Home / IBDP Maths SL 5.9 Kinematic problems involving displacement, velocity and acceleration AA HL Paper 2- Exam Style Questions

IBDP Maths SL 5.9 Kinematic problems involving displacement, velocity and acceleration AA HL Paper 2- Exam Style Questions- New Syllabus

Question

A particle P moves along a straight line such that its velocity, \( v \, \text{m s}^{-1} \), at time \( t \) seconds is modeled by the function \( v(t) = e^{-\sin t} \cos(2t) \), for \( 0 \leq t \leq 5 \).
(a) Determine the maximum speed attained by P during this interval.
(b) Calculate the total distance covered by P between \( t = 0 \) and \( t = 5 \).
(c) Find the acceleration of P at the instant it changes its direction of motion for the second time.

Syllabus Topic Codes (IB Mathematics AA HL):

SL 5.9: Kinematic problems involving displacement \( s \), velocity \( v \), acceleration \( a \) and total distance travelled; speed is the magnitude of velocity — parts (a), (b), (c)
AHL 5.10: Derivatives of \( \cos x \), \( e^x \); chain rule for composite functions — part (c)
SL 5.11: Total distance travelled is given by \( \int_{t_1}^{t_2} |v(t)| \, dt \) — part (b)
▶️ Answer/Explanation

(a) Maximum Speed
Speed is the magnitude of velocity, \( |v(t)| \). Using a graphing calculator to find the maximum of \( |e^{-\sin t} \cos(2t)| \) on the interval \( [0, 5] \):
The maximum value occurs at \( t \approx 3.32 \) seconds.
Max Speed \( \approx 2.296 \dots \)
Answer: \( \boxed{2.30 \, \text{m s}^{-1}} \) (to 3 s.f.)


(b) Total Distance Travelled
Total distance is given by the integral of speed:
Distance \( = \int_{0}^{5} |e^{-\sin t} \cos(2t)| \, dt \).
Using numerical integration on a calculator:
Distance \( \approx 3.9555 \dots \)
Answer: \( \boxed{3.96 \, \text{metres}} \) (to 3 s.f.)


(c) Acceleration at Second Change of Direction
A change in direction occurs when velocity \( v(t) = 0 \).
\( e^{-\sin t} \cos(2t) = 0 \implies \cos(2t) = 0 \).
1. First change: \( 2t = \frac{\pi}{2} \implies t_1 = \frac{\pi}{4} \approx 0.785 \).
2. Second change: \( 2t = \frac{3\pi}{2} \implies t_2 = \frac{3\pi}{4} \approx 2.35619 \dots \).
Acceleration is the derivative of velocity, \( a(t) = v'(t) \).
Using the product and chain rules:
\( v'(t) = (e^{-\sin t} \cdot -\cos t) \cos(2t) + e^{-\sin t} (-2 \sin(2t)) \).
At \( t = \frac{3\pi}{4} \), \( \cos(2t) = 0 \) and \( \sin(2t) = -1 \):
\( a(\frac{3\pi}{4}) = 0 + e^{-\sin(3\pi/4)} (-2(-1)) = 2e^{-1/\sqrt{2}} \approx 0.98613 \dots \)
Answer: \( \boxed{0.986 \, \text{m s}^{-2}} \) (to 3 s.f.)

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