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An explanation of the sheath instability

dc.contributor.authorPandey, B. P.en_US
dc.contributor.authorRoy, Subrataen_US
dc.date.accessioned2010-05-06T21:04:06Z
dc.date.available2010-05-06T21:04:06Z
dc.date.issued2003-01en_US
dc.identifier.citationPandey, B. P.; Roy, Subrata (2003). "An explanation of the sheath instability." Physics of Plasmas 10(1): 5-8. <http://hdl.handle.net/2027.42/69739>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/69739
dc.identifier.urihttp://www.ncbi.nlm.nih.gov/sites/entrez?cmd=retrieve&db=pubmed&list_uids=4638010&dopt=citationen_US
dc.description.abstractWhen the sheath accelerates in its plasma–bound motion as a result of the ion response to the electric field, one has a top-heavy equilibrium. In the sheath frame ions are accelerated towards the wall–sheath boundary. In such a situation sheath may become unstable. The sheath instability is examined as the Rayleigh–Taylor (RT) instability and RT growth rate is compared with the reported sheath instability in the literature. © 2003 American Institute of Physics.en_US
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dc.format.extent54350 bytes
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleAn explanation of the sheath instabilityen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumComputational Plasma Dynamics Laboratory, Kettering University, Flint, Michigan 48504en_US
dc.identifier.pmid4638010en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/69739/2/PHPAEN-10-1-5-1.pdf
dc.identifier.doi10.1063/1.1526091en_US
dc.identifier.sourcePhysics of Plasmasen_US
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dc.owningcollnamePhysics, Department of


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