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dc.contributor.authorSarhangi, G.R.en_US
dc.contributor.authorNajafi, M.en_US
dc.contributor.authorWang, H.en_US
dc.date.accessioned2011-12-20T23:06:19Z
dc.date.available2011-12-20T23:06:19Z
dc.date.issued1992-06-24en_US
dc.identifier.citationSarhangi, G.R.; Najafi, M.; Wang, H.; , "The Stabilization of a Linearized Self-Excited Wave Equation by an Energy Absorbing Boundary," American Control Conference, 1992 , vol., no., pp.2153-2155, 24-26 June 1992en_US
dc.identifier.isbn080302109en_US
dc.identifier.urihttp://hdl.handle.net/10057/4056
dc.descriptionThe full text of this article is not available on SOAR. WSU users can access the article via IEEE Xplore database licensed by University Libraries: http://libcat.wichita.edu/vwebv/holdingsInfo?bibId=1045954en_US
dc.description.abstractWe study the linrized self-excited wave quation tt - A £ -P(s) tg=0, where P(s)>0, P(r)eL(f), in a bounded domain 0cRI with smooth bounar r whee boun y dampig is prst. coniering the prtii Fr 1r.).of he bouM~ ron which w=O on r_ and 1,+ Kmt + L= 0, on r+, find two dif t bounds for P suck that the eneg decays exponentialy in the ener spae - t tends to infinity (Herewe aumer+ n rP == frn > 3). Bothbounds deend on 0(The domain of wave equation in Rn, n > 1). The scond bound also depends on the fed-bak fuctioneK, L ELo(r) or more precisely on a positive funtion k(s) 6 Lo(r +) which detrin K and L on the prttion r+.en_US
dc.language.isoen_USen_US
dc.publisherIEEEen_US
dc.relation.ispartofseriesAmerican Control Conference, 1992 , vol., no., pp.2153-2155en_US
dc.subjectChromiumen_US
dc.subjectDampingen_US
dc.subjectH infinity controlen_US
dc.subjectNeodymiumen_US
dc.subjectPartial differential equationsen_US
dc.titleThe stabilization of a linearized self-excited wave equation by an energy absorbing boundaryen_US
dc.typeConference paperen_US
dc.description.versionPeer reviewed articleen_US
dc.rights.holder© IEEE,1992en_US


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