Year 2 Pure · Chapter 10

Addition and Double-Angle Formulae

Specification: Edexcel Pure 5.6–5.9 — Trigonometry  ·  AQA section E6, E7, E8, E9

In this chapter
  1. 1. The addition formulae
  2. 2. Double-angle formulae
  3. 3. The form R cos(θ − α)
  4. 4. Modelling with the R form
  5. Practice

Key facts — this chapter

  • 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.
  • tan⁡(A±B)≡tan⁡A±tan⁡B1∓tan⁡Atan⁡B\tan(A \pm B) \equiv \dfrac{\tan A \pm \tan B}{1 \mp \tan A\tan B}.
  • sin⁡2A≡2sin⁡Acos⁡A\sin 2A \equiv 2\sin A\cos A, and cos⁡2A≡cos⁡2A−sin⁡2A≡2cos⁡2A−1≡1−2sin⁡2A\cos 2A \equiv \cos^2 A - \sin^2 A \equiv 2\cos^2 A - 1 \equiv 1 - 2\sin^2 A.
  • tan⁡2A≡2tan⁡A1−tan⁡2A\tan 2A \equiv \dfrac{2\tan A}{1 - \tan^2 A}.
  • acos⁡θ+bsin⁡θ≡Rcos⁡(θ−α)a\cos\theta + b\sin\theta \equiv R\cos(\theta - \alpha), where R=a2+b2R = \sqrt{a^2 + b^2} and tan⁡α=ba\tan\alpha = \frac{b}{a}. Its largest value is RR and its smallest is −R-R.
  • To solve acos⁡θ+bsin⁡θ=ca\cos\theta + b\sin\theta = c, write the left side in this form first.

sin⁡(A+B)\sin(A + B) is not sin⁡A+sin⁡B\sin A + \sin B: try A=B=π2A = B = \frac{\pi}{2}, which gives 00 on the left and 22 on the right. This chapter finds what it really is. The formulae that come out of it turn sums of sines and cosines into single waves, which is how a wave’s height and timing are found in models.

1. The addition formulae

Key result

sin⁡(A+B)≡sin⁡Acos⁡B+cos⁡Asin⁡Bsin⁡(A−B)≡sin⁡Acos⁡B−cos⁡Asin⁡Bcos⁡(A+B)≡cos⁡Acos⁡B−sin⁡Asin⁡Bcos⁡(A−B)≡cos⁡Acos⁡B+sin⁡Asin⁡B\begin{aligned} \sin(A + B) &\equiv \sin A\cos B + \cos A\sin B \\ \sin(A - B) &\equiv \sin A\cos B - \cos A\sin B \\ \cos(A + B) &\equiv \cos A\cos B - \sin A\sin B \\ \cos(A - B) &\equiv \cos A\cos B + \sin A\sin B \end{aligned}tan⁡(A±B)≡tan⁡A±tan⁡B1∓tan⁡Atan⁡B\tan(A \pm B) \equiv \frac{\tan A \pm \tan B}{1 \mp \tan A\tan B}

Watch the signs in the cosine formulae: a ++ inside the bracket gives a −- between the terms.

A line OP of length 1 at angle A plus B above the horizontal. A right-angled triangle OQP has its right angle at Q, with OQ at angle A, so OQ = cos B and QP = sin B. Perpendiculars from P and Q to the horizontal, and a horizontal from Q, split the height of P into sin B cos A plus cos B sin A
The height of P, which is sin(A + B), split into two pieces.

A geometric proof

In the figure, OP=1OP = 1 makes angle A+BA + B with the horizontal, so PP is at height sin⁡(A+B)\sin(A + B). The right-angled triangle OQPOQP has angle BB at OO, so OQ=cos⁡BOQ = \cos B and QP=sin⁡BQP = \sin B.

  • QQ is at height OQsin⁡A=cos⁡Bsin⁡AOQ\sin A = \cos B\sin A.
  • QPQP makes angle AA with the vertical, so PP is a further QPcos⁡A=sin⁡Bcos⁡AQP\cos A = \sin B\cos A above QQ.

Adding the two pieces, sin⁡(A+B)=sin⁡Acos⁡B+cos⁡Asin⁡B\sin(A + B) = \sin A\cos B + \cos A\sin B. The horizontal distances give cos⁡(A+B)=cos⁡Acos⁡B−sin⁡Asin⁡B\cos(A + B) = \cos A\cos B - \sin A\sin B in the same way. Replacing BB with −B-B gives the two minus formulae, and dividing sin⁡(A+B)\sin(A + B) by cos⁡(A+B)\cos(A + B) gives the one for tan⁡\tan.

Worked example 10.1 · An exact value

Find the exact value of cos⁡π12\cos\tfrac{\pi}{12}.


  1. Write π12\tfrac{\pi}{12} as a difference of angles you know: π12=π3−π4\tfrac{\pi}{12} = \tfrac{\pi}{3} - \tfrac{\pi}{4}.

  2. Use cos⁡(A−B)\cos(A - B):

    cos⁡π12=cos⁡π3cos⁡π4+sin⁡π3sin⁡π4=12×22+32×22=2+64\begin{aligned} &\cos\tfrac{\pi}{12} \\ &= \cos\tfrac{\pi}{3}\cos\tfrac{\pi}{4} + \sin\tfrac{\pi}{3}\sin\tfrac{\pi}{4} \\ &= \tfrac{1}{2} \times \tfrac{\sqrt2}{2} + \tfrac{\sqrt3}{2} \times \tfrac{\sqrt2}{2} \\ &= \tfrac{\sqrt2 + \sqrt6}{4} \end{aligned}

Worked example 10.2 · Two angles in different quadrants

AA is acute with sin⁡A=35\sin A = \tfrac{3}{5}, and BB is obtuse with cos⁡B=−513\cos B = -\tfrac{5}{13}. Find the exact value of sin⁡(A+B)\sin(A + B).


  1. Find the missing ratios, with the right signs. AA is acute, so cos⁡A=45\cos A = \tfrac{4}{5}. BB is obtuse, where sine is positive, so sin⁡B=1213\sin B = \tfrac{12}{13}.

  2. Substitute:

    sin⁡(A+B)=35×(−513)+45×1213=−15+4865=3365\begin{aligned} &\sin(A + B) \\ &= \tfrac{3}{5} \times \left(-\tfrac{5}{13}\right) + \tfrac{4}{5} \times \tfrac{12}{13} \\ &= \tfrac{-15 + 48}{65} = \tfrac{33}{65} \end{aligned}

Worked example 10.3 · Undoing the formula

Given that tan⁡(x+π4)=3\tan\left(x + \tfrac{\pi}{4}\right) = 3, find the exact value of tan⁡x\tan x.


tan⁡π4=1\tan\tfrac{\pi}{4} = 1, so the formula gives

tan⁡x+11−tan⁡x=3tan⁡x+1=3−3tan⁡xtan⁡x=12\begin{aligned} \frac{\tan x + 1}{1 - \tan x} &= 3 \\ \tan x + 1 &= 3 - 3\tan x \\ \tan x &= \tfrac{1}{2} \end{aligned}

2. Double-angle formulae

Put B=AB = A in the addition formulae and they become the double-angle formulae. Using sin⁡2A+cos⁡2A≡1\sin^2 A + \cos^2 A \equiv 1 turns the cosine one into three versions: choose the one that leaves only the function you want.

Key result

sin⁡2A≡2sin⁡Acos⁡Acos⁡2A≡cos⁡2A−sin⁡2A≡2cos⁡2A−1≡1−2sin⁡2Atan⁡2A≡2tan⁡A1−tan⁡2A\begin{aligned} \sin 2A &\equiv 2\sin A\cos A \\ \cos 2A &\equiv \cos^2 A - \sin^2 A \\ &\equiv 2\cos^2 A - 1 \\ &\equiv 1 - 2\sin^2 A \\ \tan 2A &\equiv \frac{2\tan A}{1 - \tan^2 A} \end{aligned}

Rearranging the cosine versions gives cos⁡2A≡12(1+cos⁡2A)\cos^2 A \equiv \frac{1}{2}(1 + \cos 2A) and sin⁡2A≡12(1−cos⁡2A)\sin^2 A \equiv \frac{1}{2}(1 - \cos 2A). With A=x2A = \frac{x}{2} these are the half-angle formulae, and they are what you’ll use to integrate sin⁡2x\sin^2 x and cos⁡2x\cos^2 x in Chapter 15.

Worked example 10.4 · Double angles from a single ratio

Given that cos⁡x=13\cos x = \tfrac{1}{3} and xx is acute, find the exact values of sin⁡2x\sin 2x and cos⁡2x\cos 2x.


  1. sin⁡x=1−19=223\sin x = \sqrt{1 - \tfrac{1}{9}} = \tfrac{2\sqrt2}{3}, positive because xx is acute.

  2. Then

    sin⁡2x=2×223×13=429cos⁡2x=2×19−1=−79\begin{aligned} \sin 2x &= 2 \times \tfrac{2\sqrt2}{3} \times \tfrac{1}{3} = \tfrac{4\sqrt2}{9} \\ \cos 2x &= 2 \times \tfrac{1}{9} - 1 = -\tfrac{7}{9} \end{aligned}

Worked example 10.5 · Solving with a double angle

Solve sin⁡2x=sin⁡x\sin 2x = \sin x for 0≤x≤2π0 \le x \le 2\pi.


  1. Expand and factorise. Don’t divide by sin⁡x\sin x, which would lose solutions:

    2sin⁡xcos⁡x−sin⁡x=0sin⁡x (2cos⁡x−1)=0\begin{aligned} 2\sin x\cos x - \sin x &= 0 \\ \sin x\,(2\cos x - 1) &= 0 \end{aligned}
  2. sin⁡x=0\sin x = 0 gives x=0,π,2πx = 0, \pi, 2\pi. cos⁡x=12\cos x = \tfrac{1}{2} gives x=π3,5π3x = \tfrac{\pi}{3}, \tfrac{5\pi}{3}.

So x=0, π3, π, 5π3, 2πx = 0,\ \tfrac{\pi}{3},\ \pi,\ \tfrac{5\pi}{3},\ 2\pi.

Worked example 10.6 · Choosing the right version

Solve cos⁡2x=5cos⁡x−3\cos 2x = 5\cos x - 3 for 0≤x<2π0 \le x < 2\pi.


  1. The right side has cos⁡x\cos x, so use cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1:

    2cos⁡2x−1=5cos⁡x−32cos⁡2x−5cos⁡x+2=0(2cos⁡x−1)(cos⁡x−2)=0\begin{aligned} &2\cos^2 x - 1 = 5\cos x - 3 \\ &2\cos^2 x - 5\cos x + 2 = 0 \\ &(2\cos x - 1)(\cos x - 2) = 0 \end{aligned}
  2. cos⁡x=2\cos x = 2 is impossible, so cos⁡x=12\cos x = \tfrac{1}{2} and x=π3x = \tfrac{\pi}{3} or 5π3\tfrac{5\pi}{3}.

Worked example 10.7 · Proving an identity

Prove that 1−cos⁡2θsin⁡2θ≡tan⁡θ\dfrac{1 - \cos 2\theta}{\sin 2\theta} \equiv \tan\theta.


Use cos⁡2θ≡1−2sin⁡2θ\cos 2\theta \equiv 1 - 2\sin^2\theta, which makes the 11s cancel:

1−cos⁡2θsin⁡2θ≡2sin⁡2θ2sin⁡θcos⁡θ≡sin⁡θcos⁡θ≡tan⁡θ\begin{aligned} \frac{1 - \cos 2\theta}{\sin 2\theta} &\equiv \frac{2\sin^2\theta}{2\sin\theta\cos\theta} \\ &\equiv \frac{\sin\theta}{\cos\theta} \equiv \tan\theta \end{aligned}

3. The form R cos(θ − α)

Adding a cosine wave and a sine wave with the same period gives another wave with that period: it’s just taller and shifted along. Writing it as a single cosine tells you its height and where its peaks are.

Key result

For positive aa and bb,

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

where R=a2+b2R = \sqrt{a^2 + b^2} and tan⁡α=ba\tan\alpha = \frac{b}{a}, with 0<α<π20 < \alpha < \frac{\pi}{2}.

The same method gives the other forms: Rcos⁡(θ+α)R\cos(\theta + \alpha) for acos⁡θ−bsin⁡θa\cos\theta - b\sin\theta, and Rsin⁡(θ±α)R\sin(\theta \pm \alpha) for asin⁡θ±bcos⁡θa\sin\theta \pm b\cos\theta.

Left: a right-angled triangle with sides 3 and 4 and hypotenuse R = 5, with the angle alpha between the side 3 and the hypotenuse. Right: the graph of y = 3 cos theta + 4 sin theta, a single wave of height 5 whose first peak is at theta = alpha, with the two separate waves 3 cos theta (dashed) and 4 sin theta (dotted) drawn faintly
3 cos θ (dashed) plus 4 sin θ (dotted) is one wave of height R = 5, peaking at θ = α. The triangle gives R and α.

To see why, expand the right side:

Rcos⁡(θ−α)=Rcos⁡αcos⁡θ+Rsin⁡αsin⁡θ\begin{aligned} R\cos(\theta - \alpha) &= R\cos\alpha\cos\theta \\ &\quad + R\sin\alpha\sin\theta \end{aligned}

Matching the coefficients with acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta needs

Rcos⁡α=aandRsin⁡α=bR\cos\alpha = a \quad\text{and}\quad R\sin\alpha = b

Squaring and adding gives R2=a2+b2R^2 = a^2 + b^2. Dividing gives tan⁡α=ba\tan\alpha = \frac{b}{a}.

Choose a and b. The faint waves are a cos θ and b sin θ; the solid one is their sum. However you choose them, the sum is a single cosine wave, and the right-angled triangle on the left gives its height R and its shift α.

Worked example 10.8 · Writing it as one wave

Express 3cos⁡θ+4sin⁡θ3\cos\theta + 4\sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha), where R>0R > 0 and 0<α<π20 < \alpha < \tfrac{\pi}{2}. State its maximum value and the smallest positive value of θ\theta where it occurs.


  1. Rcos⁡α=3R\cos\alpha = 3 and Rsin⁡α=4R\sin\alpha = 4, so

    R=32+42=5α=tan⁡−143=0.9272…\begin{aligned} R &= \sqrt{3^2 + 4^2} = 5 \\ \alpha &= \tan^{-1}\tfrac{4}{3} = 0.9272\ldots \end{aligned}

    So 3cos⁡θ+4sin⁡θ=5cos⁡(θ−0.927)3\cos\theta + 4\sin\theta = 5\cos(\theta - 0.927), to 3 s.f.

  2. The largest value of a cosine is 11, so the maximum is 55, when θ−α=0\theta - \alpha = 0, that is θ=0.927\theta = 0.927 (3 s.f.).

Worked example 10.9 · Solving with the R form

Solve 3cos⁡θ+4sin⁡θ=23\cos\theta + 4\sin\theta = 2 for 0≤θ<2π0 \le \theta < 2\pi, giving your answers to 3 significant figures.


  1. From Example 10.8, 5cos⁡(θ−α)=25\cos(\theta - \alpha) = 2, so cos⁡(θ−α)=0.4\cos(\theta - \alpha) = 0.4, where α=0.9272…\alpha = 0.9272\ldots

  2. As θ\theta runs from 00 to 2π2\pi, θ−α\theta - \alpha runs from −0.927-0.927 to 5.3565.356. In that interval,

    θ−α=1.1592… or 5.1239…\theta - \alpha = 1.1592\ldots \text{ or } 5.1239\ldots

    (−1.159-1.159 is too small to be in the interval.)

  3. Add α\alpha: θ=2.09\theta = 2.09 or θ=6.05\theta = 6.05 (3 s.f.).

Common mistake

Find α\alpha from tan⁡α=ba\tan\alpha = \frac{b}{a}, not ab\frac{a}{b}: the sin⁡α\sin\alpha coefficient goes on top. Then check by expanding: 5cos⁡(θ−0.927)5\cos(\theta - 0.927) should give back 3cos⁡θ+4sin⁡θ3\cos\theta + 4\sin\theta.

4. Modelling with the R form

Worked example 10.10 · Temperature in a greenhouse

The temperature in a greenhouse, TT °C, tt hours after midnight is modelled by T=20−3cos⁡(πt12)−4sin⁡(πt12)T = 20 - 3\cos\left(\tfrac{\pi t}{12}\right) - 4\sin\left(\tfrac{\pi t}{12}\right). Find the highest temperature and the time of day at which it happens.


  1. Write θ=πt12\theta = \tfrac{\pi t}{12}. By Example 10.8, 3cos⁡θ+4sin⁡θ=5cos⁡(θ−α)3\cos\theta + 4\sin\theta = 5\cos(\theta - \alpha) with α=0.9272…\alpha = 0.9272\ldots, so T=20−5cos⁡(θ−α)T = 20 - 5\cos(\theta - \alpha).

  2. TT is largest when the cosine is −1-1, so the highest temperature is 20+5=2520 + 5 = 25 °C.

  3. That happens when θ−α=π\theta - \alpha = \pi:

    πt12=π+0.9272…t=15.542 (3 d.p.)\begin{aligned} \tfrac{\pi t}{12} &= \pi + 0.9272\ldots \\ t &= 15.542 \text{ (3 d.p.)} \end{aligned}

    0.5420.542 hours is 3333 minutes to the nearest minute, so the greenhouse is warmest at about 3:33 pm.

Practice

Twelve questions in three tiers. Try each one properly before opening the solution — the solutions show full method, not just answers.

Warm-up

1 [3 marks]

Find the exact value of sin⁡π12\sin\tfrac{\pi}{12}.

Show solution

π12=π3−π4\tfrac{\pi}{12} = \tfrac{\pi}{3} - \tfrac{\pi}{4}, so use sin⁡(A−B)\sin(A - B):

sin⁡π12=sin⁡π3cos⁡π4−cos⁡π3sin⁡π4=32×22−12×22=6−24\begin{aligned} \sin\tfrac{\pi}{12} &= \sin\tfrac{\pi}{3}\cos\tfrac{\pi}{4} - \cos\tfrac{\pi}{3}\sin\tfrac{\pi}{4} \\ &= \tfrac{\sqrt3}{2} \times \tfrac{\sqrt2}{2} - \tfrac{1}{2} \times \tfrac{\sqrt2}{2} \\ &= \tfrac{\sqrt6 - \sqrt2}{4} \end{aligned}
2 [3 marks]

Write each of these as a single trigonometric function or an exact value.

  1. sin⁡3xcos⁡x+cos⁡3xsin⁡x\sin 3x\cos x + \cos 3x\sin x [1]
  2. cos⁡22x−sin⁡22x\cos^2 2x - \sin^2 2x [1]
  3. 2sin⁡π8cos⁡π82\sin\tfrac{\pi}{8}\cos\tfrac{\pi}{8} [1]
Show solution

(a) sin⁡(3x+x)=sin⁡4x\sin(3x + x) = \sin 4x.

(b) cos⁡(2×2x)=cos⁡4x\cos(2 \times 2x) = \cos 4x.

(c) sin⁡(2×π8)=sin⁡π4=22\sin\left(2 \times \tfrac{\pi}{8}\right) = \sin\tfrac{\pi}{4} = \tfrac{\sqrt2}{2}.

3 [3 marks]

AA and BB are acute angles with tan⁡A=12\tan A = \tfrac{1}{2} and tan⁡B=13\tan B = \tfrac{1}{3}. Find tan⁡(A+B)\tan(A + B), and hence show that A+B=π4A + B = \tfrac{\pi}{4}.

Show solution
tan⁡(A+B)=12+131−12×13=5656=1\tan(A + B) = \frac{\frac12 + \frac13}{1 - \frac12 \times \frac13} = \frac{\frac56}{\frac56} = 1

AA and BB are acute, so 0<A+B<π0 < A + B < \pi, and the only angle there with tangent 11 is π4\tfrac{\pi}{4}.

4 [2 marks]

Given that sin⁡x=14\sin x = \tfrac{1}{4}, find the exact value of cos⁡2x\cos 2x.

Show solution

Use the version with sin⁡\sin only: cos⁡2x=1−2sin⁡2x=1−216=78\cos 2x = 1 - 2\sin^2 x = 1 - \tfrac{2}{16} = \tfrac{7}{8}.

Standard

5 [4 marks]

Solve cos⁡2x=cos⁡x\cos 2x = \cos x for 0≤x≤2π0 \le x \le 2\pi.

Show solution

Use cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1:

2cos⁡2x−cos⁡x−1=0(2cos⁡x+1)(cos⁡x−1)=0\begin{aligned} 2\cos^2 x - \cos x - 1 &= 0 \\ (2\cos x + 1)(\cos x - 1) &= 0 \end{aligned}

cos⁡x=1\cos x = 1 gives x=0x = 0 or 2π2\pi, and cos⁡x=−12\cos x = -\tfrac{1}{2} gives x=2π3x = \tfrac{2\pi}{3} or 4π3\tfrac{4\pi}{3}. So x=0, 2π3, 4π3, 2πx = 0,\ \tfrac{2\pi}{3},\ \tfrac{4\pi}{3},\ 2\pi.

6 [4 marks]

Prove that tan⁡θ+cot⁡θ≡2cosec⁡2θ\tan\theta + \cot\theta \equiv 2\operatorname{cosec} 2\theta.

Show solution
tan⁡θ+cot⁡θ≡sin⁡θcos⁡θ+cos⁡θsin⁡θ≡sin⁡2θ+cos⁡2θsin⁡θcos⁡θ≡112sin⁡2θ≡2cosec⁡2θ\begin{aligned} \tan\theta + \cot\theta &\equiv \frac{\sin\theta}{\cos\theta} + \frac{\cos\theta}{\sin\theta} \\ &\equiv \frac{\sin^2\theta + \cos^2\theta}{\sin\theta\cos\theta} \\ &\equiv \frac{1}{\frac{1}{2}\sin 2\theta} \equiv 2\operatorname{cosec} 2\theta \end{aligned}
7 [6 marks]
  1. Express 3cos⁡θ+sin⁡θ\sqrt3\cos\theta + \sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha), where R>0R > 0 and 0<α<π20 < \alpha < \tfrac{\pi}{2}, giving exact values of RR and α\alpha. [3]
  2. Hence solve 3cos⁡θ+sin⁡θ=2\sqrt3\cos\theta + \sin\theta = \sqrt2 for 0≤θ<2π0 \le \theta < 2\pi. [3]
Show solution

(a) Rcos⁡α=3R\cos\alpha = \sqrt3 and Rsin⁡α=1R\sin\alpha = 1, so R=3+1=2R = \sqrt{3 + 1} = 2 and tan⁡α=13\tan\alpha = \tfrac{1}{\sqrt3}, giving α=π6\alpha = \tfrac{\pi}{6}. So the expression is 2cos⁡(θ−π6)2\cos\left(\theta - \tfrac{\pi}{6}\right).

(b) cos⁡(θ−π6)=22\cos\left(\theta - \tfrac{\pi}{6}\right) = \tfrac{\sqrt2}{2}. As θ\theta runs from 00 to 2π2\pi, θ−π6\theta - \tfrac{\pi}{6} runs from −π6-\tfrac{\pi}{6} to 11π6\tfrac{11\pi}{6}, and in that interval

θ−π6=π4 or 7π4\theta - \tfrac{\pi}{6} = \tfrac{\pi}{4} \text{ or } \tfrac{7\pi}{4}

So θ=5π12\theta = \tfrac{5\pi}{12} or 23π12\tfrac{23\pi}{12}.

8 [4 marks]

AA is obtuse with cos⁡A=−45\cos A = -\tfrac{4}{5}, and BB is acute with sin⁡B=1213\sin B = \tfrac{12}{13}. Find the exact value of cos⁡(A−B)\cos(A - B).

Show solution

AA is obtuse, so sin⁡A=35\sin A = \tfrac{3}{5} (positive). BB is acute, so cos⁡B=513\cos B = \tfrac{5}{13}. Then

cos⁡(A−B)=−45×513+35×1213=−20+3665=1665\begin{aligned} &\cos(A - B) \\ &= -\tfrac{4}{5} \times \tfrac{5}{13} + \tfrac{3}{5} \times \tfrac{12}{13} \\ &= \tfrac{-20 + 36}{65} = \tfrac{16}{65} \end{aligned}
9 [5 marks]
  1. Show that cos⁡3x≡4cos⁡3x−3cos⁡x\cos 3x \equiv 4\cos^3 x - 3\cos x. [4]
  2. Hence find the exact value of cos⁡3x\cos 3x when cos⁡x=13\cos x = \tfrac{1}{3}. [1]
Show solution

(a) Write 3x3x as 2x+x2x + x:

cos⁡3x≡cos⁡2xcos⁡x−sin⁡2xsin⁡x≡(2cos⁡2x−1)cos⁡x−2sin⁡2xcos⁡x≡2cos⁡3x−cos⁡x−2(1−cos⁡2x)cos⁡x≡4cos⁡3x−3cos⁡x\begin{aligned} &\cos 3x \\ &\equiv \cos 2x\cos x - \sin 2x\sin x \\ &\equiv (2\cos^2 x - 1)\cos x - 2\sin^2 x\cos x \\ &\equiv 2\cos^3 x - \cos x \\ &\quad - 2(1 - \cos^2 x)\cos x \\ &\equiv 4\cos^3 x - 3\cos x \end{aligned}

(b) 4×127−3×13=427−1=−23274 \times \tfrac{1}{27} - 3 \times \tfrac{1}{3} = \tfrac{4}{27} - 1 = -\tfrac{23}{27}.

Exam style

10 [8 marks]
  1. Express 5sin⁡θ−12cos⁡θ5\sin\theta - 12\cos\theta in the form Rsin⁡(θ−α)R\sin(\theta - \alpha), where R>0R > 0 and 0<α<π20 < \alpha < \tfrac{\pi}{2}. Give α\alpha to 4 decimal places. [3]
  2. State the maximum value of 5sin⁡θ−12cos⁡θ5\sin\theta - 12\cos\theta, and the smallest positive value of θ\theta at which it occurs. [2]
  3. Solve 5sin⁡θ−12cos⁡θ=6.55\sin\theta - 12\cos\theta = 6.5 for 0≤θ<2π0 \le \theta < 2\pi, to 3 significant figures. [3]
Show solution

(a) Rsin⁡(θ−α)=Rcos⁡αsin⁡θ−Rsin⁡αcos⁡θR\sin(\theta - \alpha) = R\cos\alpha\sin\theta - R\sin\alpha\cos\theta, so Rcos⁡α=5R\cos\alpha = 5 and Rsin⁡α=12R\sin\alpha = 12. Then R=25+144=13R = \sqrt{25 + 144} = 13 and α=tan⁡−1125=1.1760\alpha = \tan^{-1}\tfrac{12}{5} = 1.1760 (4 d.p.).

(b) The maximum is 1313, when θ−α=π2\theta - \alpha = \tfrac{\pi}{2}, that is θ=π2+1.1760=2.75\theta = \tfrac{\pi}{2} + 1.1760 = 2.75 (3 s.f.).

(c) sin⁡(θ−α)=6.513=12\sin(\theta - \alpha) = \tfrac{6.5}{13} = \tfrac{1}{2}. As θ\theta runs from 00 to 2π2\pi, θ−α\theta - \alpha runs from −1.176-1.176 to 5.1075.107, and in that interval θ−α=π6\theta - \alpha = \tfrac{\pi}{6} or 5π6\tfrac{5\pi}{6}. So

θ=1.1760+0.5236=1.70θ=1.1760+2.6180=3.79\begin{aligned} \theta &= 1.1760 + 0.5236 = 1.70 \\ \theta &= 1.1760 + 2.6180 = 3.79 \end{aligned}

to 3 significant figures.

11 [8 marks]

The depth of water in a harbour, DD metres, tt hours after midnight is modelled by

D=5+1.5cos⁡(πt6)+2sin⁡(πt6)D = 5 + 1.5\cos\left(\tfrac{\pi t}{6}\right) + 2\sin\left(\tfrac{\pi t}{6}\right)
  1. Write DD in the form 5+Rcos⁡(πt6−α)5 + R\cos\left(\tfrac{\pi t}{6} - \alpha\right), giving RR exactly and α\alpha to 4 decimal places. [3]
  2. Find the greatest depth, and the first time after midnight when it occurs, to the nearest minute. [3]
  3. State the least depth. [1]
  4. Give one reason why the model may not be realistic. [1]
Show solution

(a) Rcos⁡α=1.5R\cos\alpha = 1.5 and Rsin⁡α=2R\sin\alpha = 2, so R=2.25+4=2.5R = \sqrt{2.25 + 4} = 2.5 and α=tan⁡−143=0.9273\alpha = \tan^{-1}\tfrac{4}{3} = 0.9273 (4 d.p.). So D=5+2.5cos⁡(πt6−0.9273)D = 5 + 2.5\cos\left(\tfrac{\pi t}{6} - 0.9273\right).

(b) The greatest depth is 5+2.5=7.55 + 2.5 = 7.5 m, when the cosine is 11, so πt6=0.9272…\tfrac{\pi t}{6} = 0.9272\ldots and t=1.7710…t = 1.7710\ldots Then 0.77100.7710 hours is 4646 minutes, so this is at about 1:46 am.

(c) 5−2.5=2.55 - 2.5 = 2.5 m.

(d) For example, real tides don’t repeat exactly every 1212 hours, and the depth also depends on the weather.

12 [6 marks]
  1. Prove that sin⁡2θ1+cos⁡2θ≡tan⁡θ\dfrac{\sin 2\theta}{1 + \cos 2\theta} \equiv \tan\theta. [3]
  2. Hence solve sin⁡4x1+cos⁡4x=3\dfrac{\sin 4x}{1 + \cos 4x} = \sqrt3 for 0≤x≤π0 \le x \le \pi. [3]
Show solution

(a) Use cos⁡2θ≡2cos⁡2θ−1\cos 2\theta \equiv 2\cos^2\theta - 1, which makes the 11s cancel:

sin⁡2θ1+cos⁡2θ≡2sin⁡θcos⁡θ2cos⁡2θ≡tan⁡θ\frac{\sin 2\theta}{1 + \cos 2\theta} \equiv \frac{2\sin\theta\cos\theta}{2\cos^2\theta} \equiv \tan\theta

(b) With θ=2x\theta = 2x, the equation is tan⁡2x=3\tan 2x = \sqrt3. As xx runs from 00 to π\pi, 2x2x runs from 00 to 2π2\pi, so 2x=π32x = \tfrac{\pi}{3} or 4π3\tfrac{4\pi}{3}, and x=π6x = \tfrac{\pi}{6} or 2π3\tfrac{2\pi}{3}. At both, 1+cos⁡4x=12≠01 + \cos 4x = \tfrac{1}{2} \neq 0, so the original fraction is defined.