· H2 Mathematics — Ten-Year Series, worked ← All 11 questions

2015 A-Level · Paper 1 · Question 11

2015 H2 Maths Paper 1, Question 11

Parametric equations 15 marks turning points · area
Download Paper 1 solutions (PDF)

Part (i)

3 marks

Since x=sin⁡3θx = \sin^{3}\theta and y=3sin⁡2θcos⁡θy = 3\sin^{2}\theta\cos\theta,

dxdθ=3sin⁡2θcos⁡θ.\frac{dx}{d\theta} = 3\sin^{2}\theta\cos\theta.
dydθ=3(2sin⁡θcos⁡θ⋅cos⁡θ+sin⁡2θ⋅(−sin⁡θ))\frac{dy}{d\theta} = 3\left( 2\sin\theta\cos\theta \cdot \cos\theta + \sin^{2}\theta \cdot \left( - \sin\theta \right) \right)
=6sin⁡θcos⁡2θ−3sin⁡3θ.= 6\sin\theta\cos^{2}\theta - 3\sin^{3}\theta.

By the chain rule,

dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}
=6sin⁡θcos⁡2θ−3sin⁡3θ3sin⁡2θcos⁡θ= \frac{6\sin\theta\cos^{2}\theta - 3\sin^{3}\theta}{3\sin^{2}\theta\cos\theta}
=2cos⁡θsin⁡θ−sin⁡θcos⁡θ= \frac{2\cos\theta}{\sin\theta} - \frac{\sin\theta}{\cos\theta}
=2cot⁡θ−tan⁡θ.  (shown)= 2\cot\theta - \tan\theta.\ \ \left( \text{shown} \right)

Part (ii)

6 marks

Approach

A turning point occurs where dydx=0\frac{dy}{dx} = 0. We solve 2cot⁡θ=tan⁡θ2\cot\theta = \tan\theta for tan⁡θ\tan\theta directly, since the required form tan⁡θ=k\tan\theta = \sqrt{k} asks for it.

2cot⁡θ=tan⁡θ2\cot\theta = \tan\theta
⇒2cos⁡θsin⁡θ=sin⁡θcos⁡θ\Rightarrow \frac{2\cos\theta}{\sin\theta} = \frac{\sin\theta}{\cos\theta}
⇒2cos⁡2θ=sin⁡2θ.\Rightarrow 2\cos^{2}\theta = \sin^{2}\theta.

Dividing both sides by cos⁡2θ\cos^{2}\theta, which is non-zero since 0≤θ≤12π0 \leq \theta \leq \frac{1}{2}\pi excludes θ=12π\theta = \frac{1}{2}\pi at a turning point (there dxdθ=0\frac{dx}{d\theta} = 0 too, so it is not a genuine turning point of the curve):

2=tan⁡2θ.2 = \tan^{2}\theta.

Since 0≤θ≤12π0 \leq \theta \leq \frac{1}{2}\pi gives tan⁡θ≥0\tan\theta \geq 0, we take the positive root.

∴tan⁡θ=2\therefore\tan\theta = \sqrt{2}, so k=2k = 2.

Approach

With tan⁡θ=2\tan\theta = \sqrt{2}, we read sin⁡θ\sin\theta and cos⁡θ\cos\theta off a right triangle with opposite 2\sqrt{2}, adjacent 11, hypotenuse 3\sqrt{3}, then substitute into xx and yy.

Since tan⁡θ=2\tan\theta = \sqrt{2}, sin⁡θ=23\sin\theta = \frac{\sqrt{2}}{\sqrt{3}} and cos⁡θ=13\cos\theta = \frac{1}{\sqrt{3}}.

x=sin⁡3θ=(23)3x = \sin^{3}\theta = \left( \frac{\sqrt{2}}{\sqrt{3}} \right)^{3}
=2233= \frac{2\sqrt{2}}{3\sqrt{3}}
=269.= \frac{2\sqrt{6}}{9}.
y=3sin⁡2θcos⁡θ=3⋅23⋅13y = 3\sin^{2}\theta\cos\theta = 3 \cdot \frac{2}{3} \cdot \frac{1}{\sqrt{3}}
=23= \frac{2}{\sqrt{3}}
=233.= \frac{2\sqrt{3}}{3}.

∴\therefore the turning point is (269, 233)\left( \frac{2\sqrt{6}}{9},\ \frac{2\sqrt{3}}{3} \right).

Explanation: 2cot⁡θ2\cot\theta and −tan⁡θ- \tan\theta are both strictly decreasing on (0, 12π)\left( 0,\ \frac{1}{2}\pi \right), so dydx=2cot⁡θ−tan⁡θ\frac{dy}{dx} = 2\cot\theta - \tan\theta is strictly decreasing in θ\theta, changing sign from positive to negative exactly once, at tan⁡θ=2\tan\theta = \sqrt{2}. Since dxdθ=3sin⁡2θcos⁡θ≥0\frac{dx}{d\theta} = 3\sin^{2}\theta\cos\theta \geq 0 throughout 0≤θ≤12π0 \leq \theta \leq \frac{1}{2}\pi, xx increases as θ\theta increases, so dydx\frac{dy}{dx} also changes from positive to negative as xx increases through this point.

∴\therefore the turning point is a maximum.

Part (iii)

3 marks

Approach

As θ\theta increases from 00 to 12π\frac{1}{2}\pi, x=sin⁡3θx = \sin^{3}\theta increases monotonically from 00 to 11 (since dxdθ≥0\frac{dx}{d\theta} \geq 0), and y≥0y \geq 0 throughout, so the area under CC can be written as ∫y dx\int y\, dx over this range and converted to an integral in θ\theta.

Area=∫01y dx=∫012πy dxdθ dθ\text{Area} = \int_{0}^{1}y\, dx = \int_{0}^{\frac{1}{2}\pi}y\,\frac{dx}{d\theta}\, d\theta
=∫012π3sin⁡2θcos⁡θ⋅3sin⁡2θcos⁡θ dθ= \int_{0}^{\frac{1}{2}\pi}3\sin^{2}\theta\cos\theta \cdot 3\sin^{2}\theta\cos\theta\, d\theta
=∫012π9sin⁡4θcos⁡2θ dθ.  (shown)= \int_{0}^{\frac{1}{2}\pi}9\sin^{4}\theta\cos^{2}\theta\, d\theta.\ \ \left( \text{shown} \right)

By GC, Area =0.884\text{=}0.884 (3 d.p.).

Note: this integral has the exact closed form 9π32\frac{9\pi}{32}, since 0.884≈9π32=0.8836…0.884 \approx \frac{9\pi}{32} = 0.8836\ldots; the question only asks for the 3 d.p. calculator value.

Part (iv)

3 marks

Approach

Substitute y=axy = ax directly into the parametric equations of CC to find where the line meets the curve, then divide out the root θ=0\theta = 0 (which gives the origin) to isolate tan⁡θ\tan\theta.

At a point of intersection, y=axy = ax gives

3sin⁡2θcos⁡θ=asin⁡3θ.3\sin^{2}\theta\cos\theta = a\sin^{3}\theta.

For θ≠0\theta \neq 0 (which gives the origin), dividing both sides by sin⁡2θ\sin^{2}\theta, which is non-zero:

3cos⁡θ=asin⁡θ3\cos\theta = a\sin\theta
⇒tan⁡θ=3a.  (shown)\Rightarrow \tan\theta = \frac{3}{a}.\ \ \left( \text{shown} \right)

For the line to pass through the maximum point found in (ii), where tan⁡θ=2\tan\theta = \sqrt{2}:

3a=2\frac{3}{a} = \sqrt{2}
⇒a=32\Rightarrow a = \frac{3}{\sqrt{2}}
⇒a=322.\Rightarrow a = \frac{3\sqrt{2}}{2}.

∴a=322\therefore a = \frac{3\sqrt{2}}{2}.

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