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Trigonometric proofs and applicationsAQA A-Level Maths: Revision notes

Section 1

Identities you need to know

Proofs use a small toolkit of identities, all true wherever both sides are defined:

  • sin⁡2θ+cos⁡2θ≡1\sin^2\theta+\cos^2\theta\equiv1,   1+tan⁡2θ≡sec⁡2θ\;1+\tan^2\theta\equiv\sec^2\theta,   1+cot⁡2θ≡cosec⁡2θ\;1+\cot^2\theta\equiv\operatorname{cosec}^2\theta
  • tan⁡θ≡sin⁡θcos⁡θ\tan\theta\equiv\frac{\sin\theta}{\cos\theta},   sec⁡θ≡1cos⁡θ\;\sec\theta\equiv\frac{1}{\cos\theta},   cosec⁡θ≡1sin⁡θ\;\operatorname{cosec}\theta\equiv\frac{1}{\sin\theta}
  • Addition formulae: sin⁡(A±B)≡sin⁡Acos⁡B±cos⁡Asin⁡B\sin(A\pm B)\equiv\sin A\cos B\pm\cos A\sin B and cos⁡(A±B)≡cos⁡Acos⁡B∓sin⁡Asin⁡B\cos(A\pm B)\equiv\cos A\cos B\mp\sin A\sin B
  • Double angle formulae: sin⁡2A≡2sin⁡Acos⁡A\sin2A\equiv2\sin A\cos A,   cos⁡2A≡cos⁡2A−sin⁡2A≡2cos⁡2A−1≡1−2sin⁡2A\;\cos2A\equiv\cos^2A-\sin^2A\equiv2\cos^2A-1\equiv1-2\sin^2A,   tan⁡2A≡2tan⁡A1−tan⁡2A\;\tan2A\equiv\frac{2\tan A}{1-\tan^2A} Choose the form of cos⁡2A\cos2A that matches what you want to cancel: 2cos⁡2A−12\cos^2A-1 to leave only cosines, 1−2sin⁡2A1-2\sin^2A to leave only sines.
Key termsidentityaddition formuladouble angle formula
Common mistake

Writing sin⁡(A+B)=sin⁡A+sin⁡B\sin(A+B)=\sin A+\sin B. Sine does not distribute over addition.

Section 2

How to construct a proof

To prove an identity, start from the more complicated side and transform it step by step until it equals the other side. Do not work on both sides at once and do not cross-multiply as if it were an equation, because that assumes the result you are proving. Useful moves: write everything in terms of sin⁡\sin and cos⁡\cos; use a Pythagorean identity to convert squares; replace sin⁡2A\sin2A or cos⁡2A\cos2A; factorise (difference of two squares is common); combine fractions over a common denominator. Finish with a clear concluding statement. Example: prove sin⁡2θ1+cos⁡2θ≡tan⁡θ\frac{\sin2\theta}{1+\cos2\theta}\equiv\tan\theta. LHS=2sin⁡θcos⁡θ1+(2cos⁡2θ−1)=2sin⁡θcos⁡θ2cos⁡2θ=sin⁡θcos⁡θ=tan⁡θ=RHS.\text{LHS}=\frac{2\sin\theta\cos\theta}{1+(2\cos^2\theta-1)}=\frac{2\sin\theta\cos\theta}{2\cos^2\theta}=\frac{\sin\theta}{\cos\theta}=\tan\theta=\text{RHS}. The identity holds except where cos⁡θ=0\cos\theta=0, where both sides are undefined.

Key termsproofLHS and RHS
Common mistake

Treating an identity like an equation and applying the same operation to both sides. Transform one side only.

Exam tip

If stuck, rewrite everything in sin⁡\sin and cos⁡\cos.

Section 3

Proofs using factorising and the compound angle

Example: sin⁡4x−cos⁡4x≡(sin⁡2x−cos⁡2x)(sin⁡2x+cos⁡2x)≡sin⁡2x−cos⁡2x≡−cos⁡2x\sin^4x-\cos^4x\equiv(\sin^2x-\cos^2x)(\sin^2x+\cos^2x)\equiv\sin^2x-\cos^2x\equiv-\cos2x. Example: prove cos⁡θ+sin⁡θ≡2cos⁡(θ−π4)\cos\theta+\sin\theta\equiv\sqrt2\cos\left(\theta-\frac{\pi}{4}\right). Expand the right-hand side: 2(cos⁡θcos⁡π4+sin⁡θsin⁡π4)=2⋅22(cos⁡θ+sin⁡θ)=cos⁡θ+sin⁡θ.\sqrt2\left(\cos\theta\cos\frac{\pi}{4}+\sin\theta\sin\frac{\pi}{4}\right)=\sqrt2\cdot\frac{\sqrt2}{2}(\cos\theta+\sin\theta)=\cos\theta+\sin\theta. This shows why cos⁡θ+sin⁡θ\cos\theta+\sin\theta has greatest value 2\sqrt2 and least value −2-\sqrt2. A disproof needs only one counter-example. To show sin⁡2θ≡2sin⁡θ\sin2\theta\equiv2\sin\theta is false, take θ=30∘\theta=30^{\circ}: sin⁡60∘=32≠2×12=1\sin60^{\circ}=\frac{\sqrt3}{2}\ne2\times\frac12=1.

Key termscounter-example
Exam tip

Check an identity by substituting a value such as θ=π6\theta=\frac{\pi}{6}. A check does not prove it, but a mismatch shows an error.

Section 4

Applications: kinematics and projectiles

A projectile launched at speed uu at angle θ\theta to the horizontal has components ucos⁡θu\cos\theta (horizontal, constant) and usin⁡θu\sin\theta (initial vertical). Landing on level ground needs 0=(usin⁡θ)T−12gT20=(u\sin\theta)T-\frac12gT^2, so T=2usin⁡θgT=\frac{2u\sin\theta}{g}. Range=ucos⁡θ×T=2u2sin⁡θcos⁡θg=u2sin⁡2θg.\text{Range}=u\cos\theta\times T=\frac{2u^2\sin\theta\cos\theta}{g}=\frac{u^2\sin2\theta}{g}. The range is greatest when sin⁡2θ=1\sin2\theta=1, so θ=45∘\theta=45^{\circ}. For a range less than the maximum, sin⁡2θ=sin⁡(180∘−2θ)\sin2\theta=\sin(180^{\circ}-2\theta) gives two angles that sum to 90∘90^{\circ}. Example: u=20u=20, range 30 m: sin⁡2θ=30×9.8400=0.735\sin2\theta=\frac{30\times9.8}{400}=0.735, so θ=23.7∘\theta=23.7^{\circ} or 66.3∘66.3^{\circ}.

Key termsprojectilerange
Common mistake

Using only the first solution of sin⁡2θ=k\sin2\theta=k. Two angles in 0<θ<90∘0<\theta<90^{\circ} usually fit.

Section 5

Applications: vectors and forces

Resolve a vector of magnitude FF at angle α\alpha to the xx-axis into components Fcos⁡αF\cos\alpha and Fsin⁡αF\sin\alpha. For two forces, add the components, then find the resultant magnitude with Pythagoras and its direction with tan⁡ϕ=verticalhorizontal\tan\phi=\frac{\text{vertical}}{\text{horizontal}}. Example: forces of 8 N along the xx-axis and 7 N at 60∘60^{\circ} to it. Horizontal: 8+7cos⁡60∘=11.58+7\cos60^{\circ}=11.5. Vertical: 7sin⁡60∘=7327\sin60^{\circ}=\frac{7\sqrt3}{2}. Magnitude =11.52+36.75=13=\sqrt{11.5^2+36.75}=13 N, at tan⁡−1(3.5311.5)=27.8∘\tan^{-1}\left(\frac{3.5\sqrt3}{11.5}\right)=27.8^{\circ} to the 8 N force. A force that balances them has the same magnitude and the opposite direction. On a slope at angle α\alpha, weight mgmg has components mgsin⁡αmg\sin\alpha down the slope and mgcos⁡αmg\cos\alpha into it.

Key termsresultantresolve
Common mistake

Using sin⁡\sin for the component along the axis the angle is measured from. That component uses cos⁡\cos.

Section 6

Modelling and communicating

In context questions state what the model assumes (no air resistance, a particle, a smooth surface), keep calculator values unrounded until the end, and give answers to 3 s.f. unless told otherwise. Check that the calculator is in radians or degrees as the question requires. After solving, return to the context: a range must be positive and a launch angle must lie between 0∘0^{\circ} and 90∘90^{\circ}, so reject solutions that do not fit.

Exam tip

Write the answer as a sentence with units, such as the range is 40.8 m.

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Exam questions on Trigonometric proofs and applications

  1. A student sets out to prove the identity sin⁡2θ1+cos⁡2θ≡tan⁡θ\frac{\sin2\theta}{1+\cos2\theta}\equiv\tan\theta.
    State the values of θ\theta in the interval 0≤θ≤2π0\le\theta\le2\pi for which the identity is not valid because both sides are undefined.2 marks
  2. Let f(x)=sin⁡4x−cos⁡4xf(x)=\sin^4x-\cos^4x, where xx is in radians.
    Hence solve f(x)=12f(x)=\frac12 for 0≤x≤π0\le x\le\pi.2 marks
  3. It is claimed that cos⁡θ+sin⁡θ≡2cos⁡(θ−π4)\cos\theta+\sin\theta\equiv\sqrt2\cos\left(\theta-\frac{\pi}{4}\right) for all values of θ\theta.
    Prove that the claim is true.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).