Coil-less fluxgate effect in amorphous wires

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dc.authoridBayri, Nevzat/0000-0001-7105-7707
dc.authoridKolat, Veli Serkan/0000-0002-8864-5051;
dc.authorwosidAtalay, Selcuk/AAA-5095-2021
dc.authorwosidAtalay, Funda/AAA-4130-2021
dc.authorwosidBayri, Nevzat/ABG-9663-2020
dc.authorwosidKolat, Veli Serkan/ABI-5280-2020
dc.authorwosidIzgi, tekin/ABH-5655-2020
dc.contributor.authorAtalay, S.
dc.contributor.authorBayri, N.
dc.contributor.authorIzgi, T.
dc.contributor.authorAtalay, F. E.
dc.contributor.authorKolat, V. S.
dc.date.accessioned2024-08-04T20:32:16Z
dc.date.available2024-08-04T20:32:16Z
dc.date.issued2010
dc.departmentİnönü Üniversitesien_US
dc.description.abstractIn this study, the coil-less fluxgate properties of as-received amorphous microwires with the compositions (Co(0.94)Fe(0.06))(72.5)Si(12.5)B(15), Fe(77.5)Si(7.5)B(15) and Co(72.5)Si(12.5)B(15) have been investigated. As its name implies, a coil-less fluxgate is a new type of magnetic field sensor without a coil. When the (Co(0.94)Fe(0.06))(72.5)Si(12.5)B(15) wire is magnetically saturated in the circumferential direction with a 30 kHz and 48 mA driving current and under the effect of 33 pi rad/m torsional strain, there is a linear variation in the second harmonic of the voltage from wire ends, U(wire) as a function of the applied external dc magnetic field, H(z), along the wire length. The slope of the second harmonic versus H(z) curve changes in opposite directions as the direction of torsional strain changes from the positive to the negative direction. Coil-less fluxgate effects in as-received Fe(77.5)Si(7.5)B(15) and Co(72.5)Si(12.5)B(15) wires have also been investigated. A very small change in the second harmonic of voltage U(wire) is observed in Fe(77.5)Si(7.5)B(15) wire, with some small hysteresis. (C) 2010 Elsevier B.V. All rights reserved.en_US
dc.description.sponsorshipTUBITAK [TBAG-109T361]en_US
dc.description.sponsorshipThis work was supported by TUBITAK under project number TBAG-109T361.en_US
dc.identifier.doi10.1016/j.sna.2009.12.028
dc.identifier.endpage42en_US
dc.identifier.issn0924-4247
dc.identifier.issue1en_US
dc.identifier.scopus2-s2.0-76349113343en_US
dc.identifier.scopusqualityQ1en_US
dc.identifier.startpage37en_US
dc.identifier.urihttps://doi.org/10.1016/j.sna.2009.12.028
dc.identifier.urihttps://hdl.handle.net/11616/94972
dc.identifier.volume158en_US
dc.identifier.wosWOS:000275628700005en_US
dc.identifier.wosqualityQ1en_US
dc.indekslendigikaynakWeb of Scienceen_US
dc.indekslendigikaynakScopusen_US
dc.language.isoenen_US
dc.publisherElsevier Science Saen_US
dc.relation.ispartofSensors and Actuators A-Physicalen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectFluxgateen_US
dc.subjectAmorphous wireen_US
dc.subjectMagnetic sensoren_US
dc.titleCoil-less fluxgate effect in amorphous wiresen_US
dc.typeArticleen_US

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