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A volume temperature relationship for liquid GeO2 and some geophysically relevant derived parameters for network liquids

机译:Geo2和网络液体的一些地球物理相关的衍生参数

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摘要

The thermal expansivity of liquid GeO2 at temperatures just above the glass transition has been obtained using a combination of scanning calorimetry and dilatometry. The calorimetric and dilatometric curves of c p and dV/dT are normalized to the temperature derivative of fictive temperature versus temperature using the method of Webb et al. (1992). This normalization, based on the equivalence of relaxation parameters for volume and enthalpy, allows the completion of the dilatometric trace across the glass transition to yield liquid expansivity and volume. The values of liquid volume and expansivity obtained in this study are combined with high temperature densitometry determinations of the liquid volume of GeO2 by Sekiya et al. (1980) to yield a temperature-volume relation for GeO2 melt from 660 to 1400 °C. Liquid GeO2 shows a strongly temperature-dependent liquid molar expansivity, decreasing from 20.27 × 10–4 cm3 mol–1°C–1 to 1.97 × 10–4cm3 mol–1 °C–1 with increasing temperature. The coefficient of volume thermal expansion ( v ) decreases from 76.33 × 10–6 °C–1 to 2.46 × 10–6 °C–1 with increasing temperature. A qualitatively similar volume-temperature relationship, with v decreasing from 335 × 10–6 °C–1 to 33 × 10–6 °C–1 with increasing temperature, has been observed previously in liquid B2O3. The determination of the glass transition temperature, liquid volume, liquid and glassy expansivities and heat capacities in this study, combined with compressibility data for glassy and liquid GeO2 from the literature (Soga 1969; Kurkjian et al. 1972; Scarfe et al. 1987) allows the calculation of the Prigogine-Defay ratio (), c p -c v and the thermal Grüneisen parameter ( th) for GeO2. From available data on liquid SiO2 it is concluded that liquid GeO2 is not a good analog for the low pressure properties of liquid SiO2.
机译:结合扫描量热法和膨胀法已获得了液态GeO2在刚好高于玻璃化转变温度下的热膨胀系数。使用Webb等人的方法,将c p和dV / dT的量热和膨胀曲线归一化为虚拟温度对温度的温度导数。 (1992)。基于体积和焓的弛豫参数的等价关系,该归一化可以完成整个玻璃化转变的膨胀曲线,从而产生液体的膨胀性和体积。本研究中获得的液体体积和膨胀率值与Sekiya等人的高温光密度法测定GeO2的液体体积相结合。 (1980年)得出GeO2熔体的温度-体积关系为660至1400°C。液态GeO2表现出强烈的温度依赖性,其液体摩尔膨胀系数随温度升高而从20.27×10–4 cm3 mol–1°C–1降至1.97×10–4cm3 mol–1°C–1。随着温度升高,体积热膨胀系数(v)从76.33×10–6°C–1降至2.46×10–6°C–1。先前已经在液态B2O3中观察到定性相似的体积-温度关系,随着温度的升高,v从335×10–6°C–1降至33×10–6°C–1。在这项研究中,确定玻璃化转变温度,液体体积,液体和玻璃态的膨胀性和热容量,并结合文献中的玻璃态和液体GeO2的可压缩性数据(Soga 1969; Kurkjian等人1972; Scarfe等人1987)允许计算GeO2的Prigogine-Defay比(),cp -cv和Grüneisen热参数(th)。从有关液态SiO2的可用数据可以得出结论,对于液态SiO2的低压特性,液态GeO2不是很好的类似物。

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