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Thermal noise
Thermal noise
Definition
Thermal noise, also known as Johnson-Nyquist noise, is electrical noise caused by the random thermal movement of charge carriers in a conductor or resistor. It occurs independently of external voltage sources and is a fundamental property of all electrical components at temperatures above absolute zero.
Origin
The constant thermal movement of electrons causes small voltage fluctuations that can be measured as a noise signal. Higher temperatures lead to stronger noise.
Mathematical description
The effective noise voltage VRMS
across a resistor R
is described by the following formula:
VRMS=√(4kB T R Δf)
- kB: Boltzmann constant (1.38 × 10-23 J/K)
- T: Temperature (Kelvin)
- R: Resistance (Ohm)
- Δf: Frequency bandwidth (Hertz)
Properties
- Broadband: Distributed over a large frequency spectrum (white noise).
- Temperature-dependent: Increasing temperature increases the noise.
- Unavoidable: Is part of the basic characteristic of electronic systems.
Technical significance
Thermal noise sets a fundamental limit for the sensitivity of amplifiers:
- Amplifiers
- Sensors
- Radio receivers
- Medical devices (e.g. EEG, ECG)
Differentiation from other types of noise
- Shot noise: Arises from discrete charge transports.
- 1/f noise: Increases at low frequencies.
- Quantisation noise: Occurs when analogue signals are digitised.
Summary
Thermal noise is an unavoidable, temperature-dependent form of electrical noise that determines the performance limits of electronic systems.