Home / IBDP Physics- C.1 Simple harmonic motion- IB Style Questions For HL Paper 2

IBDP Physics- C.1 Simple harmonic motion- IB Style Questions For HL Paper 2 -FA 2025

Question

(a) A bar magnet of mass \(0.12\,kg\) is attached to a vertical spring of spring constant \(7.4\,N\,m^{-1}\). The mass of the spring is negligible. When the magnet is at its equilibrium position, determine the elastic potential energy stored in the spring.
The magnet–spring system oscillates vertically in simple harmonic motion, with the spring remaining stretched at all times. The graph shows how the elastic potential energy \(E_p\) of the spring varies with time \(t\) over one complete oscillation.
(b) (i) State and explain the direction of motion of the magnet at \(t = 0.2\,s\).
(ii) Describe the energy transfers that occur between \(t = 0.2\,s\) and \(t = 0.4\,s\).
(c) (i) Show that the amplitude of oscillation of the magnet is approximately \(0.1\,m\).
(ii) Calculate the maximum speed of the magnet.
(iii) Determine the kinetic energy of the magnet at \(t = 0.15\,s\).
(d) A stationary horizontal coil is placed directly below the oscillating magnet.
(i) Discuss two factors that affect the magnitude of the emf induced in the coil. Your answer should explain how an emf is induced and how each factor influences its magnitude.
(ii) A resistor is then connected across the coil, after which the amplitude of oscillation of the magnet rapidly decreases. Explain this behaviour.

Most-appropriate topic codes (IB Physics):

Topic C.1: Simple harmonic motion (Energy, Period) — parts (a), (b), (c)
Topic D.4: Induction (Faraday’s law, Lenz’s law) — part (d)
▶️ Answer/Explanation
Detailed solution

(a)
At equilibrium, the weight of the magnet equals the spring force: \(mg = kx\).
\(x = \frac{mg}{k} = \frac{0.12 \times 9.8}{7.4} \approx 0.159\,m\).
Elastic potential energy: \(E_p = \frac{1}{2}kx^2 = \frac{1}{2} \times 7.4 \times (0.159)^2 \approx 9.3 \times 10^{-2}\,J\).

(b)
(i) At \(t = 0.2\,s\), the graph shows that the elastic potential energy is decreasing. Since \(E_p \propto x^2\) and the spring is always stretched, the extension is decreasing. Therefore, the magnet is moving upwards towards the equilibrium position.
(ii) Between \(t = 0.2\,s\) and \(t = 0.4\,s\), elastic potential energy is converted into kinetic energy and gravitational potential energy as the magnet rises. The kinetic energy decreases to zero at the upper turning point.

(c)
(i) From the graph, \(E_{p,\max} \approx 0.26\,J\) and \(E_{p,\min} \approx 0.01\,J\).
\(x_{\max} = \sqrt{\frac{2 \times 0.26}{7.4}} \approx 0.265\,m\), \(x_{\min} = \sqrt{\frac{2 \times 0.01}{7.4}} \approx 0.052\,m\).
Amplitude: \(A = \frac{x_{\max} – x_{\min}}{2} \approx 0.106\,m \approx 0.1\,m\).
(ii) Angular frequency: \(\omega = \sqrt{\frac{k}{m}} = \sqrt{\frac{7.4}{0.12}} \approx 7.85\,rad\,s^{-1}\).
Maximum speed: \(v_{\max} = \omega A \approx 7.85 \times 0.106 \approx 0.83\,m\,s^{-1}\).
(iii) From the graph at \(t = 0.15\,s\), \(E_p \approx 0.14\,J\), giving an extension \(x \approx 0.195\,m\). Displacement from equilibrium: \(y = 0.195 – 0.159 = 0.036\,m\).
Oscillatory energy: \(E = \frac{1}{2}kA^2 \approx 4.1 \times 10^{-2}\,J\).
Kinetic energy: \(KE = E – \frac{1}{2}ky^2 \approx 3.6 \times 10^{-2}\,J\).

(d)
(i) An emf is induced due to the changing magnetic flux linkage through the coil (Faraday’s law). Two factors are: speed of oscillation (greater speed increases the rate of change of flux) and number of turns in the coil (emf is proportional to the number of turns).
(ii) When the resistor is connected, an induced current flows in the coil. This produces a magnetic field that opposes the motion of the magnet (Lenz’s law), doing work against the motion. Mechanical energy is dissipated as thermal energy in the resistor, causing the oscillations to be damped and the amplitude to decrease.

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