2012
DOI: 10.1007/s10955-012-0570-2
|View full text |Cite
|
Sign up to set email alerts
|

Phase Space Reduction of the One-Dimensional Fokker-Planck (Kramers) Equation

Abstract: A pointlike particle of finite mass m, moving in a one-dimensional viscous environment and biased by a spatially dependent force, is considered. We present a rigorous mapping of the FokkerPlanck equation, which determines evolution of the particle density in phase space, onto the spatial coordinate x. The result is the Smoluchowski equation, valid in the overdamped limit, m → 0, with a series of corrections expanded in powers of m. They are determined unambiguously within the recurrence mapping procedure. The … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
8
0
1

Year Published

2012
2012
2024
2024

Publication Types

Select...
6
1

Relationship

1
6

Authors

Journals

citations
Cited by 10 publications
(9 citation statements)
references
References 38 publications
0
8
0
1
Order By: Relevance
“…With respect to previous attempts at incorporating finite-mass effects in the analysis of Brownian transport through corrugated narrow channels [31][32][33], we stress that the inertial effects reported here are not of mere academic interest [26].…”
Section: Discussionmentioning
confidence: 86%
“…With respect to previous attempts at incorporating finite-mass effects in the analysis of Brownian transport through corrugated narrow channels [31][32][33], we stress that the inertial effects reported here are not of mere academic interest [26].…”
Section: Discussionmentioning
confidence: 86%
“…More complex systems, such as confined diffusion driven by an external force along the channel, 26 diffusion biased by a transverse force, 27 or motion of massive particles described by the Fokker-Planck (Kramers) equation 28,29 can be mapped onto the longitudinal coordinate x using the same reduction scheme (the small parameter is proportional to the mass of particles in the last case). Anyhow, the result has the form of Eq.…”
Section: ∂ T P(x T) = ∂ X A(x)d(x)∂ X P(x T) A(x)mentioning
confidence: 99%
“…where m, ζ , D = (βζ ) −1 , and β = (k B T ) −1 respectively denote the particle mass, the friction coefficient, the diffusion coefficient, and the inverse thermal energy (k B is the Boltzmann constant and T is the absolute temperature), V (x) and V (x) are the potential and its second spatial derivative, andĴ (x) is the current operator in the overdamped limit (the Smoluchowski current operator). The factor [1 + mV (x)/ζ 2 ] can be associated with the position dependence of the diffusion coefficient (or mobility) [32]. It would seem that one could use the results obtained in early studies of ratchet systems [33][34][35][36], with the position-dependent particle mobility (or the friction coefficient), to account for the inertial correction in the present case.…”
Section: Introductionmentioning
confidence: 99%
“…The most well known and commonly used is the high-friction expansion of the Klein-Kramers equation [28][29][30][31]. In this way, the Klein-Kramers equation can be reduced to a Smoluchowski-like one-dimensional form [32] containing a series of corrections, so that the mapped equation respects inertia, although working in coordinate space. In the lowest order of such approximate dimension reduction, the mapped equation takes the form of the Smoluchowski equation with the current operator [28][29][30][31][32]…”
Section: Introductionmentioning
confidence: 99%