Difficulty: Easy
Correct Answer: Correct
Explanation:
Introduction / Context:Diodes are often taught using a switch analogy: forward bias ≈ closed switch (low impedance), reverse bias ≈ open switch (high impedance). While this is a simplification, it is useful in understanding rectifiers, clamps, and protection circuits. The key caveats are reverse leakage at finite temperatures and eventual breakdown at sufficiently high reverse voltage.
Given Data / Assumptions:
Concept / Approach:In reverse bias, the depletion region widens, and only a tiny leakage current flows (reverse saturation current). Thus the diode presents a very high dynamic resistance, mimicking an open switch. If the reverse voltage exceeds the breakdown threshold (zener/avalanche), current rises sharply and the open-switch model no longer applies. Designers ensure normal operation stays well below breakdown unless using a zener intentionally for regulation.
Step-by-Step Solution:
Apply reverse voltage less than PIV.Observe current: only microamps to nanoamps (device-dependent) flow.Model behavior: high impedance, effectively an open switch for most circuit calculations.Note exception: at breakdown, current increases sharply and power dissipation considerations dominate.Verification / Alternative check:Use a DMM on resistance range: reverse direction reads very high resistance; forward direction reads low (or shows a diode drop in diode-test mode). Datasheets list typical reverse leakage (IR), confirming microamp-level currents at specified VR and temperature.
Why Other Options Are Wrong:Restricting validity to specific diode types, voltages, or extreme temperatures is unnecessary. The open-switch approximation is widely applicable below breakdown for most silicon diodes.
Common Pitfalls:Ignoring leakage in ultra-high-impedance nodes; in precision circuits, even microamps matter. Also, forgetting temperature dependence—leakage increases with heat.
Final Answer:Correct
Discussion & Comments