Home / IBDP Maths SL 3.3 Applications of trigonometry AA HL Paper 1- Exam Style Questions

IBDP Maths SL 3.3 Applications of trigonometry AA HL Paper 1- Exam Style Questions- New Syllabus

Question

Astrid and Bronwyn are on vacation at Blackpool beach.

Astrid is standing on the beach at point \(R\) and sees Bronwyn standing on the promenade at point \(Q\).

\(PR=400\text{ m},\; PQ=1000\text{ m},\; \angle PRX=\theta\), where \(0<\tan\theta\le \dfrac52\).

Astrid walks in a straight line from \(R\) with speed \(0.8\text{ m s}^{-1}\) until reaching point \(X\) on the promenade. She then jogs along the promenade with speed \(1.2\text{ m s}^{-1}\).

This is shown in the following diagram.

It is given that \( RX=400\sec\theta,\qquad XQ=1000-400\tan\theta. \)

The time, in seconds, for Astrid to reach Bronwyn is given by \(T\).

(a) Show that \( T=500\sec\theta+\frac{2500-1000\tan\theta}{3}. \)

(b) Find \(\dfrac{dT}{d\theta}\).

Astrid chooses the angle \(\theta\) of her walk across the beach to reach Bronwyn in the shortest possible time. You may assume that \(T\) has exactly one minimum value.

(c) Show that in this case \(PX=160\sqrt5\text{ m}\).

Most-appropriate topic code (IB DP Mathematics: Analysis and Approaches):

TOPIC SL 3.3  Applications of right-angled trigonometry (Part a)
TOPIC SL 5.6 Differentiation of trigonometric functions using the chain, product and quotient rules (Part b)
TOPIC SL 5.8  Local minimum points and optimization (Part c)
▶️ Answer/Explanation

(a)

Time taken = Distance ÷ Speed.

Walking across the beach:

\( \frac{RX}{0.8}=\frac{400\sec\theta}{0.8}=500\sec\theta. \)

Jogging along the promenade:

\( \frac{XQ}{1.2} =\frac{1000-400\tan\theta}{1.2} =\frac{2500-1000\tan\theta}{3}. \)

Hence,

\( T =500\sec\theta +\frac{2500-1000\tan\theta}{3}. \)

Answer:

\( \boxed{T=500\sec\theta+\frac{2500-1000\tan\theta}{3}} \)

(b)

Differentiate each term with respect to \(\theta\).

\( \frac{d}{d\theta}(500\sec\theta) =500\sec\theta\tan\theta, \)

\( \frac{d}{d\theta}\left(\frac{2500-1000\tan\theta}{3}\right) =-\frac{1000}{3}\sec^2\theta. \)

Therefore,

\( \boxed{\frac{dT}{d\theta} = 500\sec\theta\tan\theta -\frac{1000}{3}\sec^2\theta.} \)

This derivative measures how the total travel time changes as the walking angle changes.

(c)

At the minimum travel time,

\( \frac{dT}{d\theta}=0. \)

Hence,

\( 500\sec\theta\tan\theta = \frac{1000}{3}\sec^2\theta. \)

Divide both sides by \(\sec\theta\):

\( 500\tan\theta = \frac{1000}{3}\sec\theta. \)

Using \( \tan\theta=\frac{\sin\theta}{\cos\theta}, \qquad \sec\theta=\frac1{\cos\theta}, \)

gives \( 500\sin\theta = \frac{1000}{3}, \)

so \( \sin\theta=\frac23. \)

Then \( \cos\theta=\frac{\sqrt5}{3}, \qquad \tan\theta=\frac2{\sqrt5}. \)

Since

\( PX=400\tan\theta, \)

we obtain

\( PX = 400\left(\frac2{\sqrt5}\right) = \frac{800}{\sqrt5} = 160\sqrt5\text{ m}. \)

Thus,

\( \boxed{PX=160\sqrt5\text{ m}.} \)

The optimization step uses the first derivative to determine the angle that minimizes the total journey time.

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