A bar magnet of mass 250 g is suspended from the free end of a spring, as illustrated in Fig. 3.1. [Figure 3.1] The magnet hangs so that one pole is near the centre of a coil of wire. The coil is connected in series with a resistor and a switch. The switch is open. The magnet is displaced vertically and then allowed to oscillate with one pole remaining inside the coil. The other pole remains outside the coil. At time t = 0, the magnet is oscillating freely as it passes through its equilibrium position. At time t = 6.0s, the switch in the circuit is closed. The variation with time t of the vertical displacement y of the magnet is shown in Fig. 3.2. [Figure 3.2]
- (a)(i)the frequency f, f = ........................................................................ Hz [2][2]
- (a)(ii)the energy of the oscillations during the time t = 0 to time t = 6.0s. energy = ....................................................................... J [3][3]
- (b)(i)State Faraday's law of electromagnetic induction.[2]
- (b)(ii)Use Faraday's law and energy conservation to explain why the amplitude of the oscillations of the magnet reduces after time t = 6.0s.[3]
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Mark scheme
Marking points from the official mark scheme (May/June 2017). The mark or mark type is shown in brackets.
- [C1] e.g. period = 6/2.5
- [A1] frequency = 0.42 Hz
- [C1] energy = ½ m × 4π²f²yo²
- [C1] = ½ × 0.25 × 4π² × 0.42² × (1.5 × 10⁻²)²
- [A1] = 2.0 × 10⁻⁴ J
- [M1] (induced) e.m.f. proportional to rate of
- [A1] change of magnetic flux (linkage) or cutting of magnetic flux
- [B1] coil cuts flux/field (of moving magnet) inducing e.m.f. in coil
- [M1] (induced) current in resistor causes heating (effect)
- [A1] thermal energy/heat derived from energy of oscillations (of magnet)
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