
The semiconductor diode is the simplest electronic device — a one-way valve for current — yet it powers every phone charger, protects circuits from reverse voltage and lights our homes as LEDs. Diode theory (barrier potential, forward/reverse bias, V-I curve, breakdown, rectifiers) is asked in almost every BCS (EEE), PGCB, BPDB, BREB, DPDC, NTRCA and university electronics exam. This post explains it step by step with an animation, formulas, solved problems and MCQs.
- A diode is a p-n junction with two terminals: anode (p) and cathode (n).
- A depletion region and barrier potential form at the junction: ≈ 0.7 V for Si, ≈ 0.3 V for Ge.
- Forward bias (p positive) narrows the depletion region → large current after the cut-in voltage. Reverse bias widens it → only tiny saturation current.
- Shockley equation: I = IS(eV/ηVT − 1), VT ≈ 26 mV at room temperature.
- Uses: rectifiers, clippers, clampers, voltage regulation (Zener), LEDs, photodiodes, protection.
- Formation of the p-n junction
- Forward and reverse bias (animation)
- V-I characteristic and diode equation
- Reverse breakdown: Zener and avalanche
- Important parameters and models
- Types of diodes
- Rectifiers at a glance
- Advantages of semiconductor diodes
- Solved problems
- Practice MCQs
- বাংলায় দ্রুত রিভিশন
1. Formation of the p-n Junction
When p-type (many holes) and n-type (many electrons) silicon are joined, electrons diffuse into the p-side and holes into the n-side and recombine. This leaves behind immobile ions — negative acceptor ions on the p-side, positive donor ions on the n-side — forming the depletion region (no free carriers). The ions create an electric field and a barrier potential V0 that stops further diffusion: about 0.7 V for silicon and 0.3 V for germanium at room temperature. See PN junction formation.
2. Forward and Reverse Bias (Animation)
- Forward bias: positive terminal to p (anode), negative to n (cathode). The applied voltage opposes the barrier, the depletion region narrows, and once V exceeds the cut-in (knee) voltage current rises steeply.
- Reverse bias: positive to n, negative to p. The depletion region widens and only a very small reverse saturation current IS (nA for Si) flows, carried by minority carriers.
3. V-I Characteristic and Diode Equation
I = IS (eV / ηVT − 1), VT = kT/q ≈ 25.85 mV at 300 K- η (ideality factor) ≈ 1 for Ge and 1–2 for Si.
- Forward region: current increases exponentially after cut-in.
- Reverse region: I ≈ −IS until breakdown.
- Temperature effects: IS roughly doubles every 10 °C; forward voltage drops about 2 mV/°C.
4. Reverse Breakdown: Zener and Avalanche
| Feature | Zener breakdown | Avalanche breakdown |
|---|---|---|
| Doping | Heavy (thin depletion region) | Light/moderate |
| Voltage | Low (≲ 5 V) | Higher (≳ 6–7 V) |
| Mechanism | Strong field pulls electrons from covalent bonds (tunnelling) | Carriers gain energy and ionise atoms by collision — multiplication |
| Temperature coefficient | Negative | Positive |
More detail: PN Junction Breakdown: Zener vs Avalanche.
5. Important Parameters and Models
- Forward current rating IF(max), peak inverse voltage (PIV), power rating, reverse recovery time trr.
- Static resistance RDC = V/I; dynamic (AC) resistance rd = ΔV/ΔI ≈ ηVT/ID ≈ 26 mV / ID.
- Junction (transition) capacitance in reverse bias and diffusion capacitance in forward bias.
- Models: ideal (short when forward, open when reverse); constant-drop (0.7 V); piecewise linear (0.7 V + rd).
6. Types of Diodes
| Diode | Key feature | Application |
|---|---|---|
| Rectifier (1N4007) | High current & PIV, 50/60 Hz | Power supplies |
| Zener | Operates in reverse breakdown at fixed VZ | Voltage regulation, reference |
| LED | Emits light when forward biased (GaAs, GaN…) | Lighting, displays, indicators |
| Photodiode | Reverse current proportional to light | Optical receivers, sensors |
| Schottky | Metal–semiconductor, low drop (0.2–0.4 V), very fast | SMPS, RF detectors |
| Varactor | Capacitance varies with reverse voltage | VCOs, tuning |
| Tunnel | Heavily doped, negative-resistance region | Microwave oscillators (see negative resistance) |
| PIN | Intrinsic layer between p and n | RF switches, attenuators, photodetectors |
7. Rectifiers at a Glance
| Parameter | Half-wave | Full-wave centre-tap | Bridge |
|---|---|---|---|
| Number of diodes | 1 | 2 | 4 |
| VDC (ideal) | Vm/π | 2Vm/π | 2Vm/π |
| Ripple factor | 1.21 | 0.482 | 0.482 |
| Efficiency (max) | 40.6 % | 81.2 % | 81.2 % |
| PIV per diode | Vm | 2Vm | Vm |
| Ripple frequency (50 Hz input) | 50 Hz | 100 Hz | 100 Hz |
8. Advantages of Semiconductor Diodes (over Vacuum Diodes)
- Very small size and weight; no heater, so no warm-up time and lower power consumption.
- High efficiency and low forward voltage drop.
- Long life, mechanical ruggedness and low cost.
- Operate at low voltages and can be integrated in ICs.
- Limitations: sensitive to temperature, limited reverse voltage and current ratings, can be damaged by surges.
9. Solved Problems
Problem 1. Find the dynamic resistance of a silicon diode at 1 mA and 10 mA (η = 1). rd = 26 mV/1 mA = 26 Ω; at 10 mA = 2.6 Ω.
Problem 2. A bridge rectifier is fed from a 12 V (RMS) transformer secondary. Find Vm and the DC output (a) ideal, (b) with 0.7 V per diode.
- Vm = 12√2 ≈ 16.97 V
- (a) VDC = 2Vm/π ≈ 10.8 V
- (b) Two diodes conduct at a time: Vm′ = 16.97 − 1.4 = 15.57 V ⇒ VDC ≈ 9.9 V
Problem 3. IS = 10 nA at 25 °C. Estimate IS at 55 °C. Three 10 °C steps ⇒ 10 × 2³ = 80 nA.
10. Practice MCQs (click to see answer)
1. Barrier potential of a silicon diode at room temperature is about: (a) 0.3 V (b) 0.7 V (c) 1.1 V (d) 0.1 V
2. In forward bias, the depletion region: (a) Widens (b) Narrows (c) Stays the same (d) Disappears permanently
3. Reverse saturation current is due to: (a) Majority carriers (b) Minority carriers (c) Ions (d) Photons only
4. Reverse saturation current approximately doubles for every: (a) 1 °C (b) 5 °C (c) 10 °C (d) 50 °C rise
5. Zener breakdown has a temperature coefficient that is: (a) Positive (b) Negative (c) Zero (d) Infinite
6. The diode with the lowest forward voltage drop is the: (a) Si rectifier (b) Schottky diode (c) LED (d) Zener
7. Efficiency of a full-wave rectifier is: (a) 40.6 % (b) 81.2 % (c) 100 % (d) 50 %
8. PIV of each diode in a centre-tapped full-wave rectifier is: (a) Vm (b) 2Vm (c) Vm/2 (d) √2Vm
9. The thermal voltage VT at room temperature is about: (a) 0.7 V (b) 26 mV (c) 1 V (d) 2.6 V
10. A varactor diode is used as a: (a) Rectifier (b) Voltage-variable capacitor (c) Light source (d) Constant-current source
11. বাংলায় দ্রুত রিভিশন
- ডায়োড: p-n জাংশন; অ্যানোড (p) ও ক্যাথোড (n)। কারেন্ট একদিকে চলতে দেয়।
- জাংশনে ডিপ্লেশন অঞ্চল ও বাধা বিভব তৈরি হয় — সিলিকন ≈ ০.৭ V, জার্মেনিয়াম ≈ ০.৩ V।
- ফরোয়ার্ড বায়াস: ডিপ্লেশন সরু হয়, কাট-ইন ভোল্টেজের পর বড় কারেন্ট। রিভার্স বায়াস: ডিপ্লেশন চওড়া, খুব সামান্য স্যাচুরেশন কারেন্ট (সংখ্যালঘু বাহক)।
- শকলি সমীকরণ: I = IS(eV/ηVT − 1); VT ≈ ২৬ mV; ডায়নামিক রেজিস্ট্যান্স ≈ ২৬ mV/I।
- জেনার ব্রেকডাউন (কম ভোল্টেজ, ঋণাত্মক তাপ সহগ) বনাম অ্যাভালাঞ্চ (বেশি ভোল্টেজ, ধনাত্মক তাপ সহগ)।
- রেক্টিফায়ার: হাফ-ওয়েভ দক্ষতা ৪০.৬%, ফুল-ওয়েভ ৮১.২%; রিপল ফ্যাক্টর ১.২১ ও ০.৪৮২।
Related Posts
- PN Junction Formation: Depletion Region
- PN Junction Breakdown: Zener vs Avalanche
- FET vs BJT: Key Differences
- Bilateral vs Unilateral Elements
References: Boylestad & Nashelsky, Electronic Devices and Circuit Theory; Millman & Halkias, Integrated Electronics; Sedra & Smith, Microelectronic Circuits. Images and animations: original work by Totalecer.