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Further trigonometry – Year 13 A level maths worksheet answers to download as PDF

Year 13 further trigonometry worksheet answers – Otto the owl, Maths PDF
A Level Maths Year 13 – Worksheets with Answers – PDF
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These Year 13 further trigonometry worksheet answers give a full worked solution to all 20 questions of the further trigonometry worksheet. Try each question yourself first, then check your method step by step.

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  1. Answer to Question 1

    1. \(\cos0.06\approx1-\dfrac{0.0036}2=1-0.0018=0.9982\). The calculator gives 0.998201, so the approximation is accurate to 4 decimal places.
    2. \(1-\cos4\theta\approx\dfrac{(4\theta)^2}2=8\theta^2\) and \(\theta\sin2\theta\approx\theta\cdot2\theta=2\theta^2\). The ratio is approximately \(\dfrac{8\theta^2}{2\theta^2}=\) 4.
    3. \(\sin3\theta\approx3\theta\) and \(\tan2\theta\approx2\theta\), so the numerator is \(\approx6\theta^2\) and the ratio is approximately 6.
  2. Answer to Question 2

    Method: \(\sec\theta=\dfrac1{\cos\theta}\), \(\operatorname{cosec}\theta=\dfrac1{\sin\theta}\) and \(\cot\theta=\dfrac1{\tan\theta}\). Find the sine, cosine or tangent first (with its sign from the quadrant), then take the reciprocal.

    1. Use \(\cos60^\circ=\tfrac12\) and \(\sin30^\circ=\tfrac12\). \(\sec60^\circ=\dfrac1{\cos60^\circ}=\dfrac1{1/2}=2\). \(\operatorname{cosec}30^\circ=\dfrac1{\sin30^\circ}=2\). Both values are equal to 2.
    2. \(150^\circ\) is in the second quadrant, where tangent is negative. \(\cot45^\circ=\dfrac1{\tan45^\circ}=1\). \(\tan150^\circ=-\dfrac1{\sqrt3}\) so \(\cot150^\circ=-\sqrt3\). So \(\cot45^\circ=1\) and \(\cot150^\circ=-\sqrt3\).
    3. \(120^\circ\) is in the second quadrant (cosine negative) and \(240^\circ\) in the third (sine negative). \(\cos120^\circ=-\tfrac12\), so \(\sec120^\circ=-2\). \(\sin240^\circ=-\dfrac{\sqrt3}2\), so \(\operatorname{cosec}240^\circ=-\dfrac2{\sqrt3}=-\dfrac{2\sqrt3}3\). Rationalising the denominator gives the neat form \(-\dfrac{2\sqrt3}3\).
  3. Answer to Question 3

    1. \(\cos x=-\tfrac12\) so \(x=\) 120Β°, 240Β°.
    2. Use \(\tan^2x=\sec^2x-1\): \(\sec^2x-1+\sec x=1\), so \(\sec^2x+\sec x-2=0\), \((\sec x+2)(\sec x-1)=0\). \(\sec x=1\) gives \(x=0^\circ\). \(\sec x=-2\) gives \(x=120^\circ,240^\circ\). Solutions: 0Β°, 120Β°, 240Β°.
    3. Use \(\operatorname{cosec}^2x=1+\cot^2x\): \(\cot^2x-\cot x-2=0\), \((\cot x-2)(\cot x+1)=0\). \(\cot x=2\): \(\tan x=\tfrac12\), \(x=26.6^\circ,206.6^\circ\). \(\cot x=-1\): \(\tan x=-1\), \(x=135^\circ,315^\circ\). Solutions: 26.6Β°, 135Β°, 206.6Β°, 315Β°.
  4. Answer to Question 4

    Method: use the compound angle formulae \(\sin(A\pm B)=\sin A\cos B\pm\cos A\sin B\), \(\cos(A\pm B)=\cos A\cos B\mp\sin A\sin B\) and \(\tan(A\pm B)=\dfrac{\tan A\pm\tan B}{1\mp\tan A\tan B}\), with exact values of \(30^\circ\), \(45^\circ\) and \(60^\circ\).

    1. Use \(\sin(A-B)\) with \(A=45^\circ\) and \(B=30^\circ\). \(\sin(45^\circ-30^\circ)=\sin45^\circ\cos30^\circ-\cos45^\circ\sin30^\circ=\dfrac{\sqrt2}2\cdot\dfrac{\sqrt3}2-\dfrac{\sqrt2}2\cdot\dfrac12=\dfrac{\sqrt6-\sqrt2}4\). So \(\sin15^\circ=\dfrac{\sqrt6-\sqrt2}4\approx0.2588\).
    2. Write \(75^\circ=45^\circ+30^\circ\) and use \(\cos(A+B)\). \(\cos(45^\circ+30^\circ)=\cos45^\circ\cos30^\circ-\sin45^\circ\sin30^\circ=\dfrac{\sqrt6}4-\dfrac{\sqrt2}4=\dfrac{\sqrt6-\sqrt2}4\). This equals \(\sin15^\circ\), as expected since \(\cos75^\circ=\sin(90^\circ-75^\circ)\).
    3. Use \(\tan60^\circ=\sqrt3\) and \(\tan45^\circ=1\), then rationalise the denominator. \(\tan(60^\circ+45^\circ)=\dfrac{\sqrt3+1}{1-\sqrt3}\). Multiply by \(\dfrac{1+\sqrt3}{1+\sqrt3}\): \(\dfrac{(\sqrt3+1)^2}{1-3}=\dfrac{4+2\sqrt3}{-2}=-(2+\sqrt3)\). The answer is negative because \(105^\circ\) is in the second quadrant.
  5. Answer to Question 5

    1. \(2\sin x\cos x-\sin x=0\), so \(\sin x(2\cos x-1)=0\) (do not divide by \(\sin x\)). \(\sin x=0\) gives \(x=0^\circ,180^\circ\). \(\cos x=\tfrac12\) gives \(x=60^\circ,300^\circ\). Solutions: 0Β°, 60Β°, 180Β°, 300Β°.
    2. Use \(\cos2x=2\cos^2x-1\): \(2\cos^2x+3\cos x+1=0\), \((2\cos x+1)(\cos x+1)=0\). \(\cos x=-\tfrac12\) gives \(x=120^\circ,240^\circ\). \(\cos x=-1\) gives \(x=180^\circ\). Solutions: 120Β°, 180Β°, 240Β°.
  6. Answer to Question 6

    1. \(R\sin(x+\alpha)=R\sin x\cos\alpha+R\cos x\sin\alpha\). Comparing: \(R\cos\alpha=5\), \(R\sin\alpha=12\). \(R=\sqrt{25+144}=13\) and \(\tan\alpha=\dfrac{12}5\), so \(\alpha=67.38^\circ\). Hence \(f(x)=13\sin(x+67.38^\circ)\).
    2. Maximum 13, minimum \(-13\). The maximum occurs when \(x+67.38^\circ=90^\circ\), so \(x=22.62^\circ\).
    3. \(13\sin(x+67.38^\circ)=6.5\) gives \(\sin(x+67.38^\circ)=0.5\). So \(x+67.38^\circ=30^\circ,150^\circ,390^\circ\) (the values \(30^\circ\) gives a negative \(x\)). \(x=82.62^\circ\) or \(x=322.62^\circ\). Solutions: 82.6Β°, 322.6Β°.
  7. Answer to Question 7

    Method: the small-angle approximations only work in radians: \(\sin\theta\approx\theta\), \(\tan\theta\approx\theta\), \(\cos\theta\approx1-\dfrac{\theta^2}{2}\). Replace each function, simplify, and the powers of \(\theta\) usually cancel.

    1. 0.08 radians is a small angle, so replace \(\tan0.08\) by \(0.08\). \(\tan\theta\approx\theta\), so \(h\approx400\times0.08=\) 32 m. So the tower is about 32 m tall.
    2. Use the calculator in radian mode. \(h=400\tan0.08=400\times0.080171=\) 32.1 m. So the true height is about 32.1 m.
    3. Divide the difference by the true value and multiply by 100. Error \(=\dfrac{32.068-32}{32.068}\times100=0.21\%\). So the approximation is very good, with an error of about 0.2%.
    4. Compare the approximation with the true value for a large angle. The approximation needs \(\theta\) close to 0. For \(\theta=1\), \(\tan1=1.557\) but the approximation gives 1, an error of over 35%. So small-angle approximations should only be used for angles close to zero.
  8. Answer to Question 8

    Method: \(\sec\theta=\dfrac1{\cos\theta}\), \(\operatorname{cosec}\theta=\dfrac1{\sin\theta}\) and \(\cot\theta=\dfrac1{\tan\theta}\). Find the sine, cosine or tangent first (with its sign from the quadrant), then take the reciprocal.

    1. Use \(\operatorname{cosec}5^\circ=\dfrac1{\sin5^\circ}\) and \(\cot5^\circ=\dfrac1{\tan5^\circ}\). \(L=\dfrac{0.45}{\sin5^\circ}=5.16\) m and \(d=0.45\cot5^\circ=\dfrac{0.45}{\tan5^\circ}=5.14\) m. The two lengths are close because the angle is small.
    2. A gradient of 1 in 12 means a rise of 1 m for every 12 m across. \(\tan\theta=\tfrac1{12}\) gives \(\theta=\arctan\dfrac1{12}=4.76^\circ\). The ramp must be at most 4.76Β°. So the angle must be at most \(4.76^\circ\).
    3. A smaller angle gives a longer ramp, so the largest allowed angle gives the shortest ramp. The minimum length is \(L=0.45\operatorname{cosec}4.76^\circ=5.42\) m and the run is \(d=0.45\times12=5.4\) m. The 5Β° ramp is slightly too steep. So the ramp must be at least 5.42 m long, with a horizontal run of 5.4 m.
  9. Answer to Question 9

    1. \(R=\sqrt{9+16}=5\), \(\tan\alpha=\dfrac43\), \(\alpha=53.13^\circ\). So \(h=6+5\sin(30t+53.13)^\circ\).
    2. Greatest depth \(6+5=11\) m, least depth \(6-5=1\) m.
    3. Need \(5\sin(30t+53.13)^\circ\ge3\), so \(\sin(30t+53.13)^\circ\ge0.6\). \(\sin^{-1}0.6=36.87^\circ\), so the argument lies between \(36.87^\circ\) and \(143.13^\circ\), or between \(396.87^\circ\) and \(503.13^\circ\). First interval: \(0\le30t\le90\), giving \(0\le t\le3\). Second interval: \(343.74\le30t\le360\) (the limit of the range), giving \(11.46\le t\le12\). So boats can enter from midnight until 03:00, and from about 11:28 onwards (11.46 h \(=\) 11 h 27.5 min).
  10. Answer to Question 10

    1. The range is largest when \(\sin2\theta\) takes its largest value. The maximum value of \(\sin2\theta\) is 1, when \(2\theta=90^\circ\), so \(\theta=45^\circ\). Maximum range \(=\dfrac{400}{9.8}=40.8\) m. So the maximum range is about 40.8 m, at an angle of \(45^\circ\).
    2. Substitute \(R=30\), \(u=20\) and \(g=9.8\), then rearrange. \(30=\dfrac{400\sin2\theta}{9.8}\) gives \(\sin2\theta=\dfrac{294}{400}=0.735\). This is the required result.
    3. Since \(0^\circ<2\theta<180^\circ\), the sine equation has two solutions for \(2\theta\). \(2\theta=\sin^{-1}0.735=47.31^\circ\) or \(180^\circ-47.31^\circ=132.69^\circ\). So \(\theta=23.6^\circ\) (a flat kick) or \(66.4^\circ\) (a high kick). The two angles add up to \(90^\circ\), a general property of projectiles.
  11. Answer to Question 11

    Method: use the compound angle formulae \(\sin(A\pm B)=\sin A\cos B\pm\cos A\sin B\), \(\cos(A\pm B)=\cos A\cos B\mp\sin A\sin B\) and \(\tan(A\pm B)=\dfrac{\tan A\pm\tan B}{1\mp\tan A\tan B}\), with exact values of \(30^\circ\), \(45^\circ\) and \(60^\circ\).

    1. Substitute \(\tan A=\tfrac13\) and \(\tan B=\tfrac12\) into the formula for \(\tan(A+B)\). \(\tan(A+B)=\dfrac{\tan A+\tan B}{1-\tan A\tan B}=\dfrac{\frac13+\frac12}{1-\frac16}=\dfrac{5/6}{5/6}=1\). This is the required result.
    2. Both angles are acute, so \(A+B\) lies between \(0^\circ\) and \(180^\circ\); its tangent is positive, so it is acute. \(\tan(A+B)=1\) with \(A+B\) acute (here \(18.43^\circ+26.57^\circ\)), so \(A+B=45^\circ\). So the path has turned through \(45^\circ\) in total.
    3. Since \(A+B=45^\circ\), use the exact value of \(\sin45^\circ\). \(\sin45^\circ=\dfrac{\sqrt2}2\). So \(\sin(A+B)=\dfrac{\sqrt2}2\).
    4. Use the formula for \(\tan(B-A)\) and multiply the top and bottom by 6. \(\tan(B-A)=\dfrac{\frac12-\frac13}{1+\frac16}=\dfrac{1/6}{7/6}=\dfrac17\). So \(\tan(B-A)=\tfrac17\).
  12. Answer to Question 12

    Method: \(\sec\theta=\dfrac1{\cos\theta}\), \(\operatorname{cosec}\theta=\dfrac1{\sin\theta}\) and \(\cot\theta=\dfrac1{\tan\theta}\). Find the sine, cosine or tangent first (with its sign from the quadrant), then take the reciprocal.

    1. Use \(\operatorname{cosec}30^\circ=2\) and \(\cot30^\circ=\sqrt3\). Beam length \(=12\operatorname{cosec}30^\circ=12\times2=24\) m. Distance \(=12\cot30^\circ=12\sqrt3=20.8\) m. So the beam is 24 m long and lights a spot about 20.8 m away.
    2. Rearrange to find \(\cot\theta\), then take the reciprocal to get \(\tan\theta\). \(12\cot\theta=20\) gives \(\tan\theta=\dfrac{12}{20}=0.6\), so \(\theta=31.0^\circ\). So the beam must make about \(31.0^\circ\) with the horizontal.
    3. Dividing \(\sin^2\theta+\cos^2\theta=1\) by \(\sin^2\theta\): \(1+\cot^2\theta=\operatorname{cosec}^2\theta\). With \(\cot\theta=\dfrac{20}{12}=\dfrac53\): \(\operatorname{cosec}^2\theta=1+\dfrac{25}9=\dfrac{34}9\), so \(\operatorname{cosec}\theta=\dfrac{\sqrt{34}}3\) and the beam length is \(12\times\dfrac{\sqrt{34}}3=4\sqrt{34}=23.3\) m. So the beam length is \(4\sqrt{34}\approx23.3\) m. Check: \(\sqrt{12^2+20^2}=\sqrt{544}=23.3\) by Pythagoras.
  13. Answer to Question 13

    Method: the small-angle approximations only work in radians: \(\sin\theta\approx\theta\), \(\tan\theta\approx\theta\), \(\cos\theta\approx1-\dfrac{\theta^2}{2}\). Replace each function, simplify, and the powers of \(\theta\) usually cancel.

    1. Replace \(\sin\theta\) and \(\cos\theta\) by their approximations. \(\sin\theta\approx\theta\) gives \(L\sin\theta\approx L\theta\). \(1-\cos\theta\approx\dfrac{\theta^2}2\) gives \(L(1-\cos\theta)\approx\dfrac{L\theta^2}2\). These are the required approximations.
    2. Substitute \(L=2.5\) and \(\theta=0.2\). Displacement \(\approx2.5\times0.2=0.5\) m. Rise \(\approx\dfrac{2.5\times0.04}2=0.05\) m. So the seat moves about 0.5 m sideways and rises about 5 cm.
    3. Use the calculator in radian mode for the exact values. Exact displacement \(=2.5\sin0.2=0.4967\) m (error \(\dfrac{0.5-0.4967}{0.4967}=0.67\%\)). Exact rise \(=2.5(1-\cos0.2)=0.04983\) m (error \(\dfrac{0.05-0.04983}{0.04983}=0.33\%\)). Both errors are below 1%, so the approximations are good for \(\theta=0.2\).
  14. Answer to Question 14

    1. Rearrange the double angle formula \(\cos2\theta=2\cos^2\theta-1\) to make \(\cos^2\theta\) the subject. \(\cos2\theta=2\cos^2\theta-1\), so \(\cos^2\theta=\dfrac{1+\cos2\theta}2\). Hence \(I=\dfrac{I_0}2(1+\cos2\theta)\). This is the required result.
    2. Divide by \(I_0\) and take the positive square root since \(\theta\) is acute. \(\cos^2\theta=0.75\) gives \(\cos\theta=\dfrac{\sqrt3}2\) and \(\theta=30^\circ\). So \(\theta=30^\circ\).
    3. Divide by \(I_0\), take the positive square root and use the inverse cosine. \(\cos^2\theta=0.2\) gives \(\cos\theta=0.4472\), so \(\theta=63.4^\circ\). So \(\theta\approx63.4^\circ\).
    4. \(\cos^2\theta\le1\), so \(I\le I_0\); the maximum occurs at \(\theta=0^\circ\).
  15. Answer to Question 15

    1. LHS \(=\dfrac1{\sin2x}+\dfrac{\cos2x}{\sin2x}=\dfrac{1+\cos2x}{\sin2x}=\dfrac{2\cos^2x}{2\sin x\cos x}=\dfrac{\cos x}{\sin x}=\cot x\). \(\blacksquare\)
    2. \(\sin3x=\sin(2x+x)=\sin2x\cos x+\cos2x\sin x=2\sin x\cos^2x+(1-2\sin^2x)\sin x\). Replace \(\cos^2x=1-\sin^2x\): \(2\sin x-2\sin^3x+\sin x-2\sin^3x=3\sin x-4\sin^3x\). \(\blacksquare\)
    3. \(3\sin x-4\sin^3x=\sin x\) gives \(2\sin x-4\sin^3x=0\), \(2\sin x(1-2\sin^2x)=0\). \(\sin x=0\): \(x=0^\circ,180^\circ\). \(\sin^2x=\tfrac12\) and \(\sin x>0\) in the range: \(\sin x=\dfrac1{\sqrt2}\), \(x=45^\circ,135^\circ\). Solutions: 0Β°, 45Β°, 135Β°, 180Β°.
    4. With \(x=15^\circ\): \(\cot15^\circ=\operatorname{cosec}30^\circ+\cot30^\circ=2+\sqrt3\). \(\blacksquare\)
  16. Answer to Question 16

    1. \(t=6\): \(14+3\sin90^\circ+4\cos90^\circ=14+3+0=17\). \(t=12\): \(14+3\sin180^\circ+4\cos180^\circ=14+0-4=10\). \(t=3\): \(14+3\sin45^\circ+4\cos45^\circ=14+\dfrac{7\sqrt2}2=18.95\approx19.0\).
    2. \(R=5\), \(\tan\alpha=\dfrac43\), \(\alpha=53.13^\circ\). \(T=14+5\sin(15t+53.13)^\circ\). Maximum \(19\) Β°C, minimum \(9\) Β°C.
    3. Maximum when \(15t+53.13=90\), so \(t=2.46\) hours after 11:00, that is 13:28.
    4. \(14+5\sin(15t+53.13)^\circ\ge17\) gives \(\sin(15t+53.13)^\circ\ge0.6\). The argument lies in \([36.87^\circ,143.13^\circ]\) giving \(0\le t\le6\), and in \([396.87^\circ,503.13^\circ]\), giving \(22.92\le t\le24\) (within range). Total \(=6+(24-22.92)=7.08\) hours.
  17. Answer to Question 17

    1. \(\sec^2x=1+\tan^2x\), so \(2+2\tan^2x+3\tan x-5=0\), i.e. \(2\tan^2x+3\tan x-3=0\).
    2. \(\tan x=\dfrac{-3\pm\sqrt{9+24}}4=\dfrac{-3\pm\sqrt{33}}4\), so \(\tan x=0.6861\) or \(-2.1861\). \(\tan x=0.6861\): \(x=34.5^\circ\) and \(214.5^\circ\). \(\tan x=-2.1861\): \(x=180^\circ-65.4^\circ=114.6^\circ\) and \(294.6^\circ\). Solutions: 34.5Β°, 114.6Β°, 214.5Β°, 294.6Β°.
    3. \(\sec x=\dfrac1{\cos x}\) and \(|\cos x|\le1\), so \(|\sec x|\ge1\). In the table the values are all at least 1.
    4. The tangent has period \(180^\circ\), so every value \(k\) is reached twice in \(360^\circ\). That gives two solutions for each root, four in total.
  18. Answer to Question 18

    1. \(\cos A=\sqrt{1-\frac{64}{289}}=\dfrac{15}{17}\), \(\sin B=\sqrt{1-\frac9{25}}=\dfrac45\) (both positive as the angles are acute).
    2. \(\sin(A+B)=\sin A\cos B+\cos A\sin B=\dfrac8{17}\cdot\dfrac35+\dfrac{15}{17}\cdot\dfrac45=\dfrac{24+60}{85}=\dfrac{84}{85}\).
    3. \(\cos(A+B)=\cos A\cos B-\sin A\sin B=\dfrac{45}{85}-\dfrac{32}{85}=\dfrac{13}{85}\). Check: \(\dfrac{84^2+13^2}{85^2}=\dfrac{7056+169}{7225}=1\).
    4. \(\tan A=\dfrac8{15}\) and \(\tan B=\dfrac43\). \(\tan(A-B)=\dfrac{\frac8{15}-\frac43}{1+\frac8{15}\cdot\frac43}=\dfrac{-\frac{12}{15}}{\frac{77}{45}}=-\dfrac45\cdot\dfrac{45}{77}=-\dfrac{36}{77}\).
    5. \(A=28.07^\circ\) and \(B=53.13^\circ\), so \(A+B=81.2^\circ\). This is acute, consistent with \(\cos(A+B)=\frac{13}{85}>0\).
  19. Answer to Question 19

    1. \(R=5\), \(\alpha=53.13^\circ\), so \(3\sin x+4\cos x=5\sin(x+53.13^\circ)\).
    2. The denominator \(7+5\sin(x+53.13^\circ)\) varies from \(2\) to \(12\). So \(B\) is greatest when the denominator is smallest: \(B_{max}=\dfrac12\), and \(B_{min}=\dfrac1{12}\).
    3. The denominator is least when \(\sin(x+53.13^\circ)=-1\), so \(x+53.13=270\), giving \(x=216.87^\circ\).
    4. \(7+5\sin(x+53.13^\circ)=4\) gives \(\sin(x+53.13^\circ)=-0.6\). So \(x+53.13=216.87^\circ\) or \(323.13^\circ\), giving \(x=163.74^\circ\) or \(x=270^\circ\). Check \(x=270\): \(7-3+0=4\). Solutions: 163.7Β°, 270Β°.
  20. Answer to Question 20

    1. \(3\times36^\circ+2\times36^\circ=180^\circ\), so \(3\theta=180^\circ-2\theta\) and \(\cos3\theta=\cos(180^\circ-2\theta)=-\cos2\theta\).
    2. \(4c^3-3c=-(2c^2-1)\), so \(4c^3+2c^2-3c-1=0\).
    3. At \(c=-1\): \(-4+2+3-1=0\), so \((c+1)\) is a factor. Dividing: \(4c^3+2c^2-3c-1=(c+1)(4c^2-2c-1)\). Since \(\cos36^\circ>0\), \(c\ne-1\) so \(4c^2-2c-1=0\) and \(c=\dfrac{2\pm\sqrt{4+16}}8=\dfrac{1\pm\sqrt5}4\). The positive root gives \(\cos36^\circ=\dfrac{1+\sqrt5}4\).
    4. \(c^2=\dfrac{(1+\sqrt5)^2}{16}=\dfrac{6+2\sqrt5}{16}\), so \(\cos72^\circ=2c^2-1=\dfrac{6+2\sqrt5}8-1=\dfrac{2\sqrt5-2}8=\dfrac{\sqrt5-1}4\). Then \(\cos36^\circ-\cos72^\circ=\dfrac{1+\sqrt5-\sqrt5+1}4=\dfrac12\). \(\blacksquare\)

How to use these Year 13 further trigonometry worksheet answers

First, try every question on the worksheet without looking. Then compare your working with the solution line by line, not only the final answer. When your answer is different, find the first step that changes, because that is where the mistake is. After that, read the matching part of the further trigonometry lesson again. Finally, check that the method is secure with the quiz or the test.

Also, the Year 13 further trigonometry worksheet answers are available as a PDF, so you can mark printed work quickly. Moreover, all the pages of this chapter work together, so you can move between them at any time. For example, many pupils read the lesson on Monday, practise on Wednesday and test themselves on Friday. In short, these Year 13 further trigonometry worksheet answers show every step, so nothing is left unexplained.