Detalhes bibliográficos
Ano de defesa: |
2008 |
Autor(a) principal: |
Lima, Cleânio da Luz |
Orientador(a): |
Não Informado pela instituição |
Banca de defesa: |
Não Informado pela instituição |
Tipo de documento: |
Dissertação
|
Tipo de acesso: |
Acesso aberto |
Idioma: |
por |
Instituição de defesa: |
Não Informado pela instituição
|
Programa de Pós-Graduação: |
Não Informado pela instituição
|
Departamento: |
Não Informado pela instituição
|
País: |
Não Informado pela instituição
|
Palavras-chave em Português: |
|
Link de acesso: |
http://www.repositorio.ufc.br/handle/riufc/1091
|
Resumo: |
The molibidatos up a large class of inorganic compounds and have been the subject of several investigations. Usually the members of this family have Y2XO4.nH2O general formula, where Y = (Na, Ca), X = (Mo, S, W, Mn) with n = (0, 1, 3, 4...). The Na2MoO4.2H2O was studied through experiments of Raman spectroscopy aimed at investigating the effects of hydrostatic pressure on their properties structural and vibrational. The material Na2MoO4.2H2O experiencing a transition phase when the compressor is half the mixture of alcohols, this transition is structural. When the compressor is the way nujol (mineral oil) Na2MoO4.2H2O try the two-phase transitions. The difference for these events is that the Na2MoO4.2H2O interacts with the environment compressor alcohol, since the pressure to relax the spectrum of the material presents itself as being semidesidratrado not going back to the original phase. When the compressor means is the nujol, as well as an additional step, the Na2MoO4.2H2O, in the process of relaxation, restores the original phase, where the interim stage is deleted due to the effect of hysteresis. Therefore, it identifies three distinct phases in Na2MoO4.2H2O, in a range of 0 to 3.0 GPa (phase α), another between 3.0 and 4.0 GPa (phase δ) and third over 4.0 GPa (phase β). The first transition from phase α to phase δ is a conformal transition, due to distortions in tetraedros MoO4, leaving the group of symmetry D2h 15. The second transition is a structural transition due to the collapse of two modes in a single event, especially in the modes of the network, which indicates a transition to a structure for greater symmetry than the previous (possibly of the orthorhombic for tetragonal). |