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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
Back to Practice Questions
ElectricalElectronics
PrevNext

The reverse current in a diode is of the order of ____.

A

KA

B

mA

C

μA\mu AμA

D

A

Correct Answer

Concept & PrincipleElectricalElectronics
Option C

μA\mu AμA

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.

💡 Explanation

The reverse current, also known as reverse saturation current (I0I_0I0​ or ISI_SIS​), in a standard silicon PN junction diode is very small and typically ranges in the micro-ampere (µAµAµA) or nano-ampere (nAnAnA) range at room temperature. This current is primarily due to the flow of minority charge carriers across the junction under reverse bias conditions.

🔢 Key Formulas

ID=IS(eVDnVT−1)I_D = I_S (e^{\frac{V_D}{n V_T}} - 1)ID​=IS​(enVT​VD​​−1) — The Shockley diode equation, where ISI_SIS​ is the reverse saturation current

IR≈ISI_R \approx I_SIR​≈IS​ — The approximation for reverse current under reverse bias (VD<0V_D < 0VD​<0)

⚙️ Working Principle

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.

📌 Key Points
  • ▸

    Reverse current is primarily dependent on temperature rather than the applied reverse voltage.

  • ▸

    For silicon diodes, ISI_SIS​ is generally smaller than in germanium diodes due to the larger energy band gap.

  • ▸

    Reverse saturation current approximately doubles for every 10°C10°C10°C rise in temperature.

✅ Advantages
  • ▸

    Minimizes power dissipation in the OFF state

  • ▸

    Allows for high-efficiency rectification

❌ Disadvantages / Limitations
  • ▸

    Temperature sensitivity can lead to thermal runaway

  • ▸

    Limits the high-temperature operating range of circuits

🛠️ Applications / Uses
  • ▸

    Signal detection and rectification

  • ▸

    Voltage clamping and clipping circuits

📄 Additional Information
  • ▸

    Germanium diodes typically have higher ISI_SIS​ (in the range of μA\mu AμA) compared to silicon diodes (nAnAnA range).

  • ▸

    Option A (KA) represents massive current, Option B (mA) is typical for forward current, and Option D (A) is for high-power devices.

📊 Diagram / Illustration
Reverse Saturation Current
IR≈ISI_R \approx I_SIR​≈IS​
Typically in μA\mu AμA or nAnAnA
✅

C is correct — The reverse current in a diode is typically of the order of μA\mu AμA (micro-amperes) due to the low concentration of thermally generated minority charge carriers.

Core Concepts Used
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PN Junction Diode Reverse Bias Minority Charge Carriers Reverse Saturation Current
💡 EXAM TIP

Always remember that while forward current depends on the barrier potential and resistance, reverse current is a leakage phenomenon dominated by ambient temperature.

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