Active electrostatic stabilization of liquid bridges in low gravity
In experiments performed aboard NASA's low-gravity KC-135 aircraft, it was found that rapid active control of radial electrostatic stresses can be used to suppress the growth of the (2,0) mode on capillary bridges in air. This mode naturally becomes unstable on a cylindrical bridge when the len...
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| Veröffentlicht in: | Journal of fluid mechanics 2002-04, Vol.457, p.285-294 |
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| container_end_page | 294 |
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| container_start_page | 285 |
| container_title | Journal of fluid mechanics |
| container_volume | 457 |
| creator | THIESSEN, DAVID B. MARR-LYON, MARK J. MARSTON, PHILIP L. |
| description | In experiments performed aboard NASA's low-gravity KC-135 aircraft, it was found
that rapid active control of radial electrostatic stresses can be used to suppress the
growth of the (2,0) mode on capillary bridges in air. This mode naturally becomes
unstable on a cylindrical bridge when the length exceeds the Rayleigh–Plateau (RP)
limit. Capillary bridges having a small amount of electrical conductivity were deployed
with a ring electrode concentric with each end of the bridge. A signal produced by
optically sensing the shape of the bridge was used to control the electrode potentials
so as to counteract the growth of the (2,0) mode. Occasionally the uncontrolled
growth of the (3,0) mode was observed when the length far exceeded the RP limit.
Rapid breakup from the growth of the (2,0) mode on long bridges was confirmed
following deactivation of the control. |
| doi_str_mv | 10.1017/S0022112002007760 |
| format | Article |
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that rapid active control of radial electrostatic stresses can be used to suppress the
growth of the (2,0) mode on capillary bridges in air. This mode naturally becomes
unstable on a cylindrical bridge when the length exceeds the Rayleigh–Plateau (RP)
limit. Capillary bridges having a small amount of electrical conductivity were deployed
with a ring electrode concentric with each end of the bridge. A signal produced by
optically sensing the shape of the bridge was used to control the electrode potentials
so as to counteract the growth of the (2,0) mode. Occasionally the uncontrolled
growth of the (3,0) mode was observed when the length far exceeded the RP limit.
Rapid breakup from the growth of the (2,0) mode on long bridges was confirmed
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that rapid active control of radial electrostatic stresses can be used to suppress the
growth of the (2,0) mode on capillary bridges in air. This mode naturally becomes
unstable on a cylindrical bridge when the length exceeds the Rayleigh–Plateau (RP)
limit. Capillary bridges having a small amount of electrical conductivity were deployed
with a ring electrode concentric with each end of the bridge. A signal produced by
optically sensing the shape of the bridge was used to control the electrode potentials
so as to counteract the growth of the (2,0) mode. Occasionally the uncontrolled
growth of the (3,0) mode was observed when the length far exceeded the RP limit.
Rapid breakup from the growth of the (2,0) mode on long bridges was confirmed
following deactivation of the control.</description><subject>Conductivity</subject><subject>Electrodes</subject><subject>Electrostatics</subject><subject>Exact sciences and technology</subject><subject>Fluid dynamics</subject><subject>Fluid mechanics</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Gravity</subject><subject>Hydrodynamic stability</subject><subject>Magnetohydrodynamics and electrohydrodynamics</subject><subject>Physics</subject><subject>Surface-tension-driven instability</subject><issn>0022-1120</issn><issn>1469-7645</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</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>eNp1kF9LwzAUxYMoOKcfwLeC6Fv15k-T9nFOncJAREXfQpYmI7NrZ9JN56c3Y0NF8ekQzu_enHsQOsRwigGLs3sAQjAmUQCE4LCFOpjxIhWcZduos7LTlb-L9kKYAGAKheigfk-3bmESUxnd-ia0qnU6iTJylfuIj6ZOGptU7nXuymTkXTk2IXF1UjVvydirhWuX-2jHqiqYg4120ePV5UP_Oh3eDm76vWGqGSdtykhOIeOlYgp4kRGS69IWuhxZDJRTxS3Li8JkmHJghBmqjLACmCKmtAZy2kUn670z37zOTWjl1AVtqkrVppkHSUS8vCAkgke_wEkz93XMJjHDOaPxexEpvKZ0vDt4Y-XMu6nyS4lBrkqVf0qNM8ebzSpoVVmvau3C9yDluCAii1y65lxozfuXr_yL5IKKTPLBncTP5PyJnF_IQeTpJouarkv-EfnfNJ_zT5Mi</recordid><startdate>20020425</startdate><enddate>20020425</enddate><creator>THIESSEN, DAVID B.</creator><creator>MARR-LYON, MARK J.</creator><creator>MARSTON, PHILIP L.</creator><general>Cambridge University Press</general><scope>BSCLL</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TB</scope><scope>7U5</scope><scope>7UA</scope><scope>7XB</scope><scope>88I</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>C1K</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>FR3</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>H8D</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KR7</scope><scope>L.G</scope><scope>L6V</scope><scope>L7M</scope><scope>M2O</scope><scope>M2P</scope><scope>M7S</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope><scope>Q9U</scope><scope>S0W</scope></search><sort><creationdate>20020425</creationdate><title>Active electrostatic stabilization of liquid bridges in low gravity</title><author>THIESSEN, DAVID B. ; 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Fluid Mech</addtitle><date>2002-04-25</date><risdate>2002</risdate><volume>457</volume><spage>285</spage><epage>294</epage><pages>285-294</pages><issn>0022-1120</issn><eissn>1469-7645</eissn><coden>JFLSA7</coden><abstract>In experiments performed aboard NASA's low-gravity KC-135 aircraft, it was found
that rapid active control of radial electrostatic stresses can be used to suppress the
growth of the (2,0) mode on capillary bridges in air. This mode naturally becomes
unstable on a cylindrical bridge when the length exceeds the Rayleigh–Plateau (RP)
limit. Capillary bridges having a small amount of electrical conductivity were deployed
with a ring electrode concentric with each end of the bridge. A signal produced by
optically sensing the shape of the bridge was used to control the electrode potentials
so as to counteract the growth of the (2,0) mode. Occasionally the uncontrolled
growth of the (3,0) mode was observed when the length far exceeded the RP limit.
Rapid breakup from the growth of the (2,0) mode on long bridges was confirmed
following deactivation of the control.</abstract><cop>Cambridge, UK</cop><pub>Cambridge University Press</pub><doi>10.1017/S0022112002007760</doi><tpages>10</tpages></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 0022-1120 |
| ispartof | Journal of fluid mechanics, 2002-04, Vol.457, p.285-294 |
| issn | 0022-1120 1469-7645 |
| language | eng |
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| source | Cambridge University Press Journals Complete |
| subjects | Conductivity Electrodes Electrostatics Exact sciences and technology Fluid dynamics Fluid mechanics Fundamental areas of phenomenology (including applications) Gravity Hydrodynamic stability Magnetohydrodynamics and electrohydrodynamics Physics Surface-tension-driven instability |
| title | Active electrostatic stabilization of liquid bridges in low gravity |
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