Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1729
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dc.contributor.authorSatin, Seemaen_US
dc.contributor.authorParvate, Abhayen_US
dc.contributor.authorGANGAL, A. D.en_US
dc.date.accessioned2019-02-14T05:05:04Z
dc.date.available2019-02-14T05:05:04Z
dc.date.issued2013-07en_US
dc.identifier.citationChaos, Solitons and Fractals, 52, 30-35.en_US
dc.identifier.issn0960-0779en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1729-
dc.identifier.urihttps://doi.org/10.1016/j.chaos.2013.03.013en_US
dc.description.abstractA Fokker–Planck equation on fractal curves is obtained, starting from Chapmann–Kolmogorov equation on fractal curves. This is done using the recently developed calculus on fractals, which allows one to write differential equations on fractal curves. As an important special case, the diffusion and drift coefficients are obtained, for a suitable transition probability to get the diffusion equation on fractal curves. This equation is of first order in time, and, in space variable it involves derivatives of order α, α being the dimension of the curve. An exact solution of this equation with localized initial condition shows departure from ordinary diffusive behavior due to underlying fractal space in which diffusion is taking place and manifests a subdiffusive behavior. We further point out that the dimension of the fractal path can be estimated from the distribution function.en_US
dc.language.isoenen_US
dc.publisherElsevier B.V.en_US
dc.subjectFractal curvesen_US
dc.subjectPhysical phenomenaen_US
dc.subjectAnomalous transporten_US
dc.subjectCentral Limit theoremen_US
dc.subject2013en_US
dc.titleFokker–Planck equation on fractal curvesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleChaosen_US
dc.publication.originofpublisherForeignen_US
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