Falling plumes in bacterial bioconvection
Experiments by Kessler on bioconvection in laboratory suspensions of bacteria (Bacillus subtilis), contained in a deep chamber, reveal the development of a thin upper boundary layer of cell-rich fluid which becomes unstable, leading to the formation of falling plumes. We use the continuum descriptio...
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Veröffentlicht in: | Journal of fluid mechanics 2001-10, Vol.445, p.121-149 |
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container_title | Journal of fluid mechanics |
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creator | METCALFE, AISLING M. PEDLEY, T. J. |
description | Experiments by Kessler on bioconvection in laboratory suspensions of bacteria (Bacillus
subtilis), contained in a deep chamber, reveal the development of a thin upper
boundary layer of cell-rich fluid which becomes unstable, leading to the formation of
falling plumes. We use the continuum description of such a suspension developed by
Hillesdon et al. (1995) as the basis for a theoretical model of the boundary layer and
an axisymmetric plume. If the boundary layer has dimensionless thickness λ [Lt ] 1, the
plume has width λ1/2. A similarity solution is found for the plume in which the cell
flux and volume flux can be matched to those in the boundary layer and in the bulk of
the suspension outside both regions. The corresponding model for a two-dimensional
plume fails to give a self-consistent solution. |
doi_str_mv | 10.1017/S0022112001005547 |
format | Article |
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subtilis), contained in a deep chamber, reveal the development of a thin upper
boundary layer of cell-rich fluid which becomes unstable, leading to the formation of
falling plumes. We use the continuum description of such a suspension developed by
Hillesdon et al. (1995) as the basis for a theoretical model of the boundary layer and
an axisymmetric plume. If the boundary layer has dimensionless thickness λ [Lt ] 1, the
plume has width λ1/2. A similarity solution is found for the plume in which the cell
flux and volume flux can be matched to those in the boundary layer and in the bulk of
the suspension outside both regions. The corresponding model for a two-dimensional
plume fails to give a self-consistent solution.</description><identifier>ISSN: 0022-1120</identifier><identifier>EISSN: 1469-7645</identifier><identifier>DOI: 10.1017/S0022112001005547</identifier><identifier>CODEN: JFLSA7</identifier><language>eng</language><publisher>Cambridge, UK: Cambridge University Press</publisher><subject>Bacillus subtilis ; Bacteriology ; Biological and medical sciences ; Boundary layers ; Fundamental and applied biological sciences. Psychology ; Microbiology ; Motility, taxis ; Plumes</subject><ispartof>Journal of fluid mechanics, 2001-10, Vol.445, p.121-149</ispartof><rights>2001 Cambridge University Press</rights><rights>2001 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c557t-c544f22f5671746a347fc3984871ac1e89d6c37690ccb26b54ef28f8c2c411493</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.cambridge.org/core/product/identifier/S0022112001005547/type/journal_article$$EHTML$$P50$$Gcambridge$$H</linktohtml><link.rule.ids>164,314,776,780,27903,27904,55607</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=1121050$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>METCALFE, AISLING M.</creatorcontrib><creatorcontrib>PEDLEY, T. J.</creatorcontrib><title>Falling plumes in bacterial bioconvection</title><title>Journal of fluid mechanics</title><addtitle>J. Fluid Mech</addtitle><description>Experiments by Kessler on bioconvection in laboratory suspensions of bacteria (Bacillus
subtilis), contained in a deep chamber, reveal the development of a thin upper
boundary layer of cell-rich fluid which becomes unstable, leading to the formation of
falling plumes. We use the continuum description of such a suspension developed by
Hillesdon et al. (1995) as the basis for a theoretical model of the boundary layer and
an axisymmetric plume. If the boundary layer has dimensionless thickness λ [Lt ] 1, the
plume has width λ1/2. A similarity solution is found for the plume in which the cell
flux and volume flux can be matched to those in the boundary layer and in the bulk of
the suspension outside both regions. The corresponding model for a two-dimensional
plume fails to give a self-consistent solution.</description><subject>Bacillus subtilis</subject><subject>Bacteriology</subject><subject>Biological and medical sciences</subject><subject>Boundary layers</subject><subject>Fundamental and applied biological sciences. Psychology</subject><subject>Microbiology</subject><subject>Motility, taxis</subject><subject>Plumes</subject><issn>0022-1120</issn><issn>1469-7645</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><sourceid>8G5</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><sourceid>GUQSH</sourceid><sourceid>M2O</sourceid><recordid>eNqFkFtLAzEQhYMoWKs_wLdFRPBhNZPr7qMUWy8FqZcXX0I2zZbUvdRkK_rvTWlRUMSXmYHzzeHMIHQI-AwwyPMHjAkBIBgDxpwzuYV6wESeSsH4Nuqt5HSl76K9EOYRoziXPXQ61FXlmlmyqJa1DYlrkkKbznqnq6RwrWmbN2s61zb7aKfUVbAHm95HT8PLx8FVOr4bXQ8uxqnhXHaxMlYSUnIhQTKhKZOloXnGMgnagM3yqTBUihwbUxBRcGZLkpWZIYYBsJz20cnad-Hb16UNnapdMLaqdGPbZVCUZSInQP8FCWDBMJMRPPoBztulb-IRKybLY9QsQrCGjG9D8LZUC-9q7T8UYLV6sfr14rhzvDHWweiq9LoxLnwvQrTnOGLpGnOhs-9fsvYvSkgquRKjSZzGz_eTm6G6jTzdRNF14d10Zr8D_x3mE2cUldc</recordid><startdate>20011025</startdate><enddate>20011025</enddate><creator>METCALFE, AISLING M.</creator><creator>PEDLEY, T. 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J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c557t-c544f22f5671746a347fc3984871ac1e89d6c37690ccb26b54ef28f8c2c411493</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>Bacillus subtilis</topic><topic>Bacteriology</topic><topic>Biological and medical sciences</topic><topic>Boundary layers</topic><topic>Fundamental and applied biological sciences. Psychology</topic><topic>Microbiology</topic><topic>Motility, taxis</topic><topic>Plumes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>METCALFE, AISLING M.</creatorcontrib><creatorcontrib>PEDLEY, T. 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J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Falling plumes in bacterial bioconvection</atitle><jtitle>Journal of fluid mechanics</jtitle><addtitle>J. Fluid Mech</addtitle><date>2001-10-25</date><risdate>2001</risdate><volume>445</volume><spage>121</spage><epage>149</epage><pages>121-149</pages><issn>0022-1120</issn><eissn>1469-7645</eissn><coden>JFLSA7</coden><abstract>Experiments by Kessler on bioconvection in laboratory suspensions of bacteria (Bacillus
subtilis), contained in a deep chamber, reveal the development of a thin upper
boundary layer of cell-rich fluid which becomes unstable, leading to the formation of
falling plumes. We use the continuum description of such a suspension developed by
Hillesdon et al. (1995) as the basis for a theoretical model of the boundary layer and
an axisymmetric plume. If the boundary layer has dimensionless thickness λ [Lt ] 1, the
plume has width λ1/2. A similarity solution is found for the plume in which the cell
flux and volume flux can be matched to those in the boundary layer and in the bulk of
the suspension outside both regions. The corresponding model for a two-dimensional
plume fails to give a self-consistent solution.</abstract><cop>Cambridge, UK</cop><pub>Cambridge University Press</pub><doi>10.1017/S0022112001005547</doi><tpages>29</tpages></addata></record> |
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subjects | Bacillus subtilis Bacteriology Biological and medical sciences Boundary layers Fundamental and applied biological sciences. Psychology Microbiology Motility, taxis Plumes |
title | Falling plumes in bacterial bioconvection |
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