Physics Electronics PMDC Conceptual Practice
PMDC Verified Question 59 of 494
In a practical reverse-biased silicon \( \text{P-N} \) junction diode, the reverse leakage current before breakdown is typically on the order of:
A
Amperes (\( \text{A} \))
B
Milliamperes (\( \text{mA} \))
C
Microamperes (\( \mu\text{A} \)) to nanoamperes (\( \text{nA} \))
D
Kiloamperes (\( \text{kA} \))
Tap any option to test your recall and reveal the step-by-step Propolis autopsy.

Propolis Cognitive Error Autopsy

Official Correct Choice:
Option C: Microamperes (\( \mu\text{A} \)) to nanoamperes (\( \text{nA} \))
Concept:

The reverse saturation current is caused by thermally generated minority carriers swept across the junction by the internal field.

Formula:

$$I_0 \propto T^3 e^{-E_g / k_B T} \quad (\text{order of } \mu\text{A for Ge, nA for Si})$$

Solution:

  • Because minority carrier density at room temperature is extremely low, the reverse leakage current is minute, typically \( \mu\text{A} \) for Germanium and \( \text{nA} \) to \( \mu\text{A} \) for Silicon.


Why other options are incorrect:

  • Option A: Amperes represent massive macroscopic power currents.


  • Option B: Milliamperes represent normal forward-bias conduction currents in standard diodes.


  • Option D: Kiloamperes represent industrial-scale short-circuit fault currents.

Quality & Fidelity Assurance: Every question on BeambePrep is rigorously curated against the official PMDC syllabus with zero filler, zero out-of-syllabus content, and zero typos. When an authentic past paper originally contained a historical mistake or ambiguity from the examining board (such as UHS or NUMS), BeambePrep faithfully reflects the original paper while detailing the nuance and scientific consensus in the autopsy above.

Want to solve full-length papers under timed exam conditions?

Practice with zero-scroll lockdown sprints, dynamic latency zone timers, live peer selection telemetry, and the automated Amber mistake recovery loop.