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dc.contributor.authorN. Jaitanongen_US
dc.contributor.authorW. C. Vittayakornen_US
dc.contributor.authorR. Yimnirunen_US
dc.contributor.authorA. Chaipanichen_US
dc.date.accessioned2018-09-04T04:47:57Z-
dc.date.available2018-09-04T04:47:57Z-
dc.date.issued2010-12-01en_US
dc.identifier.issn15635112en_US
dc.identifier.issn00150193en_US
dc.identifier.other2-s2.0-79955697070en_US
dc.identifier.other10.1080/00150193.2010.482900en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=79955697070&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/50941-
dc.description.abstractLead magnesium niobate titanate (PMNT) - Portland cement (PC) composites were produced. PMNT amount used in this work was 50% by volume. The ferroelectric (P-E) hysteresis behaviors were investigated as function of both frequency and electric field for all composites. From the results, it was found that there was an increase in both the instantaneous remnant polarization (Pir) and coercive field (Eic) when the applied field increased from 5 kV/cm to 20 kV/cm, Pirwas found to increase from 1.5 to 9.8 μC/cm2and Eicwaas found to increase from 3.4 to 13.8 kV/cm. On the other hand, Pirand Eicwere found to reduce from 11.1 to 8.8 μC/cm2and from 10.8 to 15.3 kV/cm respectively, when the frequency was increased from 30-90 Hz; ascribed to the delayed response of the polarization reversal to the varying external field.en_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titleFerroelectric hysteresis behavior of 0-3 PMNT-cement compositesen_US
dc.typeJournalen_US
article.title.sourcetitleFerroelectricsen_US
article.volume405en_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsSuranaree University of Technologyen_US
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