Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5
| Ano de defesa: | 2016 |
|---|---|
| Autor(a) principal: | |
| Orientador(a): | |
| Banca de defesa: | |
| Tipo de documento: | Dissertação |
| Tipo de acesso: | Acesso aberto |
| Idioma: | por |
| Instituição de defesa: |
Universidade Federal de São Carlos
Câmpus São Carlos |
| Programa de Pós-Graduação: |
Programa de Pós-Graduação em Ciência e Engenharia de Materiais - PPGCEM
|
| Departamento: |
Não Informado pela instituição
|
| País: |
Não Informado pela instituição
|
| Palavras-chave em Português: | |
| Área do conhecimento CNPq: | |
| Link de acesso: | https://repositorio.ufscar.br/handle/20.500.14289/8478 |
Resumo: | Mixed conductive glassy materials have in their composition, in addition to a glass former, a metallic element in two oxidation states and ions with high mobility, generally alkaline or Ag+ ions. These materials can be used in solid state batteries. However, from a scientific point of view, there are still some issues to be solved, such as the mechanism that best explains the behavior of electric conduction in these materials, and why there is a marked drop in conductivity as a function of composition, for equimolar compositions between the modifier that introduces the ionic conduction, and the transition metal oxide that introduces the electronic conduction. Therefore, to advance the frontier of knowledge about the conduction mechanisms present in mixed conductive glasses, the ternary system of the glass family 0.50[xAg2O(1-x)V2O5].0.50P2O5, (0 ≤ x ≤ 1) was chosen. Each vitreous composition was synthesized and characterized by X-ray diffraction, differential scanning calorimetry, Helium pycnometry, and impedance spectroscopy. The impedance spectroscopy measurements of the composition x=0.6 revealed a semicircle with a deformation at low frequency. This semicircle cannot be adjusted by a single RC circuit. The analysis of the pre-exponential factor and the activation energies of the glasses shows lower values for the glasses rich in vanadium, that is, in the "electronic" region, when compared to the pre-exponential factor of the glasses of the region richest in silver, or in the "ionic" region. This behavior is in accordance with the theoretical expressions for each of the conductivity mechanisms. In an attempt to quantify the ionic and electronic contributions, the electromotive force method (F.E.M) was applied. This method was selected because, theoretically, it allows a precise quantification of the electronic and ionic conductivities. However, the experimental results showed that the generated electrochemical cell did not correspond to the expected one, therefore it was not possible to quantify the ionic and electronic contributions to the total electrical conductivity. |
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Diaz Marin, Juan JairoRodrigues, Ana Candida Martinshttp://lattes.cnpq.br/4499231813051400http://lattes.cnpq.br/38372985861230613ddebda1-543d-4042-a0be-b7ce5ce15ad92017-02-07T15:21:29Z2017-02-07T15:21:29Z2016-10-27DIAZ MARIN, Juan Jairo. Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5. 2016. Dissertação (Mestrado em Ciência e Engenharia de Materiais) – Universidade Federal de São Carlos, São Carlos, 2016. Disponível em: https://repositorio.ufscar.br/handle/20.500.14289/8478.https://repositorio.ufscar.br/handle/20.500.14289/8478Mixed conductive glassy materials have in their composition, in addition to a glass former, a metallic element in two oxidation states and ions with high mobility, generally alkaline or Ag+ ions. These materials can be used in solid state batteries. However, from a scientific point of view, there are still some issues to be solved, such as the mechanism that best explains the behavior of electric conduction in these materials, and why there is a marked drop in conductivity as a function of composition, for equimolar compositions between the modifier that introduces the ionic conduction, and the transition metal oxide that introduces the electronic conduction. Therefore, to advance the frontier of knowledge about the conduction mechanisms present in mixed conductive glasses, the ternary system of the glass family 0.50[xAg2O(1-x)V2O5].0.50P2O5, (0 ≤ x ≤ 1) was chosen. Each vitreous composition was synthesized and characterized by X-ray diffraction, differential scanning calorimetry, Helium pycnometry, and impedance spectroscopy. The impedance spectroscopy measurements of the composition x=0.6 revealed a semicircle with a deformation at low frequency. This semicircle cannot be adjusted by a single RC circuit. The analysis of the pre-exponential factor and the activation energies of the glasses shows lower values for the glasses rich in vanadium, that is, in the "electronic" region, when compared to the pre-exponential factor of the glasses of the region richest in silver, or in the "ionic" region. This behavior is in accordance with the theoretical expressions for each of the conductivity mechanisms. In an attempt to quantify the ionic and electronic contributions, the electromotive force method (F.E.M) was applied. This method was selected because, theoretically, it allows a precise quantification of the electronic and ionic conductivities. However, the experimental results showed that the generated electrochemical cell did not correspond to the expected one, therefore it was not possible to quantify the ionic and electronic contributions to the total electrical conductivity.Materiais vítreos condutores mistos apresentam em sua composição, além de um formador de vidro, um elemento metálico em dois estados de oxidação e íons com alta mobilidade, em geral íons alcalinos ou Ag+. Esses materiais podem ser utilizados em baterias de estado sólido. Porém, de um ponto de vista cientifico, ainda existem algumas questões a serem resolvidas, como por exemplo, qual é o mecanismo que melhor explica o comportamento da condução elétrica nestes materiais, e por que ocorre uma queda acentuada da condutividade em função da composição, geralmente para composições equimolares entre o modificador que introduz a condução iônica, e o óxido de metal de transição que introduz a condução eletrônica. Portanto, para avançar na fronteira do conhecimento sobre os mecanismo de condução presentes em vidros condutores mistos, foi escolhido o sistema ternário da família de vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5, (0 ≤ x ≤ 1). Cada composição vítrea foi sintetizada e caracterizada por difração de raios X (DRX), calorimetria diferencial de varredura (DSC), picnometria com Hélio, e espectroscopia de impedância. As medidas de espectroscopia de impedância da composição x=0,6 revelaram um semicírculo com uma deformação em baixas frequências. Este semicírculo não pode ser ajustado por um circuito RC simples. A análise do fator pré-exponencial e das energias de ativação dos vidros mostra valores menores para os vidros ricos em vanádio, isto é, na região “eletrônica”, quando comparados ao fator pré-exponencial dos vidros da região mais rica em prata, ou seja, na região “iônica”. Este comportamento está de acordo com as expressões teóricas para cada um dos mecanismos de condutividade. Na tentativa de se quantificar as contribuições iônicas e eletrônicas, foi aplicado o método da força eletromotriz (F.E.M). Este método foi selecionado por, teoricamente, permitir uma quantificação precisa das condutividades eletrônicas e iônicas. No entanto, os resultados experimentais mostraram que a célula eletroquímica gerada não correspondeu ao esperado, portanto, não foi possível fazer uma quantificação das contribuições iônica e eletrônica à condutividade elétrica total.Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES)porUniversidade Federal de São CarlosCâmpus São CarlosPrograma de Pós-Graduação em Ciência e Engenharia de Materiais - PPGCEMUFSCarMateriais vítreosCondutividade mistaENGENHARIAS::ENGENHARIA DE MATERIAIS E METALURGICA::MATERIAIS NAO METALICOSCondutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/masterThesisOnline600600901b2e03-1fc6-4525-8d1a-d61ea51a9dc4info:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFSCARinstname:Universidade Federal de São Carlos (UFSCAR)instacron:UFSCARORIGINALDissJJDM.pdfDissJJDM.pdfapplication/pdf2138364https://repositorio.ufscar.br/bitstreams/e820e41d-a04c-4967-96e5-645f4829ebaf/download81a3b370c5733bc609efb97a1674e0e5MD51trueAnonymousREADLICENSElicense.txtlicense.txttext/plain; charset=utf-81957https://repositorio.ufscar.br/bitstreams/19894f2e-11d7-4954-bd33-ecca1f9923be/downloadae0398b6f8b235e40ad82cba6c50031dMD52falseAnonymousREADTEXTDissJJDM.pdf.txtDissJJDM.pdf.txtExtracted texttext/plain157489https://repositorio.ufscar.br/bitstreams/11ec02df-1752-4b3f-85a0-7e1e536621fa/downloadfbc31423b5a29b8bfc2f7c141d78d28bMD55falseAnonymousREADTHUMBNAILDissJJDM.pdf.jpgDissJJDM.pdf.jpgIM Thumbnailimage/jpeg3403https://repositorio.ufscar.br/bitstreams/536e3a9a-16cb-4612-b60e-1c5bef6393db/downloaddcdc4096769c1e9970abacd7d37fb593MD56falseAnonymousREAD20.500.14289/84782025-02-05 17:29:50.926Acesso abertoopen.accessoai:repositorio.ufscar.br:20.500.14289/8478https://repositorio.ufscar.brRepositório InstitucionalPUBhttps://repositorio.ufscar.br/oai/requestrepositorio.sibi@ufscar.bropendoar:43222025-02-05T20:29:50Repositório Institucional da UFSCAR - Universidade Federal de São Carlos (UFSCAR)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 |
| dc.title.por.fl_str_mv |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| title |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| spellingShingle |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 Diaz Marin, Juan Jairo Materiais vítreos Condutividade mista ENGENHARIAS::ENGENHARIA DE MATERIAIS E METALURGICA::MATERIAIS NAO METALICOS |
| title_short |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| title_full |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| title_fullStr |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| title_full_unstemmed |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| title_sort |
Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5 |
| author |
Diaz Marin, Juan Jairo |
| author_facet |
Diaz Marin, Juan Jairo |
| author_role |
author |
| dc.contributor.authorlattes.por.fl_str_mv |
http://lattes.cnpq.br/3837298586123061 |
| dc.contributor.author.fl_str_mv |
Diaz Marin, Juan Jairo |
| dc.contributor.advisor1.fl_str_mv |
Rodrigues, Ana Candida Martins |
| dc.contributor.advisor1Lattes.fl_str_mv |
http://lattes.cnpq.br/4499231813051400 |
| dc.contributor.authorID.fl_str_mv |
3ddebda1-543d-4042-a0be-b7ce5ce15ad9 |
| contributor_str_mv |
Rodrigues, Ana Candida Martins |
| dc.subject.por.fl_str_mv |
Materiais vítreos Condutividade mista |
| topic |
Materiais vítreos Condutividade mista ENGENHARIAS::ENGENHARIA DE MATERIAIS E METALURGICA::MATERIAIS NAO METALICOS |
| dc.subject.cnpq.fl_str_mv |
ENGENHARIAS::ENGENHARIA DE MATERIAIS E METALURGICA::MATERIAIS NAO METALICOS |
| description |
Mixed conductive glassy materials have in their composition, in addition to a glass former, a metallic element in two oxidation states and ions with high mobility, generally alkaline or Ag+ ions. These materials can be used in solid state batteries. However, from a scientific point of view, there are still some issues to be solved, such as the mechanism that best explains the behavior of electric conduction in these materials, and why there is a marked drop in conductivity as a function of composition, for equimolar compositions between the modifier that introduces the ionic conduction, and the transition metal oxide that introduces the electronic conduction. Therefore, to advance the frontier of knowledge about the conduction mechanisms present in mixed conductive glasses, the ternary system of the glass family 0.50[xAg2O(1-x)V2O5].0.50P2O5, (0 ≤ x ≤ 1) was chosen. Each vitreous composition was synthesized and characterized by X-ray diffraction, differential scanning calorimetry, Helium pycnometry, and impedance spectroscopy. The impedance spectroscopy measurements of the composition x=0.6 revealed a semicircle with a deformation at low frequency. This semicircle cannot be adjusted by a single RC circuit. The analysis of the pre-exponential factor and the activation energies of the glasses shows lower values for the glasses rich in vanadium, that is, in the "electronic" region, when compared to the pre-exponential factor of the glasses of the region richest in silver, or in the "ionic" region. This behavior is in accordance with the theoretical expressions for each of the conductivity mechanisms. In an attempt to quantify the ionic and electronic contributions, the electromotive force method (F.E.M) was applied. This method was selected because, theoretically, it allows a precise quantification of the electronic and ionic conductivities. However, the experimental results showed that the generated electrochemical cell did not correspond to the expected one, therefore it was not possible to quantify the ionic and electronic contributions to the total electrical conductivity. |
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2016 |
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2016-10-27 |
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2017-02-07T15:21:29Z |
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2017-02-07T15:21:29Z |
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DIAZ MARIN, Juan Jairo. Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5. 2016. Dissertação (Mestrado em Ciência e Engenharia de Materiais) – Universidade Federal de São Carlos, São Carlos, 2016. Disponível em: https://repositorio.ufscar.br/handle/20.500.14289/8478. |
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https://repositorio.ufscar.br/handle/20.500.14289/8478 |
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DIAZ MARIN, Juan Jairo. Condutividade iônica e eletrônica em vidros 0,50[xAg2O(1-x)V2O5].0,50P2O5. 2016. Dissertação (Mestrado em Ciência e Engenharia de Materiais) – Universidade Federal de São Carlos, São Carlos, 2016. Disponível em: https://repositorio.ufscar.br/handle/20.500.14289/8478. |
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Universidade Federal de São Carlos Câmpus São Carlos |
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Universidade Federal de São Carlos Câmpus São Carlos |
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