Topological chaos in inviscid and viscous mixers
Topological chaos may be used to generate highly effective laminar mixing in a simple batch stirring device. Boyland, Aref and Stremler (2000) have computed a material stretch rate that holds in a chaotic flow, provided it has appropriate topological properties, irrespective of the details of the fl...
| Main Authors: | , , |
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| Format: | Journal article |
| Language: | English |
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2003
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| _version_ | 1797076535626170368 |
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| author | Finn, MD Cox, S Byrne, H |
| author_facet | Finn, MD Cox, S Byrne, H |
| author_sort | Finn, MD |
| collection | OXFORD |
| description | Topological chaos may be used to generate highly effective laminar mixing in a simple batch stirring device. Boyland, Aref and Stremler (2000) have computed a material stretch rate that holds in a chaotic flow, provided it has appropriate topological properties, irrespective of the details of the flow. Their theoretical approach, while widely applicable, cannot predict the size of the region in which this stretch rate is achieved. Here, we present numerical simulations to support the observation of Boyland et al. that the region of high stretch is comparable with that through which the stirring elements move during operation of the device. We describe a fast technique for computing the velocity field for either inviscid, irrotational or highly viscous flow, which enables accurate numerical simulation of dye advection. We calculate material stretch rates, and find close agreement with those of Boyland et al., irrespective of whether the fluid is modelled as inviscid or viscous, even though there are significant differences between the flow fields generated in the two cases. |
| first_indexed | 2024-03-07T00:05:06Z |
| format | Journal article |
| id | oxford-uuid:774917d1-feb6-4f88-b19e-1c91376e1232 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T00:05:06Z |
| publishDate | 2003 |
| record_format | dspace |
| spelling | oxford-uuid:774917d1-feb6-4f88-b19e-1c91376e12322022-03-26T20:22:53ZTopological chaos in inviscid and viscous mixersJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:774917d1-feb6-4f88-b19e-1c91376e1232EnglishSymplectic Elements at Oxford2003Finn, MDCox, SByrne, HTopological chaos may be used to generate highly effective laminar mixing in a simple batch stirring device. Boyland, Aref and Stremler (2000) have computed a material stretch rate that holds in a chaotic flow, provided it has appropriate topological properties, irrespective of the details of the flow. Their theoretical approach, while widely applicable, cannot predict the size of the region in which this stretch rate is achieved. Here, we present numerical simulations to support the observation of Boyland et al. that the region of high stretch is comparable with that through which the stirring elements move during operation of the device. We describe a fast technique for computing the velocity field for either inviscid, irrotational or highly viscous flow, which enables accurate numerical simulation of dye advection. We calculate material stretch rates, and find close agreement with those of Boyland et al., irrespective of whether the fluid is modelled as inviscid or viscous, even though there are significant differences between the flow fields generated in the two cases. |
| spellingShingle | Finn, MD Cox, S Byrne, H Topological chaos in inviscid and viscous mixers |
| title | Topological chaos in inviscid and viscous mixers |
| title_full | Topological chaos in inviscid and viscous mixers |
| title_fullStr | Topological chaos in inviscid and viscous mixers |
| title_full_unstemmed | Topological chaos in inviscid and viscous mixers |
| title_short | Topological chaos in inviscid and viscous mixers |
| title_sort | topological chaos in inviscid and viscous mixers |
| work_keys_str_mv | AT finnmd topologicalchaosininviscidandviscousmixers AT coxs topologicalchaosininviscidandviscousmixers AT byrneh topologicalchaosininviscidandviscousmixers |