Originally posted by raiken
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Thermal noise is distinct from shot noise, which consists of additional current fluctuations that occur when a voltage is applied and a macroscopic current starts to flow. For the general case, the above definition applies to charge carriers in any type of conducting medium (e.g. ions in an electrolyte), not just resistors. It can be modeled by a voltage source representing the noise of the non-ideal resistor in series with an ideal noise free resistor.
The power spectral density, or voltage variance (mean square) per hertz of bandwidth, is given by
{v_{n}^2} = 4 k_B T R
where kB is Boltzmann's constant in joules per kelvin, T is the resistor's absolute temperature in kelvin, and R is the resistor value in ohms (Ω). Use this equation for quick calculation:
sqrt{{v_{n}^2}} = 0.13 sqrt{R} nV}/\sqrt{Hz}}.
For example, a 1 kΩ resistor at a temperature of 300 K has
sqrt{{v_{n}^2}} = sqrt{4 * 1.38 * 10^{-23} * {J}/{K} * 300K * 1 {k ohm} = 4.07 nV/\sqrt per Hz}}.
Originally posted by raiken
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-g
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