Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis
Autor(a) principal: | |
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Data de Publicação: | 2007 |
Outros Autores: | |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UFBA |
Texto Completo: | http://www.repositorio.ufba.br/ri/handle/ufba/583 |
Resumo: | The well-known Vogel-Fulcher-Tammann-Hesse equation (VFTH, log10 eta = A+B/(T-T0), eta in Pa.s and T in K) has been extensively used in the description & characterization of cooperative molecular motion by means of the temperature dependence with viscosity, eta, e.g., using Angell's classification. Experimental evidence has been pointed out for the statistical correlation between its three adjustable parameters A, B and T0, which may bring questions on the reliability of fitted VFTH parameters. In this work VFTH equation was applied over a wide temperature range (between glass transition temperature, Tg and the melting point, Tm) for 38 oxide glasses, considering simple, binary and ternary compositions of silicates and borates systems. These systems include strong, moderate and fragile glass-forming liquids. For this task was used the Levenberg-Marquart non-linear fitting procedure to find viscosity parameters B and T0, maintaining A=-5 fixed, intending to reduce the number of adjustable parameters. Despite this restriction, the VFTH equation has shown to adjust very well to experimental data in wide temperature range. Simple criteria were developed in the past to characterize glass-forming liquids, one of them (due to Angell) is the strong-fragile classification. In this work we apply Correspondence Analysis (CA) to verify the correlation between B and T0 parameters as well as between Tg and Tm. CA is a descriptive and exploratory technique designed to analyze simple multi-way tables containing some measure of correspondence between rows and columns. From these results is possible to map either borate (and almost fragile) or silicate (usually strong up to near fragile) systems. As a statistical tool, CA corroborates correlation mainly between B and T0 and justifies the use of B, T0 and Tg as the main parameters for the fragility indexes m = BTg/(Tg-T0)^2 and D = B/T0. |
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Aparicio, CristinaNascimento, Marcio Luis FerreiraAparicio, CristinaNascimento, Marcio Luis Ferreira2010-11-10T20:02:29Z2010-11-10T20:02:29Z200709214526http://www.repositorio.ufba.br/ri/handle/ufba/583Physica. B, Condensed Matter, v. 398, p. 71-77The well-known Vogel-Fulcher-Tammann-Hesse equation (VFTH, log10 eta = A+B/(T-T0), eta in Pa.s and T in K) has been extensively used in the description & characterization of cooperative molecular motion by means of the temperature dependence with viscosity, eta, e.g., using Angell's classification. Experimental evidence has been pointed out for the statistical correlation between its three adjustable parameters A, B and T0, which may bring questions on the reliability of fitted VFTH parameters. In this work VFTH equation was applied over a wide temperature range (between glass transition temperature, Tg and the melting point, Tm) for 38 oxide glasses, considering simple, binary and ternary compositions of silicates and borates systems. These systems include strong, moderate and fragile glass-forming liquids. For this task was used the Levenberg-Marquart non-linear fitting procedure to find viscosity parameters B and T0, maintaining A=-5 fixed, intending to reduce the number of adjustable parameters. Despite this restriction, the VFTH equation has shown to adjust very well to experimental data in wide temperature range. Simple criteria were developed in the past to characterize glass-forming liquids, one of them (due to Angell) is the strong-fragile classification. In this work we apply Correspondence Analysis (CA) to verify the correlation between B and T0 parameters as well as between Tg and Tm. CA is a descriptive and exploratory technique designed to analyze simple multi-way tables containing some measure of correspondence between rows and columns. From these results is possible to map either borate (and almost fragile) or silicate (usually strong up to near fragile) systems. As a statistical tool, CA corroborates correlation mainly between B and T0 and justifies the use of B, T0 and Tg as the main parameters for the fragility indexes m = BTg/(Tg-T0)^2 and D = B/T0.Submitted by Marcio Luis Ferreira Nascimento (mlfn@ufba.br) on 2010-11-10T20:02:29Z No. of bitstreams: 1 DataClassificationVFTH-CA-PB398-Nascimento.pdf: 701456 bytes, checksum: 87d241b6228f62ac6ff93cd0f5859213 (MD5)Made available in DSpace on 2010-11-10T20:02:29Z (GMT). No. of bitstreams: 1 DataClassificationVFTH-CA-PB398-Nascimento.pdf: 701456 bytes, checksum: 87d241b6228f62ac6ff93cd0f5859213 (MD5) Previous issue date: 2007Estados UnidosVidroViscosidadeComponente PrincipalModeloVogel-Fulcher-Tammann-HesseData classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysisArtigo de Periódicoinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionengreponame:Repositório Institucional da UFBAinstname:Universidade Federal da Bahia (UFBA)instacron:UFBAinfo:eu-repo/semantics/openAccessORIGINALDataClassificationVFTH-CA-PB398-Nascimento.pdfDataClassificationVFTH-CA-PB398-Nascimento.pdfapplication/pdf701456https://repositorio.ufba.br/bitstream/ufba/583/1/DataClassificationVFTH-CA-PB398-Nascimento.pdf87d241b6228f62ac6ff93cd0f5859213MD51LICENSElicense.txtlicense.txttext/plain1908https://repositorio.ufba.br/bitstream/ufba/583/2/license.txt26dabefb0239a887bfdfe5baaad6280aMD52TEXTDataClassificationVFTH-CA-PB398-Nascimento.pdf.txtDataClassificationVFTH-CA-PB398-Nascimento.pdf.txtExtracted texttext/plain27461https://repositorio.ufba.br/bitstream/ufba/583/3/DataClassificationVFTH-CA-PB398-Nascimento.pdf.txt8fa8eb5cbdc97527acae8e220ca557baMD53ufba/5832022-08-26 11:47:05.988oai:repositorio.ufba.br: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ório InstitucionalPUBhttp://192.188.11.11:8080/oai/requestopendoar:19322022-08-26T14:47:05Repositório Institucional da UFBA - Universidade Federal da Bahia (UFBA)false |
dc.title.en.fl_str_mv |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
title |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
spellingShingle |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis Aparicio, Cristina Vidro Viscosidade Componente Principal Modelo Vogel-Fulcher-Tammann-Hesse |
title_short |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
title_full |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
title_fullStr |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
title_full_unstemmed |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
title_sort |
Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis |
author |
Aparicio, Cristina |
author_facet |
Aparicio, Cristina Nascimento, Marcio Luis Ferreira |
author_role |
author |
author2 |
Nascimento, Marcio Luis Ferreira |
author2_role |
author |
dc.contributor.author.fl_str_mv |
Aparicio, Cristina Nascimento, Marcio Luis Ferreira Aparicio, Cristina Nascimento, Marcio Luis Ferreira |
dc.subject.eng.fl_str_mv |
Vidro Viscosidade Componente Principal Modelo Vogel-Fulcher-Tammann-Hesse |
topic |
Vidro Viscosidade Componente Principal Modelo Vogel-Fulcher-Tammann-Hesse |
description |
The well-known Vogel-Fulcher-Tammann-Hesse equation (VFTH, log10 eta = A+B/(T-T0), eta in Pa.s and T in K) has been extensively used in the description & characterization of cooperative molecular motion by means of the temperature dependence with viscosity, eta, e.g., using Angell's classification. Experimental evidence has been pointed out for the statistical correlation between its three adjustable parameters A, B and T0, which may bring questions on the reliability of fitted VFTH parameters. In this work VFTH equation was applied over a wide temperature range (between glass transition temperature, Tg and the melting point, Tm) for 38 oxide glasses, considering simple, binary and ternary compositions of silicates and borates systems. These systems include strong, moderate and fragile glass-forming liquids. For this task was used the Levenberg-Marquart non-linear fitting procedure to find viscosity parameters B and T0, maintaining A=-5 fixed, intending to reduce the number of adjustable parameters. Despite this restriction, the VFTH equation has shown to adjust very well to experimental data in wide temperature range. Simple criteria were developed in the past to characterize glass-forming liquids, one of them (due to Angell) is the strong-fragile classification. In this work we apply Correspondence Analysis (CA) to verify the correlation between B and T0 parameters as well as between Tg and Tm. CA is a descriptive and exploratory technique designed to analyze simple multi-way tables containing some measure of correspondence between rows and columns. From these results is possible to map either borate (and almost fragile) or silicate (usually strong up to near fragile) systems. As a statistical tool, CA corroborates correlation mainly between B and T0 and justifies the use of B, T0 and Tg as the main parameters for the fragility indexes m = BTg/(Tg-T0)^2 and D = B/T0. |
publishDate |
2007 |
dc.date.issued.fl_str_mv |
2007 |
dc.date.accessioned.fl_str_mv |
2010-11-10T20:02:29Z |
dc.date.available.fl_str_mv |
2010-11-10T20:02:29Z |
dc.type.driver.fl_str_mv |
Artigo de Periódico info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://www.repositorio.ufba.br/ri/handle/ufba/583 |
dc.identifier.issn.none.fl_str_mv |
09214526 |
dc.identifier.number.en.fl_str_mv |
Physica. B, Condensed Matter, v. 398, p. 71-77 |
identifier_str_mv |
09214526 Physica. B, Condensed Matter, v. 398, p. 71-77 |
url |
http://www.repositorio.ufba.br/ri/handle/ufba/583 |
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eng |
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UFBA |
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