New method for depth analysis of Y-TZP t-m phase transformation

dc.contributor.authorARATA, A.
dc.contributor.authorPRETTO, L.R. de
dc.contributor.authorUSSUI, V.
dc.contributor.authorLIMA, N.B.
dc.contributor.authorFREITAS, A.Z.
dc.contributor.authorMACHADO, J.P.B.
dc.contributor.authorTANGO, R.N.
dc.contributor.authorSOUZA, G.M. de
dc.contributor.authorLAZAR, D.R.R.
dc.coverageInternacionalpt_BR
dc.date.accessioned2018-03-06T11:18:47Z
dc.date.available2018-03-06T11:18:47Z
dc.date.issued2017pt_BR
dc.description.abstractPurpose/aim: The aim of this studywas to validate the optical coherence tomography (OCT) as a nondestructive method of analysis to evaluate the depth of tetragonal to monoclinic (t-m) transformed zone and to calculate the kinetics of phase transformation of a monolithic Y-TZP after hydrothermal aging. Specifically, to compare the activation energy of t-m transformation calculated by the depth of the transformed zone using scanning electron microscopy (SEM) and OCT. Materials and methods: Fully sintered (1450 ◦C/2 h) discs of dentalY-TZP (LAVAPLUS, 3M-ESPE)were aged in hydrothermal pressurized reactor to follow the phase transformation kinetics at 120 to 150 ◦C. Four samples per aging time were analyzed by OCT (OCP930SR, Thorlabs Inc.), = 930 nm, spectral bandwidth (FWHM) of 100 nm, nominal resolution of 6 m (lateral and axial) in air, declared digital resolution 3.09 m (axial). Three areas of 3mm (lateral) were observed to calculate the phase transformation depth (Image J). X-ray diffraction analysis (XRD) were performed, Cu-K , 20◦ to 80◦, 2 . The data were refined using the Rietveld method (GSAS). The transversal section of one specimen of each group was submitted to backscattered SEM analysis to calculate the phase transformation depth (Image J). The speed of the transformation zone front was determined plotting the phase transformation depth versus aging time. Results: XRD results indicated that Y-TZP that 66% is the maximum value of monoclinic phase concentration for all aged Y-TZP. The activation energy for the monolithic Y-TZP was 107.53 kJ/mol. One year and 5 years of hydrothermal aging at 37 ◦C will present approximately 4.21% and 15% of monoclinic phase, respectively. The comparison of the depth of the transformed zone using SEM and OCT were similar, showing a linear behavior and providing information that the opaque layer observed by OCT is related to the depth of the transformed zone (Fig. 1), any difference among the results could be a result of the refraction index correction. The energy of activation calculated by SEM and OCT were 114 kJ/mol and 100 kJ/mol, respectively. The speed calculated for the phase transformation into the bulk of the transformed zone estimated for 37 ◦C was 0.04 m/year (SEM) and 0.16 m/year (OCT). Conclusions: The results indicate that activation energy values determined by SEM and OCT observations were similar allowing the use of the OCT as a tool for monolithic Y-TZP t-m phase transformation kinetic evaluation. Moreover, OCT method has the advantage of a shorter analysis time, without the need of sample preparation steps.pt_BR
dc.format.extente6-e6pt_BR
dc.identifier.citationARATA, A.; PRETTO, L.R. de; USSUI, V.; LIMA, N.B.; FREITAS, A.Z.; MACHADO, J.P.B.; TANGO, R.N.; SOUZA, G.M. de; LAZAR, D.R.R. New method for depth analysis of Y-TZP t-m phase transformation. <b>Dental Materials</b>, v. 33, p. e6-e6, 2017. suppl. 1. DOI: <a href="https://dx.doi.org/10.1016/j.dental.2017.08.009">10.1016/j.dental.2017.08.009</a>. Disponível em: http://repositorio.ipen.br/handle/123456789/28641.
dc.identifier.doi10.1016/j.dental.2017.08.009pt_BR
dc.identifier.issn0109-5641pt_BR
dc.identifier.orcidhttps://orcid.org/0000-0001-7384-304X
dc.identifier.orcidhttps://orcid.org/0000-0002-5018-9126
dc.identifier.orcidhttps://orcid.org/0000-0002-6444-9224
dc.identifier.suplementosuppl. 1pt_BR
dc.identifier.urihttp://repositorio.ipen.br/handle/123456789/28641
dc.identifier.vol33pt_BR
dc.relation.ispartofDental Materialspt_BR
dc.rightsopenAccesspt_BR
dc.subjectcrystal-phase transformations
dc.subjecttomography
dc.subjectoptical modes
dc.subjectcoherence length
dc.subjectscanning electron microscopy
dc.subjectmeasuring methods
dc.titleNew method for depth analysis of Y-TZP t-m phase transformationpt_BR
dc.typeResumos em periódicospt_BR
dspace.entity.typePublication
ipen.autorDOLORES RIBEIRO RICCI LAZAR
ipen.autorANDERSON ZANARDI DE FREITAS
ipen.autorNELSON BATISTA DE LIMA
ipen.autorVALTER USSUI
ipen.autorLUCAS RAMOS DE PRETTO
ipen.autorANELYSE ARATA
ipen.codigoautor240
ipen.codigoautor880
ipen.codigoautor550
ipen.codigoautor191
ipen.codigoautor11268
ipen.codigoautor11273
ipen.contributor.ipenauthorDOLORES RIBEIRO RICCI LAZAR
ipen.contributor.ipenauthorANDERSON ZANARDI DE FREITAS
ipen.contributor.ipenauthorNELSON BATISTA DE LIMA
ipen.contributor.ipenauthorVALTER USSUI
ipen.contributor.ipenauthorLUCAS RAMOS DE PRETTO
ipen.contributor.ipenauthorANELYSE ARATA
ipen.date.recebimento18-03pt_BR
ipen.identifier.fi4.070pt_BR
ipen.identifier.ipendoc24482pt_BR
ipen.identifier.iwosAguardar WoSpt_BR
ipen.range.fi3.000 - 4.499
ipen.type.genreResumo
relation.isAuthorOfPublicatione2f75c76-2269-40cf-b463-bc5207084c5f
relation.isAuthorOfPublicationa8d821f0-a0a4-4d52-b582-5c5d0afce8f5
relation.isAuthorOfPublication92984f2d-b6bd-4cd9-950a-e1105bf78d83
relation.isAuthorOfPublication1cce9f1b-6fcb-4537-8c18-841807a33b68
relation.isAuthorOfPublication64a32d36-2971-45c5-a8a3-c266b2ed3e42
relation.isAuthorOfPublicationf948e8e6-da7c-4c8c-8f76-dc2d73382f3c
relation.isAuthorOfPublication.latestForDiscoveryf948e8e6-da7c-4c8c-8f76-dc2d73382f3c
sigepi.autor.atividadeARATA, A.:11273:720:Spt_BR
sigepi.autor.atividadePRETTO, L.R. de:11268:920:Npt_BR
sigepi.autor.atividadeUSSUI, V.:191:720:Npt_BR
sigepi.autor.atividadeLIMA, N.B.:550:730:Npt_BR
sigepi.autor.atividadeFREITAS, A.Z.:880:920:Npt_BR
sigepi.autor.atividadeLAZAR, D.R.R.:240:720:Npt_BR

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