α—Ti氢处理后的组织结构与性能

研究了氢化处理退火α－Ｔｉ板材的组织，结构及性能的影响，α－Ｔｉ在室温出现两种结构的氢化物：有序的ｆｃｔγ相（ＴｉＨ）和Ｆｃｃδ（ＴｉＨ）２。分析了Ｘ射线衍射只查觉到δ相的原因，氢化物的数量及形态影响除氢后基体的晶粒组织。控制氢含量可以改善伸性能及疲劳性能。     

反应烧结TiB_2－SiC复相陶瓷的物相反应、力学性能及残余应力

利用ＴｉＨ２，Ｓｉ和Ｂ４Ｃ之间的化学反应制备ＴｉＢ２－ＳｉＣ复相陶瓷，研究了反应时物相生成机理及添加Ｎｉ对材料力学性能的影响．采用ＳＥＭ观察复相陶瓷的显微结构及裂纹扩展过程，用ＸＲＤ法测定了复相陶瓷内的残余应力，探讨了复相陶瓷的增韧机理同时，残余应力测试结果表明，精磨会给材料表面带来一定的机械加工应力，但随方向而异，并对残余应力的测定造成影响     

反应烧结TiB2—SiC复相陶瓷的物相反应,力学性能及残余应力

利用ＴｉＨ２，Ｓｉ和Ｂ４Ｃ之间的化学反应制备ＴｉＢ２－ＳｉＣ复相陶瓷，研究了反应时物相生成机理及添加Ｎｉ对材料力学性能的影响，采用ＳＥＭ观察复相陶瓷的显微结构及裂纹扩展过程，用ＸＲＤ法测定了复相陶瓷内的残余应力，探讨了复相陶瓷的增韧机理，同时，残余应力测试结果表明，精磨会给材料表面带来一定的机械加工应力，但随方向而异、并对残余应力的测定造成影响。     

TiO2—Al—B系反应烧结制备的复相陶瓷和原位Al基复合材料

采用反应烧结方法，利用ＴｉＯ２，Ａｌ和Ｂ粉末间的放热反应的较低的温度下制备Ａｌ２Ｏ３－ＴｉＢ２复相陶瓷和原位生长Ａｌ２Ｏ３和ＴｉＢ２弥散粒子增强Ａｌ复合，Ａｌ２Ｏ３－ＴｉＢ２复相陶瓷是密度ρ－０．８的多孔体，由尺寸小于２μｍ，在基体中呈现均匀分布，没有发现Ａｌ３Ｔｉ生成，这种原位Ａｌ基复合材料具有优于ＳｉＣｗ／Ａｌ复合材料的强度。     

高能球磨制备TiB_2/TiC纳米复合粉体

研究了通过高能球磨制备ＴｉＢ２／ＴｉＣ纳米复合粉体的反应过程和机理,对粉体的显微结构进行了表征．实验结果表明,采用金属 Ｔｉ和 Ｂ４Ｃ为原料,在球磨过程中, ＴｉＣ先于 ＴｉＢ２形成．球磨５ｈ后Ｔｉ与Ｂ４Ｃ反应生成ＴｉＢ２和ＴｉＣ,在随后的长时间高能球磨过程中ＴｉＢ２和ＴｉＣ两相保持稳定．球磨 ３０ｈ后,直径约 ８ｎｍ的 ＴｉＣ纳米粒子分布在 １００～２００ ｎｍ的 ＴｉＢ２粒子中,形成均匀分布的纳米ＴｉＢ２／ＴｉＣ复合粉体．     

TiO_2－Al－B系反应烧结制备的复相陶瓷和原位Al基复合材料

采用反应烧结方法，利用ＴｉＯ２，Ａｌ和Ｂ粉末间的放热反应在较低的温度下制备Ａｌ２Ｏ３－ＴｉＢ２复相陶瓷和原位生长Ａｌ２Ｏ３和ＴｉＢ２弥散粒子增强Ａｌ复合材料Ａｌ２Ｏ３－ＴｉＢ２复相陶瓷是密度ρ～０．８的多孔体，由尺寸约１０μｍ的生长单元构成晶粒，在陶瓷中还含有少量的Ａｌ３Ｔｉ．Ａｌ基复合材料中原位形成的Ａｌ２Ｏ３和ＴｉＢ２粒子尺寸小于２μｍ，在基体中呈现均匀分布，没有发现Ａｌ３Ｔｉ生成．这种原位Ａｌ基复合材料具有优于ＳｉＣｗ／Ａｌ复合材料的强度．     

活性填料在制备陶瓷基复合材料中的应用

研究了Ｔｉ,ＴｉＨ２等活性填料在聚碳硅烷先驱体裂解制备ＳｉＣ陶瓷材料中的应用,Ｔｉ、ＴｉＨ２等可增加聚碳硅烷的裂解陶瓷产率,可与Ｎ２气氛反应生成氮化物,导致体积膨胀而降低陶瓷的气孔率,提高材料性能。     

B4C-TiB2复相陶瓷的强韧化研究

采用热压烧结工艺，制备Ｂ４Ｃ－ＴｉＢ２复相陶瓷。结果表明，复相陶瓷的抗弯强度，断裂韧性和显向硬度受第二相ＴｉＢ２颗粒的影响，其中Ｂ４Ｃ－３０ｖｏｌ％ＴｉＢ２材料的弯曲强度为７２５ＭＰａ，比单体Ｂ４Ｃ提高６５％，Ｂ４Ｃ－４５ｖｏｌ＾ＴｉＢ２材料的断裂韧性为６．７ＭＰａ．ｍ＾１／２，比单体Ｂ４Ｃ提高８４％，由Ｂ４Ｃ基体和ＴｉＢ２颗粒热膨胀系数不匹配导致的残余应国是Ｂ４Ｃ－Ｔdisplay status     

真空烧结炉漏气率对TiB_2-Ni金属陶瓷性能的影响

研究了真空烧结炉的不同漏气率对ＴｉＢ２Ｎｉ金属陶瓷的机械性能的影响。结果表明：低漏气率真空烧结炉烧出的ＴｉＢ２Ｎｉ试样性能比高漏气率炉烧出的试样性能优异得多。     

真粉烧结炉漏气率对TiB2—Ni金属陶瓷性能的影响

研究了真空烧结炉的不同漏气率对ＴｉＢ２－Ｎｉ金属陶瓷的机械性能的影响。结果表明：低漏气率真空烧结炉烧出的ＴｉＢ２－Ｎｉ试样性能比高温气率炉烧出的试样得多。     

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.     

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.     

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.     

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.     

Thermoelectric power of single-phase samples of Tl2CaBa2Cu2O y and Ba2CaSr2Cu2O y

Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-T _c . The thermopower was positive and decreased linearly with increasing temperature aboveT _c (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.     

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     

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.