Title:
Phase bubbles and spatiotemporal chaos in granular patterns

dc.contributor.author Moon, Sung Joon en_US
dc.contributor.author Shattuck, M. D. en_US
dc.contributor.author Bizon, C. en_US
dc.contributor.author Goldman, Daniel I. en_US
dc.contributor.author Swift, J. B. en_US
dc.contributor.author Swinney, Harry L. en_US
dc.contributor.corporatename Georgia Institute of Technology. School of Physics en_US
dc.contributor.corporatename University of Texas at Austin. Center for Nonlinear Dynamics en_US
dc.contributor.corporatename University of Texas at Austin. Dept. of Physics en_US
dc.contributor.corporatename Northwest Research Associates. Colorado Research Associates Division en_US
dc.date.accessioned 2012-08-29T19:02:39Z
dc.date.available 2012-08-29T19:02:39Z
dc.date.issued 2001-12-04
dc.description © 2001 The American Physical Society en_US
dc.description The electronic version of this article is the complete one and can be found online at: http://link.aps.org/doi/10.1103/PhysRevE.65.011301| DOI: 10.1103/PhysRevE.65.011301 en_US
dc.description.abstract We use inelastic hard sphere molecular dynamics simulations and laboratory experiments to study patterns in vertically oscillated granular layers. The simulations and experiments reveal that phase bubbles spontaneously nucleate in the patterns when the container acceleration amplitude exceeds a critical value, about 7g, where the pattern is approximately hexagonal, oscillating at one-fourth the driving frequency (f/4). A phase bubble is a localized region that oscillates with a phase opposite (differing by π) to that of the surrounding pattern; a localized phase shift is often called an arching in studies of two-dimensional systems. The simulations show that the formation of phase bubbles is triggered by undulation at the bottom of the layer on a large length scale compared to the wavelength of the pattern. Once formed, a phase bubble shrinks as if it had a surface tension, and disappears in tens to hundreds of cycles. We find that there is an oscillatory momentum transfer across a kink, and the shrinking is caused by a net collisional momentum inward across the boundary enclosing the bubble. At increasing acceleration amplitudes, the patterns evolve into randomly moving labyrinthian kinks (spatiotemporal chaos). We observe in the simulations that f/3 and f/6 subharmonic patterns emerge as primary instabilities, but that they are unstable to the undulation of the layer. Our experiments confirm the existence of transient f/3 and f/6 patterns. en_US
dc.identifier.citation Sung Joon Moon, M. D. Shattuck, C. Bizon, Daniel I. Goldman, J. B. Swift, Harry L. Swinney, "Phase bubbles and spatiotemporal chaos in granular patterns,” Physical Review E, 65, 011301 (2001) en_US
dc.identifier.issn 1063-651X
dc.identifier.uri http://hdl.handle.net/1853/44583
dc.language.iso en_US en_US
dc.publisher Georgia Institute of Technology en_US
dc.publisher.original American Physical Society en_US
dc.subject Pattern formation en_US
dc.subject Granular systems en_US
dc.subject Fluid dynamics en_US
dc.subject Vertically oscillated granular layers en_US
dc.title Phase bubbles and spatiotemporal chaos in granular patterns en_US
dc.type Text
dc.type.genre Article
dspace.entity.type Publication
local.contributor.author Goldman, Daniel I.
local.contributor.corporatename College of Sciences
local.contributor.corporatename School of Physics
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relation.isOrgUnitOfPublication 2ba39017-11f1-40f4-9bc5-66f17b8f1539
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