The Philosophical Magazine A Journal of Theoretical Experimental and Applied Physics · 2004 · 45 citations · 22 references
Natural SciencesChemistryMaterials ScienceInorganic ChemistryPhase TransformationsPhysical ChemistryCrystal ChemistryPartial MeltingPhase ChangePhase Transition AnalysisPhase TransitionsRaman SpectroscopyMeltingMelting BehaviorMelting PointPhase Transformation AnalysisSilicate Crystal StructuresSilicate Melt StructureSilicate Phase EquilibriaSilicate Transformation
Abstract Raman spectra of binary alkali silicates were measured at various temperatures from 1300°C to room temperature to investigate the relation between structural change and phase transformation phenomena. Distribution of structural units of Q n was estimated at each temperature by the deconvolution of spectra based on the equilibrium 2Q3 ↔ Q2 + Q4. The Q n distributions of sodium and potassium silicate systems strongly depend on temperature and the equilibrium shifts to the left-hand side with decreasing temperature, but those of lithium silicate system were less sensitive to the temperature variation. In alkali disilicates (33 mol% R2O–67 mol% SiO2, where R=Li, Na or K), the Q n distributions near the melting point were independent of alkali ion species, and they held the relation [Q2] = [Q4] ≈ [Q3]/4. This means that two of 6Q3 units (six-memberd ring) in crystals are transformed into a pair of Q2 and Q4 in the melting process. Below the melting point, the Q n distribution in lithium disilicate melt remained while, in sodium and potassium disilicate melts, [Q3] increased with decreasing temperature. Crystallization of the alkali disilicate melts is discussed considering the configuration entropy of Q n units. In 25 mol% Li2O–75 mol% SiO2, which is in the range of the immiscibility dome, the Q n distribution was maintained even when phase separation occurs in the cooling process.
22