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dc.contributor.authorA. Prasatkhetragarnen_US
dc.contributor.authorP. Ketsuwanen_US
dc.contributor.authorS. Anantaen_US
dc.contributor.authorR. Yimnirunen_US
dc.contributor.authorD. P. Cannen_US
dc.date.accessioned2018-09-10T03:17:35Z-
dc.date.available2018-09-10T03:17:35Z-
dc.date.issued2009-06-15en_US
dc.identifier.issn0167577Xen_US
dc.identifier.other2-s2.0-64049099243en_US
dc.identifier.other10.1016/j.matlet.2009.02.063en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=64049099243&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/59580-
dc.description.abstractCeramics in a PZT-PCN system with the formula (1 - x)Pb(Zr1/2Ti1/2)O3-(x)Pb(Co1/3Nb2/3)O3, where x = 0.0, 0.1, 0.2, 0.3, 0.4, 0.5, and 1.0, were prepared using a solid-state mixed-oxide technique with columbite-CoNb2O6and wolframite-ZrTiO4precursors. The crystal structure of the specimens studied with X-ray diffraction (XRD) analysis showed a coexistence between tetragonal and pseudo cubic phases at composition x = 0.2. The SEM micrograph showed that the average grain size significantly decreased with increasing PCN content. A maximum dielectric constant was observed at composition x = 0.2, while the transition temperature strongly decreased with increasing PCN content. All ceramics also showed diffused phase transition behaviors with a minimum diffusivity at x = 0.2. The morphotropic phase boundary (MPB) lay at the 0.8PZT-0.2PCN composition. © 2009 Elsevier B.V.en_US
dc.subjectEngineeringen_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titlePhase formation, microstructure, and dielectric properties of (1 - x)PZT-(x)PCN ceramicsen_US
dc.typeJournalen_US
article.title.sourcetitleMaterials Lettersen_US
article.volume63en_US
article.stream.affiliationsNaresuan Universityen_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsSuranaree University of Technologyen_US
article.stream.affiliationsOregon State Universityen_US
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