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The mathematical model can also be used to describe stock market fluctuations and other phenomena not resembling (other than mathematically) the random movement of minute particles.
Brownian motion was discovered by the biologist Robert Brown[?] in 1827. The story goes that Brown was studying pollen particles floating in water under the microscope, and he observed them executing the jittery motion that now bears his name. By doing the same with particles of dust, he was able to rule out that the motion was due to pollen being "alive", but it remained to explain the origin of the motion. The first to give a theory of Brownian motion was none other than Albert Einstein in 1905.
At that time the atomic nature of matter was still a controversial idea. Einstein observed that, if the kinetic theory of fluids was right, then the molecules of water would move at random and so a small particle would receive a random number of impacts of random strength and from random directions in any short period of time. This random bombardment by the molecules of the fluid would cause a sufficiently small particle to move in exactly the way described by Brown.
Description of the mathematical model
Mathematically, Brownian motion is a Wiener process, a stochastic process in which the conditional probability distribution of the particle's position at time t+dt, given that its position at time t is p, is a Normal distribution with a mean of p+μ dt and a variance of σ^{2} dt; the parameter μ is the drift velocity, and the parameter σ^{2} is the power of the noise. Brownian motion is related to the random walk problem and it is generic in the sense that many different stochastic processes reduce to Brownian motion in suitable limits.
The mathematical theory of Brownian motion has been applied in contexts ranging far beyond the movement of particles in fluids. For example, in the modern theory of option pricing, asset classes are sometimes modeled as if they move according to a Brownian motion with drift.
It turns out that the Wiener process is not a physically realistic model of the motion of Brownian particles. More sophisticated formulations of the problem have led to the mathematical theory of diffusion processes. The accompanying equation of motion is called the Langevin equation or the FokkerPlanck equation depending on whether it is formulated in terms of random trajectories or probability densities.
See also osmosis.
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