25℃至熔点温度范围内碱硅酸盐的热力学量

Katsuaki Takahashi, T. Yoshio
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引用次数: 57

摘要

用连续高温量热计测定了碱硅酸盐玻璃和晶体在25℃至熔点之间的热含量。确定了R2O⋅2SiO2 (R=Li, Na, K)组成的玻璃和晶体在上述温度范围内的熵,并计算了由晶体形成玻璃反应的自由能变化。将所得的自由能值与ΔG=ΔT⋅ΔHf/Tm和ΔG=(ΔT⋅ΔHf/Tm)⋅(T/Tm)两个近似方程计算的自由能值进行比较。这一比较表明,除了熔点附近较窄的温度范围外,这些方程的自由能值不适用于动力学过程的讨论。研究了300℃和600℃时SiO2的摩尔比热容与组成(R2O/SiO2的摩尔比)的关系。在Na2O-SiO2晶体体系中,热容随Na2O/SiO2比线性增加。这条直线的斜率和Na2O组成为零时的交点分别近似对应于结晶Na2O和结晶SiO2的热容。从这一结果可以推测,可加性近似适用于Na2O-SiO2晶体的热容。对于Na2O-SiO2和K2O-SiO2玻璃和过冷液体,热容量的组分依赖性在R2O/SiO2=0.5时出现了一个变化。从玻璃和液体的结构角度对这些结果进行了讨论。
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Thermodynamic Quantities of Alkali Silicates in the Temperature Range from 25°C to Melting Point
The heat contents of the alkali silicate glasses and crystals have been measured from 25°C to melting temperature with a continuous high-temperature calorimeter.The entropy in the above temperature range is determined for the glasses and crystals of the composition R2O⋅2SiO2 (R=Li, Na, K). The free-energy change is calculated for the reaction of forming the glasses from the crystals. The free-energy values thus obtained are compared with those calculated from two approximate equations, ΔG=ΔT⋅ΔHf/Tm and ΔG=(ΔT⋅ΔHf/Tm)⋅(T/Tm). This comparison indicates that the free-energy values from these equations are inapplicable to the discussion on the kinetic process except for the case in the narrow temperature range near the melting point.The relation between the heat capacity per mole of SiO2 and composition expressed by the mole ratio R2O/SiO2 at 300° and 600°C is also investigated. In the system Na2O-SiO2 crystals, the heat capacity increases linearly with Na2O/SiO2 ratio. The slope of this straight line and the intersection at zero Na2O composition approximately correspond to the heat capacity of crystalline Na2O and that of crystalline SiO2, respectively. From this result, it can be assumed that the additivity approximately holds for the heat capacity of Na2O-SiO2 crystals.For Na2O-SiO2 and K2O-SiO2 glasses and supercooled liquids, the composition dependence of heat capacity shows an inflection at the composition of R2O/SiO2=0.5. These results are discussed from the view point of structure of glass and liquid.
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