In the diagram, point QQ is 400 m400\text{ m} vertically above point AA. Initially, a balloon is at point QQ and moves horizontally in a straight line at a constant speed of 10 m10\text{ m} per second away from an observer stationed at point AA. At time tt seconds, after the start, the balloon is at point PP where QPQP is x mx\text{ m} and the angle of elevation of the balloon from the observer at AA is β\beta radians. Find exactly the rate of change of β\beta at the instant when xx is 100 m100\text{ m}. A gardener designs a flower bed ABCABC in the shape of an isosceles triangle inscribed in a circular plot of land with radius 66 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. Relate the angle of elevation $\beta$ to the horizontal distance $x$.

From the given diagram, the balloon forms a right-angled triangle with the ground. The constant vertical height is 400 m400\text{ m} and the horizontal distance is x mx\text{ m}.
tan⁡β=400x\tan \beta = \frac{400}{x}

2. Differentiate the equation with respect to time $t$.

Differentiating both sides implicitly with respect to tt:
sec⁡2βdβdt=−400x2dxdt\sec^2 \beta \frac{d\beta}{dt} = -\frac{400}{x^2} \frac{dx}{dt}

3. Determine the exact value of $\sec^2 \beta$ at the specified instant.

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+(4)2=17\sec^2 \beta = 1 + (4)^2 = 17
(Note: A common student mistake is to find β=tan⁡−1(4)\beta = \tan^{-1}(4) using a calculator, which introduces rounding errors and violates the 'find exactly' instruction.)

4. Substitute the known rates and values to solve for $\frac{d\beta}{dt}$.

The balloon moves horizontally away at a constant speed, so dxdt=10 m/s\frac{dx}{dt} = 10\text{ m/s}.
Substitute x=100x = 100, dxdt=10\frac{dx}{dt} = 10, and sec⁡2β=17\sec^2 \beta = 17 into the differentiated equation:
17dβdt=−400(100)2(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 rad/s-\frac{2}{85} \text{ rad/s}

9(b)

1. Formulate the expression for the area of the flower bed $ABC$ in terms of $\theta$.

Let MM be the midpoint of BCBC. By symmetry, the altitude from AA to BCBC passes through MM and the centre of the circle OO.
The angle subtended by arc BCBC at the centre is ∠BOC=2∠BAC=2θ\angle BOC = 2\angle BAC = 2\theta.
In the right-angled △BOM\triangle BOM, ∠BOM=θ\angle BOM = \theta.
BM=OBsin⁡θ=6sin⁡θ  ⟹  BC=2BM=12sin⁡θBM = OB \sin\theta = 6\sin\theta \implies BC = 2BM = 12\sin\theta
OM=OBcos⁡θ=6cos⁡θOM = OB \cos\theta = 6\cos\theta
The height of △ABC\triangle ABC is AM=AO+OM=6+6cos⁡θAM = AO + OM = 6 + 6\cos\theta.
The area of the flower bed, AA, is:
A=12⋅BC⋅AMA = \frac{1}{2} \cdot BC \cdot AM
A=12(12sin⁡θ)(6+6cos⁡θ)A = \frac{1}{2}(12\sin\theta)(6 + 6\cos\theta)
A=36sin⁡θ(1+cos⁡θ)=36sin⁡θ+36sin⁡θcos⁡θA = 36\sin\theta(1 + \cos\theta) = 36\sin\theta + 36\sin\theta\cos\theta
Using the double angle identity sin⁡(2θ)=2sin⁡θcos⁡θ\sin(2\theta) = 2\sin\theta\cos\theta:
A=36sin⁡θ+18sin⁡(2θ)A = 36\sin\theta + 18\sin(2\theta)

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

dAdθ=36cos⁡θ+18(2)cos⁡(2θ)=36cos⁡θ+36cos⁡(2θ)\frac{\mathrm{d}A}{\mathrm{d}\theta} = 36\cos\theta + 18(2)\cos(2\theta) = 36\cos\theta + 36\cos(2\theta)
To find the maximum area, set 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 resulting trigonometric equation for acute $\theta$.

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, cos⁡θ>0\cos\theta > 0.
Thus, cos⁡θ=12\cos\theta = \frac{1}{2}, which gives θ=π3\theta = \frac{\pi}{3}.

4. Calculate the exact maximum possible 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=273A = 18\sqrt{3} + 9\sqrt{3} = 27\sqrt{3}
The exact maximum area is 273 m227\sqrt{3}\text{ m}^2.

5. Use the second derivative test to justify that this 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 area is a maximum.

Answer

Area =36sin⁡θ+18sin⁡(2θ)= 36\sin\theta + 18\sin(2\theta), exact maximum area =273 m2= 27\sqrt{3}\text{ m}^2

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