Abstract
The Langevin equation describing the Brownian motion of particles is studied in the case when the friction depends nonlinearly on the particle velocity. The intensity \(D(\upsilon )\) of the thermal random force driving the particles then, in equilibrium systems, also depends on the velocity, and the equation of motion should contain an additional ‘spurious’ force proportional to the derivative of \(D(\upsilon )\). This force is chosen in the kinetic representation, for which the stationary probability density for velocities is the Maxwell distribution and simultaneously the generalized Einstein relation is obeyed. A general formula for the diffusion coefficient of the particle is obtained and then specified for various models of dissipative forces studied in the literature, in particular, for the power-law friction. In this case the scaling of the diffusion coefficient with the model parameters is obtained also by a simple dimensional analysis, for systems both at equilibrium and far from it, when \(D\) is usually assumed to be independent of \(\upsilon \).
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Acknowledgments
This work was supported by the Agency for the Structural Funds of the EU within the Projects NFP 26220120021, 26220120033, 26110230061, and by the Grant VEGA 1/0370/12.
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Lisý, V., Tóthová, J. & Glod, L. Diffusion in a Medium with Nonlinear Friction. Int J Thermophys 35, 2001–2010 (2014). https://doi.org/10.1007/s10765-013-1501-4
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DOI: https://doi.org/10.1007/s10765-013-1501-4