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dc.contributorVirginia Techen_US
dc.contributor.authorXing, Zengpingen_US
dc.contributor.authorDong, Shuxiangen_US
dc.contributor.authorZhai, Junyien_US
dc.contributor.authorYan, Lien_US
dc.contributor.authorLi, Jiefangen_US
dc.contributor.authorViehland, Dwight D.en_US
dc.date.accessioned2014-01-28T18:00:17Z
dc.date.available2014-01-28T18:00:17Z
dc.date.issued2006-09-01
dc.identifier.citationXing, Zengping; Dong, Shuxiang; Zhai, Junyi; et al., "Resonant bending mode of Terfenol-D/steel/Pb(Zr,Ti)O-3 magnetoelectric laminate composites," Appl. Phys. Lett. 89, 112911 (2006); http://dx.doi.org/10.1063/1.2353819
dc.identifier.issn0003-6951
dc.identifier.urihttp://hdl.handle.net/10919/25198
dc.description.abstractResonant bending-mode Tb1-xDyxFe2-y/elastic-steel/Pb(Zr,Ti)O-3 magnetoelectric (ME) laminate composites have been investigated. An elastic-steel layer with a relatively high Q(m) significantly increases the resonant enhancement of the ME coefficient due to an increased effective Q(m) of the laminate. The three-phase ME laminates have a low first-order bending frequency of similar to 5 kHz, with a resonance-enhanced ME coefficient of similar to 40 V/cm Oe. (c) 2006 American Institute of Physics. (c) 2006 American Institute of Physics.
dc.format.mimetypeapplication/pdfen_US
dc.language.isoen_US
dc.publisherAIP Publishing
dc.subjectLead zirconate titanateen_US
dc.subjectTerfenol-den_US
dc.subjectEfficiencyen_US
dc.subjectFrequencyen_US
dc.subjectTransverseen_US
dc.subjectDependenceen_US
dc.subjectEnergyen_US
dc.subjectPhysicsen_US
dc.titleResonant bending mode of Terfenol-D/steel/Pb(Zr,Ti)O-3 magnetoelectric laminate compositesen_US
dc.typeArticleen_US
dc.identifier.urlhttp://scitation.aip.org/content/aip/journal/apl/89/11/10.1063/1.2353819
dc.date.accessed2014-01-17
dc.title.serialApplied Physics Letters
dc.identifier.doihttps://doi.org/10.1063/1.2353819
dc.type.dcmitypeTexten_US


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