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Refractive Index and Compressibility of the KAlSi3O8 Glassat Pressures up to 6.0 GPa

机译:压力高达6.0 GPa时KAlSi3O8玻璃的折射率和可压缩性

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摘要

The refractive index of potassium aluminosilicate glass of the KAlSi3O8 composition in the pressure range up to 6.0 GPa has been measured using a polarizing interference microscope and an apparatus with diamond anvils. The changes in the relative density, which characterize the compressibility of the K2O·A12O3·6SiO2 glass, have been estimated in the pressure range under investigation from the measured refractive indices within the framework of the theory of photoelasticity. The results have been compared with the data previously obtained for the Na2O;;Al2O3;;6SiO2 glass. Although the molar contents of A12O3 and M2O (where M = K or Na) are identical in these glasses, the KAlSi3O8 glass exhibits a higher compressibility, which agrees with the lower degree of depoly-merization of this glass as compared to that observed in the NaAlSi3O8 glass. The pressure derivative of the bulkmodulus K_t', which is calculated from the Birch-Murnaghan equation for the KAlSi3O8 glass (K_t', = 7-9), ishigher than that for the NaAlSi3O8 glass (K_t' = 5.5-6.0). An increase in the pressure derivative of the bulk modulusK_t' upon replacement of the Na~+ cations by the K~+ cations is explained by the inhibition of compression ofthe large K~+ cations, which are located in cavities and have a considerably larger orbital radius than the Na~+ cations. This manifests itself in the fact that the curves describing the dependences of the change in the relative density (d - d0)/d (compressibility) on the pressure P for the KAlSi3O8 and NaAlSi3O8 glasses converge at pressures above 4.0 GPa.
机译:已经使用偏振干涉显微镜和带有金刚石砧的设备测量了在高达6.0GPa的压力范围内的KAlSi 3 O 8组成的铝硅酸钾玻璃的折射率。相对密度的变化是表征K2O·Al2O3·6SiO2玻璃可压缩性的特征,它是在光弹性理论的框架内根据测量的折射率在所研究的压力范围内估算的。将结果与先前获得的Na2O ;; Al2O3 ;; 6SiO2玻璃的数据进行了比较。尽管这些玻璃中的Al2O3和M2O(其中M = K或Na)的摩尔含量相同,但KAlSi3O8玻璃具有较高的可压缩性,与在玻璃中观察到的较低的解聚度相吻合。 NaAlSi3O8玻璃。根据Birch-Murnaghan方程计算的KAlSi3O8玻璃(K_t'= 7-9)的体积模量K_t'的压力导数高于NaAlSi3O8玻璃的K_t'= 5.5-6.0的压力导数。用K〜+阳离子代替Na〜+阳离子后,体积模量K_t'的压力导数增加是由于抑制了大K〜+阳离子的压缩所致,这些大K〜+阳离子位于空穴中,并且轨道较大半径比Na〜+阳离子大。这本身表现为以下事实:描述相对密度(d-d0)/ d(可压缩性)变化对KAlSi3O8和NaAlSi3O8玻璃的压力P的依赖性的曲线在高于4.0 GPa的压力下会聚。

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