The swim force as a body force
- Creators
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Yan, Wen
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Brady, John F.
Abstract
Net (as opposed to random) motion of active matter results from an average swim (or propulsive) force. It is shown that the average swim force acts like a body force – an internal body force. As a result, the particle-pressure exerted on a container wall is the sum of the swim pressure [Takatori et al., Phys. Rev. Lett., 2014, 113, 028103] and the 'weight' of the active particles. A continuum description is possible when variations occur on scales larger than the run length of the active particles and gives a Boltzmann-like distribution from a balance of the swim force and the swim pressure. Active particles may also display 'action at a distance' and accumulate adjacent to (or be depleted from) a boundary without any external forces. In the momentum balance for the suspension – the mixture of active particles plus fluid – only external body forces appear.
Additional Information
© 2015 Royal Society of Chemistry. This article is licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported Licence. Received 29th May 2015; accepted 2nd July 2015. First published online 02 Jul 2015. This work was supported by NSF Grant No. CBET 1437570.Attached Files
Published - c5sm01318f.pdf
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Additional details
- Eprint ID
- 58884
- Resolver ID
- CaltechAUTHORS:20150714-134052439
- NSF
- CBET 1437570
- Created
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2015-07-15Created from EPrint's datestamp field
- Updated
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2021-11-10Created from EPrint's last_modified field