硅酸盐体系玻璃形成范围的研究:玻璃形成范围的研究,2

M. Imaoka, T. Yamazaki
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Figs. 12 and 13) are remarkably different from the corresponding borate systems. In the borate systems, a glass-fromation range spreads on the right side of the SiO2-D line (cf. Fig. 10), and therefore it has been estimated that the co-ordination number of Ti4+ is 6. (In order for the Ti4+ ion to take 6-co-ordination as a network-former, the modifier of divalency must also be present, therefor, in the area on the left of the SiO2-D line glass-formation is impossible.) However, in the silicate system the limited line of SiO2-D is lacking. Consequently, it is concluded that the Ti4+ ion as well as the Si4+ ion takes the 4-co-ordination. The glass-formation range of the TiO2-containing systems are shown in the hatched areas of Figs. 12 and 13, which are limited by the AD line.The WO3-containing silicate systems have a remarkably narrow glass-formation range compared with borate systems. The vitrified range of the B2O3-WO3-alkali oxide system has two feet, but the silicate system, we suppose, lacks the left foot. Moreover, it is considered that the left foot consists of WO3 and alkali borate in borate systems, but that this part becomes immiscible in silicate systems.According to the devitrification of the binary system, La2O3 systems are classified as C-type ternary systems, and their glass-formation ranges are narrower than those of borate systems. The vitrified range of the SiO2-Al2O3-La2O3 system (cf. Fig. 29) agrees with that of the corresponding borate system, but the limiting line, kl, of the immiscible range is lower than that of the borate and, accordingly the glass-formation range of the former is narrower than that of the latter. Other La-silicate systems are similar. 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引用次数: 20

摘要

继之前的报告“硼酸盐体系的玻璃形成范围的研究”(the Journal, 69, 282(1961))之后,我们研究了硅酸盐体系的玻璃形成范围。虽然硅酸盐玻璃早已被使用,但对硅酸盐体系的玻璃形成范围还没有足够系统的研究。在本实验中,将1/80摩尔(约1g)的材料熔化在由纯铂或含20%铑的铂制成的坩埚中,温度从1400°到1750°C。除SiO2外,还使用了Li、Na、K、Be、Mg、Ca、Sr、Ba、Al、La、Ti、Zr、Th、Nb、Ta、w等16种a族元素的氧化物,二元硅酸盐体系的玻璃形成范围见表1。这些范围在某些方面与硼酸盐体系有所不同。例如,la -硅酸盐体系没有玻璃化范围,而mg -硅酸盐体系比硼酸盐具有更宽的玻璃化范围。组分离子是作为改性剂还是作为成网剂进入玻璃结构,取决于成网剂的酸度和组分离子的电负性。然而,在硅酸盐体系中,玻璃形成的实际范围等于玻璃形成范围与不混相范围之差。如果后者与前者相等或稍宽,则玻璃化范围将消失。三元体系的玻璃形成范围如图1-34所示。所研究的系统总数约达100个。实验结果表明,实际的玻璃形成范围与“玻璃形成条件”(This journal, 67,364(1959))所期望的范围(图中孵化的区域)一致。在这些体系中,含有TiO2的体系(参见图12和图13)与相应的硼酸盐体系有显著差异。在硼酸盐体系中,在SiO2-D线的右侧有一个玻璃化范围(参见图10),因此可以估计Ti4+的配位数为6。(为了使Ti4+离子以6-配位作为网络形成剂,还必须存在二价修饰剂,因此,在SiO2-D线左侧区域不可能形成玻璃。)然而,在硅酸盐体系中,缺乏二氧化硅- d的限制线。结果表明,Ti4+离子和Si4+离子均为4配位。含tio2体系的玻璃形成范围如图12和13的孵化区域所示,该区域受AD线限制。与硼酸盐体系相比,含wo3硅酸盐体系的玻璃形成范围非常窄。b2o3 - wo3 -碱氧化物体系的玻璃化范围有两个脚,但我们认为硅酸盐体系没有左脚。在硼酸盐体系中,认为左脚由WO3和碱硼酸盐组成,但在硅酸盐体系中,这部分变得不可混溶。根据二元体系的反玻化作用,La2O3体系可归为c型三元体系,其玻璃形成范围比硼酸盐体系窄。SiO2-Al2O3-La2O3体系的玻璃化范围(参见图29)与相应的硼酸盐体系的玻璃化范围一致,但不混相范围的极限线kl低于硼酸盐体系,因此前者的玻璃化范围比后者窄。其他的la -硅酸盐体系也是类似的。在含th2或Al2O3的c型三元体系中,在相应的硼酸盐体系中有玻璃化范围,我们发现只有SiO2具有玻璃化状态
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Studies of the Glass-formation Range of Silicate Systems : Investigations on the Glass-formation Range, 2
Following a previous report “Studies of the Glass-formation Range of Borate Systems” (This Journal, 69, 282 (1961)), we studied the glass-formation range of silicate systems. Although silicate glasses have long been used, sufficient systematic studies of the glassformation ranges of silicate systems have not yet been made.In this experiment, 1/80 mole (about 1g.) of materials were melted in crucibles made of pure platinum or platinum containing 20% rhodium at temperatures from 1400° to 1750°C. The oxides used besides SiO2 were 16 kinds of the oxides of a-group elements namely Li, Na, K, Be, Mg, Ca, Sr, Ba, Al, La, Ti, Zr, Th, Nb, Ta and W.The glass-formation ranges of binary silicate systems are shown in Table 1. These ranges differ in some points from those of borate systems. For instance, the La-silicate system has no vitrified range, while the Mg-silicate system has a wider glass-formation range than the borate. Whether a component ion enters into the glass structure as a modifier or as a network-former depends on the acidity of the glass-former and on the electronegativity of the component ion. In silicate systems, however, the actual range of glass-formation equals the difference between the glass-formation range and the immiscible range. If the latter is equal to the former or somewhat wider, the vitrified range will disappear.The glass-formation ranges of ternary systems are shown in Fig. 1-34. The whole number of the studied systems reached about one hundred. The Experimental results show that the actual glass-formation ranges agree with the range (hatched areas in the figures) to be expected from the “Conditions of Glass-formation” (This Journaj, 67, 364 (1959)). Among these systems, the systems containing TiO2 (cf. Figs. 12 and 13) are remarkably different from the corresponding borate systems. In the borate systems, a glass-fromation range spreads on the right side of the SiO2-D line (cf. Fig. 10), and therefore it has been estimated that the co-ordination number of Ti4+ is 6. (In order for the Ti4+ ion to take 6-co-ordination as a network-former, the modifier of divalency must also be present, therefor, in the area on the left of the SiO2-D line glass-formation is impossible.) However, in the silicate system the limited line of SiO2-D is lacking. Consequently, it is concluded that the Ti4+ ion as well as the Si4+ ion takes the 4-co-ordination. The glass-formation range of the TiO2-containing systems are shown in the hatched areas of Figs. 12 and 13, which are limited by the AD line.The WO3-containing silicate systems have a remarkably narrow glass-formation range compared with borate systems. The vitrified range of the B2O3-WO3-alkali oxide system has two feet, but the silicate system, we suppose, lacks the left foot. Moreover, it is considered that the left foot consists of WO3 and alkali borate in borate systems, but that this part becomes immiscible in silicate systems.According to the devitrification of the binary system, La2O3 systems are classified as C-type ternary systems, and their glass-formation ranges are narrower than those of borate systems. The vitrified range of the SiO2-Al2O3-La2O3 system (cf. Fig. 29) agrees with that of the corresponding borate system, but the limiting line, kl, of the immiscible range is lower than that of the borate and, accordingly the glass-formation range of the former is narrower than that of the latter. Other La-silicate systems are similar. Among the C-type ternary systems containing ThO2 or Al2O3, which have vitrified ranges in case of the corresponding borate systems, we found the glassy state only in the SiO2
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