Please use this identifier to cite or link to this item: http://cmuir.cmu.ac.th/jspui/handle/6653943832/55915
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dc.contributor.authorT. Tunkasirien_US
dc.contributor.authorG. Rujijanagulen_US
dc.contributor.authorU. Intathaen_US
dc.contributor.authorK. Pengpaten_US
dc.contributor.authorK. Sutjarittangthamen_US
dc.contributor.authorS. Eitssayeamen_US
dc.date.accessioned2018-09-05T03:04:33Z-
dc.date.available2018-09-05T03:04:33Z-
dc.date.issued2016-09-25en_US
dc.identifier.issn15635112en_US
dc.identifier.issn00150193en_US
dc.identifier.other2-s2.0-84994299218en_US
dc.identifier.other10.1080/00150193.2016.1234910en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84994299218&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/55915-
dc.description.abstract© 2016 Taylor & Francis Group, LLC. The dielectric constants of PZT-polymer composites of the 0–3 connectivity employing the simple cube model (proposed by Pauer) showed considerable deviation between the theory to experimental observation. Banno modified the model by means of incorporating a geometric factor “n” into the model. However Banno selected the “n” value based on an attempt to match theory to experimental data. In this work we assume that the “n” value equal to the ratio of the Young modulus of the polymer to that of PZT and replace “n” by the ratio into the equation derived by Banno. Our expression compares very favorably with the sets of the experimental data for the PZT-polymer composites of the 0–3 connectivity.en_US
dc.subjectMaterials Scienceen_US
dc.subjectPhysics and Astronomyen_US
dc.titleModel for the dielectric constant for 0-3 piezoelectric-polymer compositesen_US
dc.typeJournalen_US
article.title.sourcetitleFerroelectricsen_US
article.volume502en_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsMae Fah Luang Universityen_US
article.stream.affiliationsPibulsongkram Rajabhat Universityen_US
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