---
title: "Barkhausen criteria and oscillation principle"
subject: "Electronics Devices and Circuit"
chapter: 5
key: "semester_3/electronics_devices_and_circuit:barkhausen-criteria-principle"
source: https://www.bctengineer.com/q/semester_3/electronics_devices_and_circuit/barkhausen-criteria-principle
site: BCT Engineering
---

# Barkhausen criteria and oscillation principle

Electronics Devices and Circuit · Chapter 5: Signal Generator and Waveform-Shaping Circuits

- Asked in: 2068 Baisakh, 4 marks; 2070 Chaitra, 2 marks (asked 2 times)
- Video: [Oscillators & Barkhausen Criterion - Basic Introduction](https://www.youtube.com/watch?v=skDVcnVwK3A) — The Organic Chemistry Tutor
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/electronics_devices_and_circuit/barkhausen-criteria-principle
- Whole chapter: https://www.bctengineer.com/md/semester_3/electronics_devices_and_circuit/chapter-5

## Question

State Barkhausen criteria and explain the principle of oscillation.

## Short answer

Barkhausen criteria: |Aβ|=1 and 0°/360° phase. Oscillation starts from noise; the feedback network selects one frequency meeting the phase condition. Initially |Aβ|>1, amplitude grows until nonlinear limiting makes |Aβ|=1, sustaining oscillation.

## Answer

**Barkhausen criteria:** An amplifier with feedback produces sustained sinusoidal oscillation at the frequency for which the loop gain Aβ satisfies both:

1. **Magnitude condition:** |Aβ| = 1 (loop gain is exactly unity)
2. **Phase condition:** the total phase shift around the loop is 0° or 360° (positive feedback), that is, ∠Aβ = 0°, 360°, ...

Here A is the amplifier gain and β is the feedback factor.

#### Principle of oscillation
An oscillator converts dc power into ac of a fixed frequency without any input signal. It consists of an amplifier, a positive feedback network, and a frequency-determining network (LC, RC or crystal).

```text
         +---------+
 Vs=0 -->|    A    |----+----> Vo
         +---------+    |
              ^         |
              |   +-----+
              +---|  β  |<-+
                  +-----+
```

1. At switch-on, the noise and the turn-on transient present in the circuit have components of many frequencies.
2. The amplifier amplifies these. The feedback network passes back a fraction β in phase (0° or 360° for only one frequency fo). So only that component is reinforced.
3. At first, the loop gain is slightly above 1 (|Aβ| > 1), so the amplitude grows exponentially.
4. As the amplitude increases, the amplifier saturates or a limiter reduces the gain, until |Aβ| = 1. The amplitude then becomes constant: a sustained oscillation of frequency fo.

With closed-loop gain Af = A/(1 − Aβ): when Aβ = 1 the denominator is zero, so the gain is infinite, which means an output exists with no input. If |Aβ| < 1 the oscillation dies out; if |Aβ| > 1 (and not limited) the output is distorted.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What starts oscillation when the circuit is switched on?
   A. An external input signal
   B. Noise and the turn-on transient containing many frequencies
   C. A battery pulse only
   D. The load resistor
   Answer: B. Noise has all frequencies; the one with correct phase is reinforced by positive feedback. (Key point: Start of oscillation)

2. Why must |Aβ| be slightly above 1 initially?
   A. So the amplitude grows exponentially from noise
   B. So the oscillation dies out
   C. To reduce distortion
   D. To make the phase 180°
   Answer: A. |Aβ| > 1 makes the amplitude build up until limiting. (Key point: Initial loop gain)

3. How does the amplitude become constant?
   A. Saturation or a limiter reduces gain until |Aβ| = 1
   B. The feedback is disconnected
   C. β increases without limit
   D. The frequency changes
   Answer: A. As amplitude rises the gain falls, settling at |Aβ| = 1. (Key point: Amplitude stabilisation)

4. What does Aβ = 1 mean for the closed-loop gain Af = A/(1 - Aβ)?
   A. Af = 0
   B. Af = 1
   C. Af is infinite, i.e. output exists with no input
   D. Af = A
   Answer: C. The denominator becomes zero, so an output can exist without any input. (Key point: Af = A/(1 - Aβ))

## Related in Electronics Devices and Circuit

- [Barkhausen criteria and RC phase shift oscillator](https://www.bctengineer.com/question.md?key=semester_3%2Felectronics_devices_and_circuit%3Abarkhausen-rc-phase-shift) — Electronics Devices and Circuit, chapter 5, asked 3×
- [Barkhausen criteria and Wien bridge oscillator](https://www.bctengineer.com/question.md?key=semester_3%2Felectronics_devices_and_circuit%3Abarkhausen-wien-bridge) — Electronics Devices and Circuit, chapter 5, asked 2×
- [Barkhausen criteria and 50% duty cycle from 555](https://www.bctengineer.com/question.md?key=semester_3%2Felectronics_devices_and_circuit%3Abarkhausen-555-duty-cycle) — Electronics Devices and Circuit, chapter 5
- [Barkhausen criteria and RC oscillator using op-amp](https://www.bctengineer.com/question.md?key=semester_3%2Felectronics_devices_and_circuit%3Abarkhausen-rc-opamp-oscillator) — Electronics Devices and Circuit, chapter 5

## Related in other subjects

- [Barkhausen criteria; Wien bridge frequency](https://www.bctengineer.com/question.md?key=semester_2%2Fbasic_electronics_engineering%3Abarkhausen-wien-derive-frequency) — Basic Electronics Engineering, chapter 4
- [Barkhausen criteria and relaxation oscillator](https://www.bctengineer.com/question.md?key=semester_1%2Ffundamental_of_electrical_and_electronics_engineering%3Abarkhausen-relaxation-oscillator) — Fundamental of Electrical and Electronics Engineering, chapter 6
- [Barkhausen criteria and Wien bridge oscillator](https://www.bctengineer.com/question.md?key=semester_1%2Ffundamental_of_electrical_and_electronics_engineering%3Abarkhausen-wien-bridge-oscillator) — Fundamental of Electrical and Electronics Engineering, chapter 6
- [Barkhausen criteria and square wave generator](https://www.bctengineer.com/question.md?key=semester_2%2Fbasic_electronics_engineering%3Abarkhausen-square-wave-generator) — Basic Electronics Engineering, chapter 4
