PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).

Detalhes bibliográficos
Autor(a) principal: ARAÚJO, Ronaldo Andrade de
Data de Publicação: 2019
Tipo de documento: Dissertação
Idioma: por
Título da fonte: Biblioteca Digital de Teses e Dissertações da UFMA
Texto Completo: https://tedebc.ufma.br/jspui/handle/tede/tede/2965
Resumo: Structural, magnetic and magnetocaloric properties of the RNiGe3 (R = Pr, Nd, Eu, Dy, Ho and Er) compounds were studied. The samples were synthesized by arc melting technique under argon atmosphere. X-ray diffraction (XRD) measurements and analysis by using the Rietveld method confirm the desired crystallographic phase for all studied samples. Magnetization data shows antiferromagnetic ordering for RNiGe3 compounds, with Néel temperature (TN) around 21 K, 12.5 K, 14 K, 21 K, 9 K and 6 K for R = Pr, Nd, Eu, Dy, Ho and Er, respectively. For T<TN, the compounds NdNiGe3 and EuNiGe3 present an additional transition around 6.1 K and 5 K, respectively, while PrNiGe3 presents two additional transitions around 18.5 and 15.5 K. External magnetic field application induces metamagnetic phase transitions from antiferromagnetic to ferromagnetic state. However, the observed values of the magnetic moments in high magnetic field (H= 60 and 90 kOe) and low temperatures (T = 2 K) are reduced compared to the respective free ions. The metamagnetic critical magnetic field (HC) occurs around 16 kOe, 17.3 kOe, 26.5 kOe, 10.5 kOe and 9.5 kOe, for R = Pr, Nd, Dy, Ho and Er, respectively, and around 20 and 28 kOe for R=Eu. Magnetocaloric effect (MCE) of studies compounds was evaluated by means of the isothermal magnetic entropy change (-ΔSM), in which a broad peak in -ΔSM curve associated with the magnetic transition was observed. In addition, negative MCE was observed for all samples (in ΔH < HC) due to antiferromagnetic ordering. Among the studies compounds, the highest value of -ΔSM was observed for HoNiGe3. The maximum values of -ΔSM (−𝛥𝑆𝑀𝑚𝑎𝑥) and relative cooling power (RCP) observed for RNiGe3 series were respectively, 6.1 J/kg.K and 72.9 J/kg, 4.2 J/kg.K and 68.2 J/kg, 7.5 J/kg.K and 113.6 J/kg, 5.0 J/kg.K and 106 J/kg, 16.7 J/kg.K and 308.5 J/kg, and 11.3 J/kg.K and 214.7 J/kg, for R = Pr, Nd, Eu, Dy, Ho and Er, in ΔH = 50 kOe. These values are comparable to those reported in the literature for other magnetocaloric compounds, in the same temperature range. The obtained results indicate that the RNiGe3 compounds presented interesting magnetocaloric properties for application in magnetic refrigeration at cryogenic temperatures.
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spelling SILVA, Luzeli Moreira da438.074.022-68http://lattes.cnpq.br/5651616479126344SILVA, Luzeli Moreira da438.074.022-68http://lattes.cnpq.br/5651616479126344SANTOS, Adenilson Oliveira doshttp://lattes.cnpq.br/7760219759813661SILVA, Leonardo de Sousa056.750.023-32http://lattes.cnpq.br/3515712441056475ARAÚJO, Ronaldo Andrade de2020-01-08T13:50:49Z2019-07-08ARAÚJO, Ronaldo Andrade de. Propriedades magnéticas e magnetocalóricas do sistema RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).. 2019. 83 f. Dissertação( Programa de Pós-Graduação em Ciência dos Materiais/CCSST) - Universidade Federal do Maranhão, Imperatriz, 2019.https://tedebc.ufma.br/jspui/handle/tede/tede/2965Structural, magnetic and magnetocaloric properties of the RNiGe3 (R = Pr, Nd, Eu, Dy, Ho and Er) compounds were studied. The samples were synthesized by arc melting technique under argon atmosphere. X-ray diffraction (XRD) measurements and analysis by using the Rietveld method confirm the desired crystallographic phase for all studied samples. Magnetization data shows antiferromagnetic ordering for RNiGe3 compounds, with Néel temperature (TN) around 21 K, 12.5 K, 14 K, 21 K, 9 K and 6 K for R = Pr, Nd, Eu, Dy, Ho and Er, respectively. For T<TN, the compounds NdNiGe3 and EuNiGe3 present an additional transition around 6.1 K and 5 K, respectively, while PrNiGe3 presents two additional transitions around 18.5 and 15.5 K. External magnetic field application induces metamagnetic phase transitions from antiferromagnetic to ferromagnetic state. However, the observed values of the magnetic moments in high magnetic field (H= 60 and 90 kOe) and low temperatures (T = 2 K) are reduced compared to the respective free ions. The metamagnetic critical magnetic field (HC) occurs around 16 kOe, 17.3 kOe, 26.5 kOe, 10.5 kOe and 9.5 kOe, for R = Pr, Nd, Dy, Ho and Er, respectively, and around 20 and 28 kOe for R=Eu. Magnetocaloric effect (MCE) of studies compounds was evaluated by means of the isothermal magnetic entropy change (-ΔSM), in which a broad peak in -ΔSM curve associated with the magnetic transition was observed. In addition, negative MCE was observed for all samples (in ΔH < HC) due to antiferromagnetic ordering. Among the studies compounds, the highest value of -ΔSM was observed for HoNiGe3. The maximum values of -ΔSM (−𝛥𝑆𝑀𝑚𝑎𝑥) and relative cooling power (RCP) observed for RNiGe3 series were respectively, 6.1 J/kg.K and 72.9 J/kg, 4.2 J/kg.K and 68.2 J/kg, 7.5 J/kg.K and 113.6 J/kg, 5.0 J/kg.K and 106 J/kg, 16.7 J/kg.K and 308.5 J/kg, and 11.3 J/kg.K and 214.7 J/kg, for R = Pr, Nd, Eu, Dy, Ho and Er, in ΔH = 50 kOe. These values are comparable to those reported in the literature for other magnetocaloric compounds, in the same temperature range. The obtained results indicate that the RNiGe3 compounds presented interesting magnetocaloric properties for application in magnetic refrigeration at cryogenic temperatures.Neste trabalho foi realizado um estudo das propriedades estruturais, magnéticas e magnetocalóricas dos compostos da série RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er). As amostras foram sintetizadas via fusão em forno à arco voltaico, sob atmosfera de argônio. Medidas de difração de Raios X e a análise pelo método de Rietveld confirmaram que todas as amostras apresentaram a fase cristalográfica desejada. Medidas de magnetização mostraram que esses compostos apresentam ordenamento antiferromagnético com temperatura de Néel (TN) em torno de 21 K, 12,5 K, 14 K, 21 K, 9 K e 6 K, para R = Pr, Nd, Eu, Dy, Ho e Er, respectivamente. Uma transição adicional em T = 6,1 K e 5 K, foi observada para R = Nd e Eu, respectivamente. Já o composto PrNiGe3 apresenta duas transições adicionais (18,5 K, 15,5 K) em T < TN. A aplicação de campo magnético externo induz transição metamagnética em todos os compostos em estudo, porém em altos campos magnéticos os valores dos momentos magnéticos em T = 2 K estão reduzidos comparando-se com os respectivos íons livres. O campo crítico da transição metamagnética (HC) ocorre em 16 kOe, 17,3 kOe, 26,5 kOe, 10,5 kOe e 9,5 kOe, para R = Pr, Nd, Dy, Ho e Er, respectivamente e de 20 e 28 kOe para R=Eu. A magnitude do efeito magnetocalórico (EMC) dos compostos foi avaliada por meio da variação isotérmica da entropia magnética (-ΔSM), tendo sido caracterizado por um pico alargado nas curvas de -ΔSM associado com a transição magnética. EMC negativo foi observado para todas as amostras (em ΔH < HC), devido ao ordenamento antiferromagnético. O composto HoNiGe3 mostrou variação de entropia isotérmica mais intensa quando comparada aos outros compostos deste estudo. Os valores máximos da -ΔSM (−𝛥𝑆𝑀𝑚𝑎𝑥) e poder de resfriamento relativo (RCP) obtidos para a série RNiGe3 foram, respectivamente, 6,1 J/kg.K e 72,9 J/kg, 4,2 J/kg.K e 68,2 J/kg, 7,5 J/kg.K e 113,6 J/kg, 5,0 J/kg.K e 106 J/kg, 16,7 J/kg.K e 308,5 J/kg, e 11,3 J/kg.K e 214,7 J/kg, para R = Pr, Nd, Eu, Dy, Ho e Er, em ΔH = 50 kOe. Estes valores são comparáveis aos relatados na literatura para outros compostos magnetocalóricos, na mesma faixa de temperatura. Os resultados obtidos indicam que os compostos RNiGe3 apresentam propriedades magnetocalóricas interessantes para aplicação na refrigeração magnética em temperaturas criogênicas.Submitted by Maria Aparecida (cidazen@gmail.com) on 2020-01-08T13:50:49Z No. of bitstreams: 1 Ronaldo A. de Araújo.pdf: 6235294 bytes, checksum: c28695f18e10477daefcb82d5b93b26e (MD5)Made available in DSpace on 2020-01-08T13:50:49Z (GMT). No. of bitstreams: 1 Ronaldo A. de Araújo.pdf: 6235294 bytes, checksum: c28695f18e10477daefcb82d5b93b26e (MD5) Previous issue date: 2019-07-08CNPqFAPEMACAPESapplication/pdfporUniversidade Federal do MaranhãoPROGRAMA DE PÓS-GRADUAÇÃO EM CIÊNCIA DOS MATERIAIS/CCSSTUFMABrasilCOORDENAÇÃO DO CURSO ENGENHARIA DE ALIMENTOS/CCSSTCompostos intermetálicos;Propriedades magnéticas;Efeito magnetocalóricoIntermetallic compounds;Magnetic properties;Magnetocaloric effectEstrutura de Líquidos e Sólidos; CristalografiaPROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).MAGNETIC AND MAGNETHOCALORIC PROPERTIES OF THE RNiGe3 SYSTEM (R = Pr, Nd, I, Dy, Ho and Er).info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/masterThesisinfo:eu-repo/semantics/openAccessreponame:Biblioteca Digital de Teses e Dissertações da UFMAinstname:Universidade Federal do Maranhão (UFMA)instacron:UFMAORIGINALRonaldo A. de Araújo.pdfRonaldo A. de Araújo.pdfapplication/pdf6235294http://tedebc.ufma.br:8080/bitstream/tede/2965/2/Ronaldo+A.+de+Ara%C3%BAjo.pdfc28695f18e10477daefcb82d5b93b26eMD52LICENSElicense.txtlicense.txttext/plain; charset=utf-82255http://tedebc.ufma.br:8080/bitstream/tede/2965/1/license.txt97eeade1fce43278e63fe063657f8083MD51tede/29652020-01-08 10:50:49.974oai:tede2: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Biblioteca Digital de Teses e Dissertaçõeshttps://tedebc.ufma.br/jspui/PUBhttp://tedebc.ufma.br:8080/oai/requestrepositorio@ufma.br||repositorio@ufma.bropendoar:21312020-01-08T13:50:49Biblioteca Digital de Teses e Dissertações da UFMA - Universidade Federal do Maranhão (UFMA)false
dc.title.por.fl_str_mv PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
dc.title.alternative.eng.fl_str_mv MAGNETIC AND MAGNETHOCALORIC PROPERTIES OF THE RNiGe3 SYSTEM (R = Pr, Nd, I, Dy, Ho and Er).
title PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
spellingShingle PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
ARAÚJO, Ronaldo Andrade de
Compostos intermetálicos;
Propriedades magnéticas;
Efeito magnetocalórico
Intermetallic compounds;
Magnetic properties;
Magnetocaloric effect
Estrutura de Líquidos e Sólidos; Cristalografia
title_short PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
title_full PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
title_fullStr PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
title_full_unstemmed PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
title_sort PROPRIEDADES MAGNÉTICAS E MAGNETOCALÓRICAS DO SISTEMA RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).
author ARAÚJO, Ronaldo Andrade de
author_facet ARAÚJO, Ronaldo Andrade de
author_role author
dc.contributor.advisor1.fl_str_mv SILVA, Luzeli Moreira da
dc.contributor.advisor1ID.fl_str_mv 438.074.022-68
dc.contributor.advisor1Lattes.fl_str_mv http://lattes.cnpq.br/5651616479126344
dc.contributor.referee1.fl_str_mv SILVA, Luzeli Moreira da
dc.contributor.referee1ID.fl_str_mv 438.074.022-68
dc.contributor.referee1Lattes.fl_str_mv http://lattes.cnpq.br/5651616479126344
dc.contributor.referee2.fl_str_mv SANTOS, Adenilson Oliveira dos
dc.contributor.referee2Lattes.fl_str_mv http://lattes.cnpq.br/7760219759813661
dc.contributor.referee3.fl_str_mv SILVA, Leonardo de Sousa
dc.contributor.authorID.fl_str_mv 056.750.023-32
dc.contributor.authorLattes.fl_str_mv http://lattes.cnpq.br/3515712441056475
dc.contributor.author.fl_str_mv ARAÚJO, Ronaldo Andrade de
contributor_str_mv SILVA, Luzeli Moreira da
SILVA, Luzeli Moreira da
SANTOS, Adenilson Oliveira dos
SILVA, Leonardo de Sousa
dc.subject.por.fl_str_mv Compostos intermetálicos;
Propriedades magnéticas;
Efeito magnetocalórico
topic Compostos intermetálicos;
Propriedades magnéticas;
Efeito magnetocalórico
Intermetallic compounds;
Magnetic properties;
Magnetocaloric effect
Estrutura de Líquidos e Sólidos; Cristalografia
dc.subject.eng.fl_str_mv Intermetallic compounds;
Magnetic properties;
Magnetocaloric effect
dc.subject.cnpq.fl_str_mv Estrutura de Líquidos e Sólidos; Cristalografia
description Structural, magnetic and magnetocaloric properties of the RNiGe3 (R = Pr, Nd, Eu, Dy, Ho and Er) compounds were studied. The samples were synthesized by arc melting technique under argon atmosphere. X-ray diffraction (XRD) measurements and analysis by using the Rietveld method confirm the desired crystallographic phase for all studied samples. Magnetization data shows antiferromagnetic ordering for RNiGe3 compounds, with Néel temperature (TN) around 21 K, 12.5 K, 14 K, 21 K, 9 K and 6 K for R = Pr, Nd, Eu, Dy, Ho and Er, respectively. For T<TN, the compounds NdNiGe3 and EuNiGe3 present an additional transition around 6.1 K and 5 K, respectively, while PrNiGe3 presents two additional transitions around 18.5 and 15.5 K. External magnetic field application induces metamagnetic phase transitions from antiferromagnetic to ferromagnetic state. However, the observed values of the magnetic moments in high magnetic field (H= 60 and 90 kOe) and low temperatures (T = 2 K) are reduced compared to the respective free ions. The metamagnetic critical magnetic field (HC) occurs around 16 kOe, 17.3 kOe, 26.5 kOe, 10.5 kOe and 9.5 kOe, for R = Pr, Nd, Dy, Ho and Er, respectively, and around 20 and 28 kOe for R=Eu. Magnetocaloric effect (MCE) of studies compounds was evaluated by means of the isothermal magnetic entropy change (-ΔSM), in which a broad peak in -ΔSM curve associated with the magnetic transition was observed. In addition, negative MCE was observed for all samples (in ΔH < HC) due to antiferromagnetic ordering. Among the studies compounds, the highest value of -ΔSM was observed for HoNiGe3. The maximum values of -ΔSM (−𝛥𝑆𝑀𝑚𝑎𝑥) and relative cooling power (RCP) observed for RNiGe3 series were respectively, 6.1 J/kg.K and 72.9 J/kg, 4.2 J/kg.K and 68.2 J/kg, 7.5 J/kg.K and 113.6 J/kg, 5.0 J/kg.K and 106 J/kg, 16.7 J/kg.K and 308.5 J/kg, and 11.3 J/kg.K and 214.7 J/kg, for R = Pr, Nd, Eu, Dy, Ho and Er, in ΔH = 50 kOe. These values are comparable to those reported in the literature for other magnetocaloric compounds, in the same temperature range. The obtained results indicate that the RNiGe3 compounds presented interesting magnetocaloric properties for application in magnetic refrigeration at cryogenic temperatures.
publishDate 2019
dc.date.issued.fl_str_mv 2019-07-08
dc.date.accessioned.fl_str_mv 2020-01-08T13:50:49Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/masterThesis
format masterThesis
status_str publishedVersion
dc.identifier.citation.fl_str_mv ARAÚJO, Ronaldo Andrade de. Propriedades magnéticas e magnetocalóricas do sistema RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).. 2019. 83 f. Dissertação( Programa de Pós-Graduação em Ciência dos Materiais/CCSST) - Universidade Federal do Maranhão, Imperatriz, 2019.
dc.identifier.uri.fl_str_mv https://tedebc.ufma.br/jspui/handle/tede/tede/2965
identifier_str_mv ARAÚJO, Ronaldo Andrade de. Propriedades magnéticas e magnetocalóricas do sistema RNiGe3 (R = Pr, Nd, Eu, Dy, Ho e Er).. 2019. 83 f. Dissertação( Programa de Pós-Graduação em Ciência dos Materiais/CCSST) - Universidade Federal do Maranhão, Imperatriz, 2019.
url https://tedebc.ufma.br/jspui/handle/tede/tede/2965
dc.language.iso.fl_str_mv por
language por
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv application/pdf
dc.publisher.none.fl_str_mv Universidade Federal do Maranhão
dc.publisher.program.fl_str_mv PROGRAMA DE PÓS-GRADUAÇÃO EM CIÊNCIA DOS MATERIAIS/CCSST
dc.publisher.initials.fl_str_mv UFMA
dc.publisher.country.fl_str_mv Brasil
dc.publisher.department.fl_str_mv COORDENAÇÃO DO CURSO ENGENHARIA DE ALIMENTOS/CCSST
publisher.none.fl_str_mv Universidade Federal do Maranhão
dc.source.none.fl_str_mv reponame:Biblioteca Digital de Teses e Dissertações da UFMA
instname:Universidade Federal do Maranhão (UFMA)
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