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The reverse current in a diode is of the order of ____.
KA
mA
μA
A
μA
Quick Summary: The reverse current, also known as reverse saturation current ($I_0$ or $I_S$), in a standard silicon PN junction diode is very small and typically ranges in the micro-ampere ($µA$) or nano-ampere ($nA$) range at room temperature. This current is primarily due to the flow of minority charge carriers across the junction under reverse bias conditions.
The reverse current, also known as reverse saturation current (I0 or IS), in a standard silicon PN junction diode is very small and typically ranges in the micro-ampere (µA) or nano-ampere (nA) range at room temperature. This current is primarily due to the flow of minority charge carriers across the junction under reverse bias conditions.
ID=IS(enVTVD−1) — The Shockley diode equation, where IS is the reverse saturation current
IR≈IS — The approximation for reverse current under reverse bias (VD<0)
When a diode is reverse-biased, the potential barrier at the junction increases, preventing majority carriers from crossing. However, thermal energy generates electron-hole pairs, allowing minority carriers to cross the junction. Since the number of thermally generated minority carriers is small, the resulting reverse saturation current remains extremely low and is essentially independent of the applied reverse voltage until the breakdown voltage is reached.
Reverse current is primarily dependent on temperature rather than the applied reverse voltage.
For silicon diodes, IS is generally smaller than in germanium diodes due to the larger energy band gap.
Reverse saturation current approximately doubles for every 10°C rise in temperature.
Minimizes power dissipation in the OFF state
Allows for high-efficiency rectification
Temperature sensitivity can lead to thermal runaway
Limits the high-temperature operating range of circuits
Signal detection and rectification
Voltage clamping and clipping circuits
Germanium diodes typically have higher IS (in the range of μA) compared to silicon diodes (nA range).
Option A (KA) represents massive current, Option B (mA) is typical for forward current, and Option D (A) is for high-power devices.
C is correct — The reverse current in a diode is typically of the order of μA (micro-amperes) due to the low concentration of thermally generated minority charge carriers.
Always remember that while forward current depends on the barrier potential and resistance, reverse current is a leakage phenomenon dominated by ambient temperature.