Data classification with the Vogel Fulcher Tammann Hesse viscosity equation using correspondence analysis

Detalhes bibliográficos
Autor(a) principal: Aparicio, Cristina
Data de Publicação: 2007
Outros Autores: Nascimento, Marcio Luis Ferreira
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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spelling 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
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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
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