Fe2+、Fe3+对CaO-Al2O3-SiO2-MgO系微晶玻璃析晶性能的影响规律

为了利用大量的含铁铝硅酸盐固体废弃物制备具有高附加值的微晶玻璃,采用DTA、XRD、SEM、EDS等手段研究了Fe2+、Fe3+对CASM系微晶玻璃析晶性能的影响.结果表明,Fe2+在微晶玻璃中与Mg2+的作用相同,取代以网络外体形式存在的Al3+,使得微晶玻璃的析晶温度逐渐下降,而对析晶能力几乎没有影响,并当Fe2+掺入量为2%时,主晶相由铝黄长石转变为镁黄长石,在7.5%时,进一步转变为透辉石.Fe3+掺量小于7.5%时,起到补充Si4+不足的作用,当大于7.5%时,部分Fe3+起到与Fe2+、Mg2+相同的作用,使得析晶温度呈先升后降的变化,在掺量为7.5%时,铝黄长石主晶相才开始转变为镁黄长石,在10%时,转变为透辉石,且析晶能力得到大幅提升.随着Fe2+和Fe3+含量增加,虽然微晶玻璃中主晶相的变化顺序相同,但Fe2+具有降低微晶玻璃析晶温度的作用,而一定量的Fe3+可作为晶核剂提高微晶玻璃的析晶能力.     

Li2O·Al2O3·4SiO2-Ta2O5系微晶玻璃分相与析晶机理研究

采用Ta2O5为晶核剂制备Li2O.Al2O3.4SiO2-Ta2O5微晶玻璃,并研究其分相、析晶机理,构建晶化模型.结果表明Ta2O5能有效促进玻璃的体积析晶,获得了晶粒尺寸为50nm的精细组织.非等温动力学计算显示随Ta2O5含量增加,析晶活化能降低,析晶指数增加,析晶动力学参数K(Tp)作为析晶判据更为合理.研究发现,LAST玻璃冷却时因亚稳分解导致互锁分相,形核前期又借助成核生长机制发生微滴分相,晶体生长则在继承亚稳分相形貌基础上发生"他形"析晶.最终构建了LAST微晶玻璃的晶化模型.     

含钛磷酸盐玻璃NaTi2(PO4)3-0.9Ca3(PO4)2的析晶行为

利用差热分析、X射线衍射仪、液氮吸附BET孔经测试仪对组成为NaTi2(PO4)3-0.9 Ca3(PO4)2的含钛磷酸盐玻璃的析晶行为进行了研究.通过对该玻璃相继进行成核、析晶和酸浸泡处理制备了NaTi2(PO4)3骨架多孔微晶玻璃.证明该玻璃在646℃8h成核处理过程中产生了旋节分解特征的成分偏聚,形成了富TiO2玻璃相和富CaO玻璃相交错生长的连通结构,成核处理后的玻璃在738℃析晶过程中依次在富钛相和富钙相中析出NaTi2(PO4)3和β-Ca3(PO4)2.成核过程对析晶的促进作用是通过促进NaTi2(PO4)3的析出而实现的.     

掺P2O5氟化镓铟基玻璃微晶化可控性机理的探讨

用熔融法制备掺少量P2O5氟化镓铟基玻璃(20GaF3-15InF3-17CdF2-15ZnF2-10SnF2-20PbF2-3P2O5),玻璃的析晶动力学分析结果表明:掺入P2O5能使氟化镓铟基玻璃的析晶双峰间温度差△Tp(△Tp=Tp1-Tp2)增大,使可控微晶化变为可能。同时利用X射线衍射分析方法(XRD)和扫描电镜讨论了该微晶化玻璃的晶相和析晶形貌,并在593 K下保温1 h能得到透明度较好、含四方晶相ZnF2的微晶玻璃。     

CaO/SiO2质量比对不锈钢渣微晶玻璃析晶及性能的影响

以不锈钢渣、废玻璃为原料,采用熔融法制备了主晶相为硅灰石相的微晶玻璃.利用DSC、XRD、SEM等测试分析手段研究了CaO/SiO2质量比对微晶玻璃物相组成、显微结构及理化性能的影响.结果表明:随CaO/SiO2质量比增加,玻璃转变温度和析晶放热峰温度逐渐降低,且析晶放热峰变尖锐;硅灰石相XRD衍射峰强度先增强后减弱;显微结构由表面析晶向整体析晶过渡,晶粒形状由球形颗粒变为针叶状晶,最后发育成片状晶,晶体尺寸先增加后减小;当CaO/SiO2质量比为0.72时微晶玻璃性能达到较优,显微硬度为6.49 GPa,密度为3.11 g/cm3,吸水率为0.11％,耐酸性96.51％,耐碱性99.92％.制备出的微晶玻璃有望应用在建筑装饰材料领域.     

ZrO2对低温烧结 BaO-Al2O3-SiO2系微晶玻璃析晶和晶型转变的影响

用烧结法制备了化学计量比和高Ba含量的两组BaO-Al2O3-SiO2(BAS)系微晶玻璃,采用差示扫描量热法(DSC)和X射线衍射分析(XRD)等手段研究了ZrO2对BAS系微晶玻璃中六方钡长石析晶和六方钡长石向单斜钡长石晶型转变的影响.研究表明,两组BAS系玻璃的烧结温度低于850℃,晶化温度低于900℃.六方钡长石的析出为整体析晶.不加形核剂晶型转变为整体析晶;添加ZrO2晶型转变为表面析晶.提高Ba含量或添加ZrO2促进六方钡长石的析出和晶粒细化.化学计量比的BAS系微晶玻璃中添加ZrO2明显促进晶型转变.高Ba含量的BAS系微晶玻璃中添加ZrO2表现为抑制晶型转变,850℃保温100h不发生转变.     

晶种对低温烧结BaO-Al2O3-SiO2系微晶玻璃析晶的影响

用烧结法制备了化学计量比和高Ba含量的两组BaO-Al2O3-SiO2(BAS)系微晶玻璃,研究了晶种对低温烧结BaO-Al2O3-SiO2系微晶玻璃析晶的影响.结果表明,玻璃的软化温度随着品种含量的增加而提高.在两组玻璃粉中添加晶种有助于降低析晶活化能,促进六方钡长石和单斜钡长石的析出;晶种含量为1%时活化能最小,成分为化学计量比的玻璃析晶峰值温度也最低.在850℃保温时间2 h,添加1%晶种的BAS系微品玻璃全部转变为单斜钡长石.在两组成分的BAS系微晶玻璃中,六方钡长石的析出表现为整体析晶.不加晶种时,单斜钡长石通过六方钡长石一单斜钡长石的晶型转变析出,表现为整体析晶;添加晶种后,单斜钡长石主要因"同构"效应直接从基础玻璃中析出,表现为表面析晶.     

亚微米Li2O-Al2O3-SiO2微晶玻璃制备

本文利用DTA、XRD和SEM对Li2O-Al2O3-SiO2(以下简称LAS)微晶玻璃核化晶化热处理制度及氟离子在该玻璃体系中的作用进行研究.通过分析得出:含氟LAS玻璃核化温度和晶化温度分别为620℃和710℃,比相同组份的不含氟Li2O-Al2O3-SiO2玻璃核化、晶化温度分别降低了40℃和160℃左右;引入氟离子明显降低LAS玻璃析晶温度,系统的活化能降低约54kJ/mol,当含氟LAS玻璃的核化时间为1h、晶化时间为4hrs,平均微晶颗粒尺寸在50nm左右.     

B2O3-Al2O3-SiO2系微晶玻璃析晶动力学研究

采用差示扫描量热（DSC）分析法对B2O3-Al2O3-SiO2系统微晶玻璃的析晶动力学参数进行了测定，研究了该系统微晶玻璃的析晶动力学。结果表明：随着B2O3/SiO2比的降低，该系统玻璃的析晶活化能E呈先升高后降低的变化趋势，当B2O3/SiO2比为11：5时，析晶活化能最小，Emin=375．4kJ／mol，晶化指数n则先减小后增大，但均〉4，表明该系统玻璃可整体析晶。     

CaF2对CAMS系矿渣微晶玻璃析晶特性及抗腐蚀性能的影响

以白云鄂博二次选后尾矿、高炉渣和粉煤灰为主要原料,采用熔融法制得不同CaF_2含量的CaOAl_2O_3-MgO-SiO_2(CAMS)系微晶玻璃,利用DSC、XRD、SEM、EDS等测试手段,研究了CaF_2对微晶玻璃析晶行为、显微结构及抗盐酸腐蚀性能的影响。结果表明:氟化钙添加量由2%增加至8%(质量分数),基础玻璃的析晶温度降低,析晶活化能由416.28kJ/mol降为309.02kJ/mol,但微晶玻璃的主晶相仍为透辉石相。氟化钙的添加在一定程度上降低了微晶玻璃的抗盐酸腐蚀性能,当氟化钙添加量为2%时,微晶玻璃经盐酸溶液浸泡21d,腐蚀层厚度为240μm;随着CaF_2添加量继续增大,微晶玻璃抗盐酸腐蚀性能急剧下降,当氟化钙添加量为8%时,盐酸腐蚀21d后,腐蚀层厚度为743μm。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O