David flies a drone with a flight path CC, modelled by the equation y=2xy = 2^x, where x60;0x 60; 0 and y>0y > 0. He stands at the origin, OO, and sees the drone at point P(a,b)P(a,b). Assuming David's line of sight is the tangent to the curve CC at point PP which passes through the origin, find the exact coordinates of PP.

  1. (b)

    In another instance, David stands at the origin OO and flies the drone vertically upwards from a fixed point QQ, 500 m away from OO. The drone, represented by RR, is ascending upwards at a constant speed of 20 m/s. At the same time, David walks along the horizontal line segment OQOQ at a constant speed of 5 m/s. At any time tt seconds, David's position is point SS on the horizontal line segment OQOQ.

    1. (i)

      Given that the angle θ\theta, in radians, is the angle SRQSRQ, show that tan⁡θ=100−t4t\tan\theta = \dfrac{100 - t}{4t}.

    2. (ii)

      By implicit differentiation or otherwise, find dθdt\dfrac{d\theta}{dt} in terms of tt.

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Worked solution

7(b)(i)

1. Express lengths $SQ$ and $QR$ in terms of $t$.

Given that David starts at OO and moves at 5 m/s5\text{ m/s}, the distance he travels in tt seconds is OS=5tOS = 5t.
Since the total distance OQ=500 mOQ = 500\text{ m}, the remaining distance SQSQ is:
SQ=500−5tSQ = 500 - 5t

The drone ascends vertically from QQ at 20 m/s20\text{ m/s}, so its height after tt seconds is:
QR=20tQR = 20t

2. Use trigonometry in $\triangle SQR$ to express $\tan\theta$.

In the right-angled triangle SQRSQR, the angle at QQ is 90∘90^\circ. For angle SRQ=θSRQ = \theta, the opposite side is SQSQ and the adjacent side is QRQR.
tan⁡θ=SQQR\tan \theta = \frac{SQ}{QR}
tan⁡θ=500−5t20t\tan \theta = \frac{500 - 5t}{20t}
Dividing the numerator and the denominator by 5:
tan⁡θ=100−t4t(Shown)\tan \theta = \frac{100 - t}{4t} \quad \text{(Shown)}

Answer

Shown\text{Shown}

7(b)(ii)

1. Differentiate both sides of the equation from (b)(i) with respect to $t$ using implicit differentiation and the quotient rule.

ddt(tan⁡θ)=ddt(100−t4t)\frac{d}{dt}(\tan\theta) = \frac{d}{dt}\left(\frac{100 - t}{4t}\right)
sec⁡2θdθdt=4t(−1)−(100−t)(4)(4t)2\sec^2\theta \frac{d\theta}{dt} = \frac{4t(-1) - (100 - t)(4)}{(4t)^2}
sec⁡2θdθdt=−4t−400+4t16t2=−25t2\sec^2\theta \frac{d\theta}{dt} = \frac{-4t - 400 + 4t}{16t^2} = -\frac{25}{t^2}

2. Express $\sec^2\theta$ in terms of $t$ using the identity $\sec^2\theta = 1 + \tan^2\theta$.

sec⁡2θ=1+(100−t4t)2\sec^2\theta = 1 + \left(\frac{100 - t}{4t}\right)^2
sec⁡2θ=1+10000−200t+t216t2\sec^2\theta = 1 + \frac{10000 - 200t + t^2}{16t^2}
sec⁡2θ=16t2+10000−200t+t216t2\sec^2\theta = \frac{16t^2 + 10000 - 200t + t^2}{16t^2}
sec⁡2θ=17t2−200t+1000016t2\sec^2\theta = \frac{17t^2 - 200t + 10000}{16t^2}

3. Substitute the expression for $\sec^2\theta$ into the differentiated equation and simplify to isolate $\frac{d\theta}{dt}$.

(17t2−200t+1000016t2)dθdt=−25t2\left(\frac{17t^2 - 200t + 10000}{16t^2}\right) \frac{d\theta}{dt} = -\frac{25}{t^2}
dθdt=−25t2×16t217t2−200t+10000\frac{d\theta}{dt} = -\frac{25}{t^2} \times \frac{16t^2}{17t^2 - 200t + 10000}
dθdt=−40017t2−200t+10000\frac{d\theta}{dt} = -\frac{400}{17t^2 - 200t + 10000}

Answer

−40017t2−200t+10000-\frac{400}{17t^2 - 200t + 10000}

AI analysis — may contain mistakes.

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