%0 Journal Article %1 artale:3162 %A Artale, V. %A Boffetta, G. %A Celani, A. %A Cencini, M. %A Vulpiani, A. %D 1997 %I AIP %J Physics of Fluids %K cencini chaos diffusion finite-size-lyapunov-exponent fluid_dynamics fsle lyapunov %N 11 %P 3162-3171 %R 10.1063/1.869433 %T Dispersion of passive tracers in closed basins: Beyond the diffusion coefficient %U http://link.aip.org/link/?PHF/9/3162/1 %V 9 %X We investigate the spreading of passive tracers in closed basins. If the characteristic length scale of the Eulerian velocities is not very small compared with the size of the basin the usual diffusion coefficient does not give any relevant information about the mechanism of spreading. We introduce a finite size characteristic time tau(delta) which describes the diffusive process at scale delta. When delta is small compared with the typical length of the velocity field one has tau(delta)~lambda–1, where lambda is the maximum Lyapunov exponent of the Lagrangian motion. At large delta the behavior of tau(delta) depends on the details of the system, in particular the presence of boundaries, and in this limit we have found a universal behavior for a large class of system under rather general hypothesis. The method of working at fixed scale delta makes more physical sense than the traditional way of looking at the relative diffusion at fixed delay times. This technique is displayed in a series of numerical experiments in simple flows.

@article{artale:3162, abstract = {We investigate the spreading of passive tracers in closed basins. If the characteristic length scale of the Eulerian velocities is not very small compared with the size of the basin the usual diffusion coefficient does not give any relevant information about the mechanism of spreading. We introduce a finite size characteristic time tau(delta) which describes the diffusive process at scale delta. When delta is small compared with the typical length of the velocity field one has tau(delta)~lambda–1, where lambda is the maximum Lyapunov exponent of the Lagrangian motion. At large delta the behavior of tau(delta) depends on the details of the system, in particular the presence of boundaries, and in this limit we have found a universal behavior for a large class of system under rather general hypothesis. The method of working at fixed scale delta makes more physical sense than the traditional way of looking at the relative diffusion at fixed delay times. This technique is displayed in a series of numerical experiments in simple flows.}, added-at = {2007-10-05T00:42:32.000+0200}, author = {Artale, V. and Boffetta, G. and Celani, A. and Cencini, M. and Vulpiani, A.}, biburl = {https://www.bibsonomy.org/bibtex/200cdc5f9111cddc0e552e77a01790769/mcencini}, description = {Physics of Fluids: Abstract View}, doi = {10.1063/1.869433}, interhash = {c45219307b6addfc79878a79c254bcb4}, intrahash = {00cdc5f9111cddc0e552e77a01790769}, journal = {Physics of Fluids}, keywords = {cencini chaos diffusion finite-size-lyapunov-exponent fluid_dynamics fsle lyapunov}, number = 11, pages = {3162-3171}, publisher = {AIP}, timestamp = {2007-10-05T00:45:37.000+0200}, title = {Dispersion of passive tracers in closed basins: Beyond the diffusion coefficient}, url = {http://link.aip.org/link/?PHF/9/3162/1}, volume = 9, year = 1997 }