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Fokker-Planck equation

The Fokker-Planck equation describes the time evolution of the probability density function of position and velocity of a particle.

The first use of the Fokker-Planck equation was the statistical description of Brownian motion of a particle in a fluid.

Brownian motion follows the Langevin equation, which can be solved for many differrent stochastic forcings with results being averaged (the Monte Carlo Method).

However, instead of this computationally intensive approach, one can use the Fokker-Planck equation and consider , that is, the probability density function of the particle having a velocity in the interval , when it starts its motion with at time .

The general form of the Fokker-Planck equation for N variables is

,

where is the drift vector and the diffusion tensor, the latter of which results from the presence of the stochastic force.

Referenced By

Brownian motion | Brownian movement | Diffusion | Langevin equation | List of equations | List of mathematical topics (D-F) | List of mathematical topics (F-Z) | List of physics topics F-L

 

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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Fokker-Planck equation".

 

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