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Class 12 Physics Chapter 14: Semiconductor Electronics: Materials, Devices and Simple Circuits case study question with answers

One case-based question of the kind the board asks: a passage and a table, then 3 parts worth 4 marks in all, with the answer and the marking scheme for each. Written from the NCERT chapter.

Case study · 4 marks
Ananya is given an unmarked diode in a physics laboratory in Pune. She connects it in forward bias through a potentiometer, with a voltmeter across it and a milliammeter in series, and raises the voltage in steps. Her readings are in the table. She then reverses the diode, replaces the milliammeter with a microammeter, and finds 1.5 μA at 2 V and 1.6 μA at 8 V.
V (V)0.050.100.150.200.250.300.35
I (mA)0.00.10.31.04.010.018.0
Part 1 · 1 mark
The diode is most likely made of
Show answer

Answer: (a) germanium

The current becomes appreciable near 0.2 V, the threshold voltage of germanium; a silicon diode would carry almost no current below about 0.7 V.

Part 2 · 1 mark
The dynamic resistance between 0.20 V and 0.25 V is how many times the dynamic resistance between 0.30 V and 0.35 V?
Show answer

Answer: (a) 2.7

rd = ΔV/ΔI. Between 0.20 and 0.25 V: 0.05/3.0 mA ≈ 16.7 Ω. Between 0.30 and 0.35 V: 0.05/8.0 mA ≈ 6.25 Ω. Ratio ≈ 2.7. (b) inverts it; (c) assumes equal steps of V give equal resistance.

Part 3 · 2 marks
Explain why the reverse current hardly changes when the reverse voltage is raised from 2 V to 8 V.
Answer and marking scheme

The reverse current is a drift of minority carriers near the junction swept across by the field. Even a small reverse voltage sweeps all of them, so the current is limited by the minority-carrier concentration, not by the voltage: it saturates at a few μA.

  • reverse current is a drift of minority carriers (1)
  • limited by their concentration, so nearly independent of voltage (saturation) (1)
Or
Using the barrier potential, explain why the forward current stays almost zero up to about 0.2 V and then rises steeply.
Answer and marking scheme

Forward bias lowers the barrier to V₀ − V. At small V only the few carriers in the uppermost energy levels can cross, so the current is negligible. Beyond the threshold the barrier is low enough that, for each small increase in V, many more carriers have the energy to cross, so the current rises steeply (exponentially).

  • small V: barrier V₀ − V still high, only a few carriers cross (1)
  • beyond threshold many more carriers cross, so current rises exponentially (1)
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