首页> 外文会议>The Annual Meeting of The American Ceramic Society >CRYSTALLIZATION OF A Li{sub}2O·2SiO{sub}2 GLASS UNDER HIGH HYDROSTATIC PRESSURES
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CRYSTALLIZATION OF A Li{sub}2O·2SiO{sub}2 GLASS UNDER HIGH HYDROSTATIC PRESSURES

机译:高静水压压力下的Li {次} 2O·2SIO {Sub} 2玻璃结晶

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The crystallization behavior of a Li{sub}2O·2SiO{sub}2 (LS{sub}2) glass subjected to a uniform hydrostatic pressure of 4.5 or 6 GPa was investigated between 543 and 750°C using XRD, IR, Raman, TEM and DTA. The density of all the glasses (or glass-ceramics) subjected to high pressures was higher than that of the glass at ambient pressures (one atmosphere), and was 2.43 ±0.01 g/cm{sup}3 for the 4.5 GPa glass and between 2.52 ± 0.01 g/cm{sup}3 and 2.57 ± 0.01 g/cm{sup}3, depending upon processing temperature, for the 6 GPa glasses. The crystallization tendency for the glasses decreased (the crystal growth rate curve moved to higher temperatures) with increasing pressure. A decrease in the diffusion coefficient and/or developing additional stress at the glass-crystal interface at high pressures could be the likely reasons for suppressing the crystal growth rates. Like the glass at ambient pressure, the glass subjected to 4.5 GPa crystallized only LS{sub}2(orthorombic,Ccc2) crystals. The density of both glasses, ambient and 4.5 GPa, was smaller man that of the crystal, 2.46 ± 0.01 g/cm{sup}3. The structure of the crystals formed in the glasses that were subjected to 6 GPa pressure and whose density was higher than that of Li{sub}2O·SiO{sub}2 (LS) crystals, was complex and unknown. The structure of these crystals is believed to be a deformed LS-type, whose parameters yield a calculated crystal density of 2.61 g/cm{sup}3 which is higher than the measured density of these glass-ceramics, It is believed that crystallization of these glasses follows a route which favors forming only those crystals that are accompanied by a positive, but lowest possible density change.
机译:使用XRD,IR,拉曼在543和750℃之间研究了对4.5或6GPa均匀静压压力的Li {Sub} 2O·2SiO {Sub} 2(Ls {Sub} 2)玻璃的结晶行为。 TEM和DTA。在环境压力(一种大气)下,经受高压的所有玻璃(或玻璃陶瓷)的密度高于玻璃(一种大气),为4.5GPa玻璃和2.43±0.01g / cm {sup} 3。 2.52±0.01g / cm {sup} 3和2.57±0.01g / cm {sup} 3,取决于6 gpa眼镜的加工温度。玻璃的结晶趋势降低(晶体生长速率曲线移动到较高温度)随着压力的增加。在高压下玻璃晶界面处的扩散系数和/或施加额外应力的降低可能是抑制晶体生长速率的可能原因。与环境压力下的玻璃一样,对4.5GPa进行4.5GPa的玻璃仅结晶LS {亚} 2(矫形器,CCC2)晶体。眼镜,环境和4.5GPa的密度较小的男性晶体,2.46±0.01g / cm {sup} 3。形成在玻璃中的晶体的结构对6GPa压力进行6gPa压力并且其密度高于Li {SiO} 20·SiO} 2(LS)晶体,是复杂的并且未知的。认为这些晶体的结构是变形的LS型,其参数产生的计算出的2.61g / cm {sup} 3的晶体密度高于这些玻璃陶瓷的测量密度,据信结晶这些玻璃遵循仅伴随着伴随阳性但最低可能密度变化的晶体的途径。

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