In the diagram, point Q is 400 m vertically above point A. Initially, a balloon is at point Q and moves horizontally in a straight line at a constant speed of 10 m per second away from an observer stationed at point A. At time t seconds, after the start, the balloon is at point P where QP is x m and the angle of elevation of the balloon from the observer at A is β\beta radians. Find exactly the rate of change of β\beta at the instant when xx is 100 m. A gardener designs a flower bed ABCABC in the shape of an isosceles triangle inscribed in a circular plot of land with radius 6 meters, as shown in the diagram. The vertices of the triangle lie on the circumference of the circle and AB=ACAB = AC. The angle BACBAC is θ\theta, where θ\theta is acute. Express the area of the flower bed ABCABC in terms of θ\theta. As θ\theta varies, use differentiation to find the exact maximum possible area of the flower bed, and show that it is a maximum.

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Worked solution

9(a)

1. Set up an equation relating the angle of elevation $\beta$ to the horizontal distance $x$.

From the right-angled triangle formed by the observer A, the point vertically below P, and P:
tan⁡β=400x\tan \beta = \frac{400}{x}

2. Differentiate implicitly with respect to time $t$ to relate the rates of change.

Differentiating both sides with respect to tt:
sec⁡2β⋅dβdt=−400x−2⋅dxdt\sec^2 \beta \cdot \frac{d\beta}{dt} = -400x^{-2} \cdot \frac{dx}{dt}
sec⁡2β⋅dβdt=−400x2⋅dxdt\sec^2 \beta \cdot \frac{d\beta}{dt} = -\frac{400}{x^2} \cdot \frac{dx}{dt}

3. Evaluate $\sec^2 \beta$ at the instant when $x = 100$.

When x=100x = 100:
tan⁡β=400100=4\tan \beta = \frac{400}{100} = 4
Using the trigonometric identity sec⁡2β=1+tan⁡2β\sec^2 \beta = 1 + \tan^2 \beta:
sec⁡2β=1+42=17\sec^2 \beta = 1 + 4^2 = 17

4. Substitute the known values to find the exact rate of change of $\beta$.

Given the balloon's horizontal speed, dxdt=10\frac{dx}{dt} = 10.
Substitute x=100x = 100, dxdt=10\frac{dx}{dt} = 10, and sec⁡2β=17\sec^2 \beta = 17 into the differentiated equation:
17dβdt=−4001002(10)17 \frac{d\beta}{dt} = -\frac{400}{100^2} (10)
17dβdt=−40001000017 \frac{d\beta}{dt} = -\frac{4000}{10000}
17dβdt=−2517 \frac{d\beta}{dt} = -\frac{2}{5}
dβdt=−285\frac{d\beta}{dt} = -\frac{2}{85}

Answer

−285-\frac{2}{85} rad/s

9(b)(i)

1. Relate the dimensions of the triangle to the centre of the circle using a perpendicular bisector.

Let OO be the centre of the circle and MM be the midpoint of BCBC.
Since △ABC\triangle ABC is isosceles with AB=ACAB = AC, the line of symmetry AMAM passes through OO and is perpendicular to BCBC.
By the angle at centre theorem, ∠BOC=2∠BAC=2θ\angle BOC = 2\angle BAC = 2\theta.
Since △OBC\triangle OBC is isosceles (OB=OCOB = OC), OMOM bisects ∠BOC\angle BOC, so ∠MOC=θ\angle MOC = \theta.

2. Express the base, height, and area of the flower bed in terms of $\theta$.

In the right-angled △OMC\triangle OMC, the radius OC=6OC = 6.
MC=6sin⁡θ  ⟹  Base BC=2×6sin⁡θ=12sin⁡θMC = 6 \sin \theta \implies \text{Base } BC = 2 \times 6 \sin \theta = 12 \sin \theta
OM=6cos⁡θOM = 6 \cos \theta
Since θ\theta is acute, all angles in △ABC\triangle ABC are acute, meaning OO lies inside the triangle. Thus, the height is:
AM=AO+OM=6+6cos⁡θAM = AO + OM = 6 + 6 \cos \theta

Area=12×BC×AM\text{Area} = \frac{1}{2} \times BC \times AM
Area=12(12sin⁡θ)(6+6cos⁡θ)\text{Area} = \frac{1}{2}(12 \sin \theta)(6 + 6 \cos \theta)
Area=36sin⁡θ(1+cos⁡θ)\text{Area} = 36 \sin \theta(1 + \cos \theta)

Answer

36sin⁡θ(1+cos⁡θ)36 \sin \theta (1 + \cos \theta)

9(b)(ii)

1. Derive the expression for the area of the flower bed $A$ in terms of $\theta$ (from part (b)(i)).

Let OO be the centre of the circle with radius r=6r = 6. By the angle at centre theorem, ∠BOC=2θ\angle BOC = 2\theta.
Since AB=ACAB = AC, the triangle is symmetric and ∠AOB=∠AOC=2π−2θ2=π−θ\angle AOB = \angle AOC = \frac{2\pi - 2\theta}{2} = \pi - \theta.
The area of the flower bed is the sum of the areas of △AOB\triangle AOB, △AOC\triangle AOC, and △BOC\triangle BOC:
A=12(62)sin⁡(π−θ)+12(62)sin⁡(π−θ)+12(62)sin⁡(2θ)A = \frac{1}{2}(6^2)\sin(\pi - \theta) + \frac{1}{2}(6^2)\sin(\pi - \theta) + \frac{1}{2}(6^2)\sin(2\theta)
A=18sin⁡θ+18sin⁡θ+18sin⁡2θA = 18\sin\theta + 18\sin\theta + 18\sin 2\theta
A=36sin⁡θ+18sin⁡2θA = 36\sin\theta + 18\sin 2\theta

2. Differentiate the area with respect to $\theta$ and set it to zero to find stationary points.

dAdθ=36cos⁡θ+36cos⁡2θ\frac{\mathrm{d}A}{\mathrm{d}\theta} = 36\cos\theta + 36\cos 2\theta
For a maximum area, we require dAdθ=0\frac{\mathrm{d}A}{\mathrm{d}\theta} = 0:
36cos⁡θ+36cos⁡2θ=036\cos\theta + 36\cos 2\theta = 0
cos⁡2θ+cos⁡θ=0\cos 2\theta + \cos\theta = 0

3. Solve the trigonometric equation for $\theta$.

Using the double angle identity cos⁡2θ=2cos⁡2θ−1\cos 2\theta = 2\cos^2\theta - 1:
2cos⁡2θ−1+cos⁡θ=02\cos^2\theta - 1 + \cos\theta = 0
2cos⁡2θ+cos⁡θ−1=02\cos^2\theta + \cos\theta - 1 = 0
(2cos⁡θ−1)(cos⁡θ+1)=0(2\cos\theta - 1)(\cos\theta + 1) = 0
Since θ\theta is an acute angle, 0<θ<π20 < \theta < \frac{\pi}{2}, which implies cos⁡θ>0\cos\theta > 0.
Therefore, cos⁡θ=12  ⟹  θ=π3\cos\theta = \frac{1}{2} \implies \theta = \frac{\pi}{3}.

4. Calculate the exact maximum area.

Substitute θ=π3\theta = \frac{\pi}{3} into the area expression:
A=36sin⁡(π3)+18sin⁡(2π3)A = 36\sin\left(\frac{\pi}{3}\right) + 18\sin\left(\frac{2\pi}{3}\right)
A=36(32)+18(32)A = 36\left(\frac{\sqrt{3}}{2}\right) + 18\left(\frac{\sqrt{3}}{2}\right)
A=183+93=273 m2A = 18\sqrt{3} + 9\sqrt{3} = 27\sqrt{3} \text{ m}^2

5. Perform the second derivative test to verify that the area is a maximum.

d2Adθ2=−36sin⁡θ−72sin⁡2θ\frac{\mathrm{d}^2A}{\mathrm{d}\theta^2} = -36\sin\theta - 72\sin 2\theta
When θ=π3\theta = \frac{\pi}{3}:
d2Adθ2=−36sin⁡(π3)−72sin⁡(2π3)\frac{\mathrm{d}^2A}{\mathrm{d}\theta^2} = -36\sin\left(\frac{\pi}{3}\right) - 72\sin\left(\frac{2\pi}{3}\right)
d2Adθ2=−36(32)−72(32)=−543\frac{\mathrm{d}^2A}{\mathrm{d}\theta^2} = -36\left(\frac{\sqrt{3}}{2}\right) - 72\left(\frac{\sqrt{3}}{2}\right) = -54\sqrt{3}
Since d2Adθ2<0\frac{\mathrm{d}^2A}{\mathrm{d}\theta^2} < 0, the exact area 27327\sqrt{3} is indeed a maximum.

Answer

273 m227\sqrt{3} \text{ m}^2

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