos 2A version that leaves one function
a sum or difference of angles, or θ±30∘\theta \pm 30^\circ etc.compound-angle formulae
asin⁡θ+bcos⁡θa\sin\theta + b\cos\theta with a constant on the other sideRR-form
sin⁡2\sin^2 or cos⁡2\cos^2 to integratecos⁡2A\cos 2A rearranged: sin⁡2A=12(1−cos⁡2A)\sin^2 A = \tfrac{1}{2}(1 - \cos 2A)
Simplifying a compound expression

Simplify cos⁡(x−30∘)−3sin⁡(x−60∘)\cos(x - 30^\circ) - \sqrt{3}\sin(x - 60^\circ).

Solution

cos⁡(x−30∘)=cos⁡xcos⁡30∘+sin⁡xsin⁡30∘=32cos⁡x+12sin⁡x\cos(x - 30^\circ) = \cos x\cos 30^\circ + \sin x\sin 30^\circ = \tfrac{\sqrt{3}}{2}\cos x + \tfrac{1}{2}\sin x.

3sin⁡(x−60∘)=3(12sin⁡x−32cos⁡x)=32sin⁡x−32cos⁡x\sqrt{3}\sin(x - 60^\circ) = \sqrt{3}\left(\tfrac{1}{2}\sin x - \tfrac{\sqrt{3}}{2}\cos x\right) = \tfrac{\sqrt{3}}{2}\sin x - \tfrac{3}{2}\cos x.

Subtracting: (32+32)cos⁡x+(12−32)sin⁡x\left(\tfrac{\sqrt{3}}{2} + \tfrac{3}{2}\right)\cos x + \left(\tfrac{1}{2} - \tfrac{\sqrt{3}}{2}\right)\sin x.

This is already simplified; it can be written as 3+32cos⁡x−3−12sin⁡x\tfrac{\sqrt{3} + 3}{2}\cos x - \tfrac{\sqrt{3} - 1}{2}\sin x, or converted to RR-form if a single function is wanted.

Mixed functions in one equation

Solve tan⁡θ+cot⁡θ=4\tan\theta + \cot\theta = 4 for 0∘<θ<180∘0^\circ < \theta < 180^\circ.

Solution

tan⁡θ+1tan⁡θ=4⇒tan⁡2θ−4tan⁡θ+1=0⇒tan⁡θ=2±3\tan\theta + \dfrac{1}{\tan\theta} = 4 \Rightarrow \tan^2\theta - 4\tan\theta + 1 = 0 \Rightarrow \tan\theta = 2 \pm \sqrt{3}.

tan⁡θ=3.732⇒θ=75∘\tan\theta = 3.732 \Rightarrow \theta = 75^\circ; tan⁡θ=0.268⇒θ=15∘\tan\theta = 0.268 \Rightarrow \theta = 15^\circ.

(Alternatively, tan⁡θ+cot⁡θ=1sin⁡θcos⁡θ=2sin⁡2θ\tan\theta + \cot\theta = \dfrac{1}{\sin\theta\cos\theta} = \dfrac{2}{\sin 2\theta}, so sin⁡2θ=12\sin 2\theta = \tfrac{1}{2}, giving 2θ=30∘,150∘2\theta = 30^\circ, 150^\circ.)

Sec and tan together

Solve sec⁡2θ=2tan⁡θ+4\sec^2\theta = 2\tan\theta + 4 for 0∘≤θ≤360∘0^\circ \leq \theta \leq 360^\circ.

Solution

1+tan⁡2θ=2tan⁡θ+4⇒tan⁡2θ−2tan⁡θ−3=0⇒(tan⁡θ−3)(tan⁡θ+1)=01 + \tan^2\theta = 2\tan\theta + 4 \Rightarrow \tan^2\theta - 2\tan\theta - 3 = 0 \Rightarrow (\tan\theta - 3)(\tan\theta + 1) = 0.

tan⁡θ=3\tan\theta = 3: θ=71.6∘,251.6∘\theta = 71.6^\circ, 251.6^\circ. tan⁡θ=−1\tan\theta = -1: θ=135∘,315∘\theta = 135^\circ, 315^\circ.

Strategy for proving identities

  1. Start from the more complicated side.
  2. Convert everything to sin⁡\sin and cos⁡\cos if no other identity is obvious.
  3. Combine fractions over a common denominator.
  4. Look for sin⁡2+cos⁡2\sin^2 + \cos^2 or a difference of two squares.
  5. Do not cross-multiply as if solving; keep the sides separate until they match.
A proof through sin and cos

Prove that sec⁡θ−cos⁡θtan⁡θ≡sin⁡θ\dfrac{\sec\theta - \cos\theta}{\tan\theta} \equiv \sin\theta.

Solution1cos⁡θ−cos⁡θsin⁡θcos⁡θ=1−cos⁡2θcos⁡θsin⁡θcos⁡θ=1−cos⁡2θsin⁡θ=sin⁡2θsin⁡θ=sin⁡θ.\frac{\frac{1}{\cos\theta} - \cos\theta}{\frac{\sin\theta}{\cos\theta}} = \frac{\frac{1 - \cos^2\theta}{\cos\theta}}{\frac{\sin\theta}{\cos\theta}} = \frac{1 - \cos^2\theta}{\sin\theta} = \frac{\sin^2\theta}{\sin\theta} = \sin\theta.
Exam tip

Exam questions in this topic almost always come in two parts: "prove the identity" then "hence solve". The "hence" means the equation is the identity in disguise; substitute and you get a simple equation in one function.

Practice

Question
  1. Simplify sin⁡2θ1+cos⁡2θ\dfrac{\sin 2\theta}{1 + \cos 2\theta}.
  2. Solve cosec⁡2θ=3cot⁡θ−1\operatorname{cosec}^2\theta = 3\cot\theta - 1 for 0∘<θ<360∘0^\circ < \theta < 360^\circ.
  3. Express cos⁡θ+3sin⁡θ\cos\theta + \sqrt{3}\sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha).
  4. Prove that 11−sin⁡θ−11+sin⁡θ≡2tan⁡θsec⁡θ\dfrac{1}{1 - \sin\theta} - \dfrac{1}{1 + \sin\theta} \equiv 2\tan\theta\sec\theta.
Answers
  1. 2sin⁡θcos⁡θ2cos⁡2θ=tan⁡θ\dfrac{2\sin\theta\cos\theta}{2\cos^2\theta} = \tan\theta.
  2. 1+cot⁡2θ=3cot⁡θ−1⇒cot⁡2θ−3cot⁡θ+2=0⇒cot⁡θ=1,21 + \cot^2\theta = 3\cot\theta - 1 \Rightarrow \cot^2\theta - 3\cot\theta + 2 = 0 \Rightarrow \cot\theta = 1, 2: θ=45∘,225∘,26.6∘,206.6∘\theta = 45^\circ, 225^\circ, 26.6^\circ, 206.6^\circ.
  3. 2cos⁡(θ−60∘)2\cos(\theta - 60^\circ).
  4. LHS =(1+sin⁡θ)−(1−sin⁡θ)1−sin⁡2θ=2sin⁡θcos⁡2θ=2tan⁡θsec⁡θ= \dfrac{(1 + \sin\theta) - (1 - \sin\theta)}{1 - \sin^2\theta} = \dfrac{2\sin\theta}{\cos^2\theta} = 2\tan\theta\sec\theta.

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