A slice of a conducting material has its face QRLK normal to a uniform magnetic field of flux density B, as illustrated in Fig. 8.1. [Figure 8.1]. Electrons enter the slice travelling perpendicular to face PQKJ.
- (a)(i)For the free electrons moving in the slice: state the direction of the force on an electron due to movement of the electron in the magnetic field[1]
- (a)(ii)identify the faces, using the letters on Fig. 8.1, between which a potential difference is developed.[1]
- (b)Explain why the potential difference in (a)(ii) reaches a maximum value.[2]
- (c)The number of free electrons per unit volume in the slice of material is 1.3 × 10²⁹m⁻³. The thickness PQ of the slice is 0.10 mm. The magnetic flux density B is 4.6 × 10⁻³T. Calculate the potential difference across the slice for a current of 6.3 × 10⁻⁴A.[2]
- (d)The slice in (c) is a metal. By reference to your answer in (c), suggest why Hall probes are usually made using semiconductors rather than metals.[2]
This question uses a diagram from the original paper, which isn't shown here. Open the full paper from the past papers archive to see it.
Mark scheme
Marking points from the official mark scheme (Oct/Nov 2020). The mark or mark type is shown in brackets.
- [B1] downwards
- [B1] PQRS and JKLM
- [B1] (as charge separates) an electric field is created (between opposite faces)
- [B1] (maximum value is reached when) electric force (on electron) is equal and opposite to magnetic force (on electron)
- [C1] V_H = BI / ntq
- [C1] = (4.6 × 10⁻³ × 6.3 × 10⁻⁴) / (1.3 × 10²⁹ × 0.10 × 10⁻³ × 1.60 × 10⁻¹⁹)
- [A1] = 1.4 x 10⁻¹² V
- [B1] semiconductors have a (much) smaller value for n
- [B1] V_H for semiconductors is (much) larger so more easily measured
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