Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/5373
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dc.contributorDepartment of Electrical Engineering-
dc.creatorYang, F-
dc.creatorLeung, CM-
dc.creatorOr, DSW-
dc.creatorLiu, W-
dc.creatorZhang, Z-
dc.creatorDuan, Y-
dc.date.accessioned2014-12-11T08:27:14Z-
dc.date.available2014-12-11T08:27:14Z-
dc.identifier.issn0021-8979-
dc.identifier.urihttp://hdl.handle.net/10397/5373-
dc.language.isoenen_US
dc.publisherAmerican Institute of Physicsen_US
dc.rights© 2012 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in Fang Yang et al., J. Appl. Phys. 111, 07A940 (2012) and may be found at http://link.aip.org/link/?jap/111/07A940.en_US
dc.subjectElastic modulien_US
dc.subjectFilled polymersen_US
dc.subjectIron alloysen_US
dc.subjectMagnetic domain wallsen_US
dc.subjectMagnetic fluxen_US
dc.subjectMagnetic permeabilityen_US
dc.subjectMagnetoelastic effectsen_US
dc.subjectMagnetostrictionen_US
dc.subjectNeodymium alloysen_US
dc.subjectSamarium alloysen_US
dc.titleDynamic magnetoelastic properties of epoxy-bonded Sm₀. ₈₈Nd₀.₁₂Fe₁.₉₃ pseudo-1-3 negative magnetostrictive particulate compositeen_US
dc.typeJournal/Magazine Articleen_US
dc.description.otherinformationAuthor name used in this publication: Siu Wing Oren_US
dc.description.otherinformationAuthor name used in this publication: Yuan-Feng Duanen_US
dc.identifier.spage1-
dc.identifier.epage3-
dc.identifier.volume111-
dc.identifier.issue7-
dc.identifier.doi10.1063/1.3679045-
dcterms.abstractPseudo-1-3 negative magnetostrictive particulate composite is prepared by embedding and aligning light rare earth (Sm and Nd)-based negative magnetostrictive Sm₀. ₈₈Nd₀.₁₂Fe₁.₉₃ particles with randomly distributed sizes of 10–180 μm in a passive epoxy matrix using a particle volume fraction of 0.5. The dynamic magnetoelastic properties of the composite are investigated as a function of both magnetic bias field and frequency under a constant magnetic drive field. The dynamic relative permeability (μ[sub r]₃₃) exhibits a flat frequency response with no observable dispersion at all bias field levels, except for the fundamental shape resonance range of 40–50 kHz. The free (μ[sub r]₃₃[sup T]) and clamped (μ[sub r]₃₃[sup S]) relative permeabilities attain their maximum values at low bias field levels of ≤10 kA/m because of the relatively easy 180° domain-wall motion. The elastic modulus at constant magnetic field strength (E₃[sup H]) and that at constant magnetic flux density (E₃[sup B]) show a maximum negative-ΔE effect, accompanying a maximum dynamic strain coefficient (d₃₃) of −2 nm/A, at about 100 kA/m due to the maximum motion of non-180° domain walls.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of applied physics, 1 Apr. 2012, v. 111, no. 7, 07A940, p. 1-3-
dcterms.isPartOfJournal of applied physics-
dcterms.issued2012-04-01-
dc.identifier.isiWOS:000303282400144-
dc.identifier.scopus2-s2.0-84861738506-
dc.identifier.eissn1089-7550-
dc.identifier.rosgroupidr56202-
dc.description.ros2011-2012 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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