Adaptive Gaussian particle method for the solution of the Fokker-Planck equation
The Fokker‐Planck equation describes the evolution of the probability density for a stochastic ordinary differential equation (SODE) or a deterministic ordinary differential equation (ODE) with stochastic initial values. A solution strategy for this partial differential equation (PDE) up to a relati...
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Published in | Zeitschrift für angewandte Mathematik und Mechanik Vol. 92; no. 10; pp. 770 - 781 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Berlin
WILEY-VCH Verlag
01.10.2012
WILEY‐VCH Verlag |
Subjects | |
Online Access | Get full text |
ISSN | 0044-2267 1521-4001 |
DOI | 10.1002/zamm.201100088 |
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Summary: | The Fokker‐Planck equation describes the evolution of the probability density for a stochastic ordinary differential equation (SODE) or a deterministic ordinary differential equation (ODE) with stochastic initial values. A solution strategy for this partial differential equation (PDE) up to a relatively large number of dimensions is based on particle methods using Gaussians as basis functions. An initial probability density is decomposed into a sum of multivariate normal distributions and these are propagated according to the ODE. The decomposition as well as the propagation is subject to possibly large numerical errors due to the difficulty to control the spatial residual over the whole domain. In this paper a new particle method is derived, which allows a deterministic error control for the resulting probability density. It is based on global optimization and allows an adaption of an efficient surrogate model for the residual estimation.
The Fokker‐Planck equation describes the evolution of the probability density for a stochastic ordinary differential equation (SODE) or a deterministic ordinary differential equation (ODE) with stochastic initial values. A solution strategy for this partial differential equation (PDE) up to a relatively large number of dimensions is based on particle methods using Gaussians as basis functions. An initial probability density is decomposed into a sum of multivariate normal distributions and these are propagated according to the ODE. The decomposition as well as the propagation is subject to possibly large numerical errors due to the difficulty to control the spatial residual over the whole domain. In this paper a new particle method is derived, which allows a deterministic error control for the resulting probability density. It is based on global optimization and allows an adaption of an efficient surrogate model for the residual estimation. |
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Bibliography: | istex:ABECA5ED81E584477A9233C7AD8CC1F9EC46B321 ark:/67375/WNG-RPGXP76J-N ArticleID:ZAMM201100088 Phone: +49 6131 39 22831, Fax: +49 6131 39 23331 Phone: +49 40 42878 3876, Fax: +49 40 42878 2696 |
ISSN: | 0044-2267 1521-4001 |
DOI: | 10.1002/zamm.201100088 |