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Stochastic processes White and colored noises

Next we consider several noise sources. They are Gaussian sources if their support of values is due to a Gaussian distribution. Contrary the dichotomic telegraph process assumes two values, i.e. = A and 2 = A. We will always assume A = — A. [Pg.9]

The second classification of the noise classifies its temporal correlations. In case of white noise the noise is uncorrelated in time which corresponds [Pg.9]

The integral over the Gaussian white noise gives the Wiener process which stands for the trajectory of a Brownian particle. The integral during [Pg.10]

In case of a Brownian particle D is the spatial diffusion coefficient. [Pg.10]

The study of a Brownian particle suspended in a fluid lead also to the introduction of the exponentially correlated Ornstein-Uhlenbeck process [48], the only Markovian Gaussian non-white stochastic process [19, 22]. We present here the Langevin approach to this problem, hence we analyze the forces that act on a single Brownian particle. We suppose the particle having a mass m equal to unity, and we assume the force due to the hits with thermal activated molecules of the fluid to be a stochastic variable. Moreover, due to the viscosity of the fluid, a friction force proportional to the velocity of the particle has to be considered. All this yields the following equation [Pg.10]


See other pages where Stochastic processes White and colored noises is mentioned: [Pg.9]   


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