Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction

We investigate a one-dimensional, many-body system consisting of particles interacting via repulsive, short-range forces, and moving in an overdamped regime under the effect of a drag force that depends on direction. That is, particles moving to the right do not experience the same drag as those mov...

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Main Authors: Angel Ricardo Plastino, Roseli S. Wedemann, Constantino Tsallis
Format: Article
Language:English
Published: MDPI AG 2021-09-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/13/9/1621
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author Angel Ricardo Plastino
Roseli S. Wedemann
Constantino Tsallis
author_facet Angel Ricardo Plastino
Roseli S. Wedemann
Constantino Tsallis
author_sort Angel Ricardo Plastino
collection DOAJ
description We investigate a one-dimensional, many-body system consisting of particles interacting via repulsive, short-range forces, and moving in an overdamped regime under the effect of a drag force that depends on direction. That is, particles moving to the right do not experience the same drag as those moving to the left. The dynamics of the system, effectively described by a non-linear, Fokker–Planck equation, exhibits peculiar features related to the way in which the drag force depends on velocity. The evolution equation satisfies an <i>H</i>-theorem involving the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>S</mi><mi>q</mi></msub></semantics></math></inline-formula> nonadditive entropy, and admits particular, exact, time-dependent solutions closely related, but not identical, to the <i>q</i>-Gaussian densities. The departure from the canonical, <i>q</i>-Gaussian shape is related to the fact that in one spatial dimension, in contrast to what occurs in two or more spatial dimensions, the drag’s dependence on direction entails that its dependence on velocity is necessarily (and severely) non-linear. The results reported here provide further evidence of the deep connections between overdamped, many-body systems, non-linear Fokker–Planck equations, and the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>S</mi><mi>q</mi></msub></semantics></math></inline-formula>-thermostatistics.
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spelling doaj.art-96113f8c2e574424ad3c9656fac913cb2023-11-22T15:27:32ZengMDPI AGSymmetry2073-89942021-09-01139162110.3390/sym13091621Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on DirectionAngel Ricardo Plastino0Roseli S. Wedemann1Constantino Tsallis2CeBio y Departamento de Ciencias Básicas, Universidad Nacional del Noroeste de la Província de Buenos Aires, UNNOBA-Conicet, Roque Saenz Peña, Junin 456, ArgentinaInstituto de Matemática e Estatística, Universidade do Estado do Rio de Janeiro, Rua São Francisco Xavier 524, Rio de Janeiro 20550-900, RJ, BrazilCentro Brasileiro de Pesquisas Físicas and National Institute of Science and Technology for Complex Systems, Rua Xavier Sigaud 150, Rio de Janeiro 22290-180, RJ, BrazilWe investigate a one-dimensional, many-body system consisting of particles interacting via repulsive, short-range forces, and moving in an overdamped regime under the effect of a drag force that depends on direction. That is, particles moving to the right do not experience the same drag as those moving to the left. The dynamics of the system, effectively described by a non-linear, Fokker–Planck equation, exhibits peculiar features related to the way in which the drag force depends on velocity. The evolution equation satisfies an <i>H</i>-theorem involving the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>S</mi><mi>q</mi></msub></semantics></math></inline-formula> nonadditive entropy, and admits particular, exact, time-dependent solutions closely related, but not identical, to the <i>q</i>-Gaussian densities. The departure from the canonical, <i>q</i>-Gaussian shape is related to the fact that in one spatial dimension, in contrast to what occurs in two or more spatial dimensions, the drag’s dependence on direction entails that its dependence on velocity is necessarily (and severely) non-linear. The results reported here provide further evidence of the deep connections between overdamped, many-body systems, non-linear Fokker–Planck equations, and the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>S</mi><mi>q</mi></msub></semantics></math></inline-formula>-thermostatistics.https://www.mdpi.com/2073-8994/13/9/1621non-linear Fokker–Planck equationdirection-dependent drag<i>H</i>-theorem
spellingShingle Angel Ricardo Plastino
Roseli S. Wedemann
Constantino Tsallis
Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
Symmetry
non-linear Fokker–Planck equation
direction-dependent drag
<i>H</i>-theorem
title Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
title_full Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
title_fullStr Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
title_full_unstemmed Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
title_short Nonlinear Fokker-Planck Equation for an Overdamped System with Drag Depending on Direction
title_sort nonlinear fokker planck equation for an overdamped system with drag depending on direction
topic non-linear Fokker–Planck equation
direction-dependent drag
<i>H</i>-theorem
url https://www.mdpi.com/2073-8994/13/9/1621
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