新型可见光固化树脂

针对一些过氧化物固化不能满足特殊的施工环境,以及紫外光固化存在对人体有害、应用范围窄、厚膜固化性不好等缺点,开发了1种利用可见光光源进行固化的变性乙烯基酯树脂(VLC树脂),通过测定其黏度、比重、酸价、力学性能、Tg、热变形温度、积层板在一定浓度的酸、碱、水、有机溶剂等介质里面的强度保持率,分别对树脂液态特性、树脂浇铸体及积层板的力学性能以及积层板的耐腐蚀性能进行了表征,通过与一般的过氧化物固化的乙烯基酯树脂的浇铸体及积层板性能比较,可以看出:可见光固化与常见的过氧化物固化相比,性能相当甚至更佳,并且可见光固化速度极快,苯乙烯挥发极少,作业简单,无须加促进剂和固化剂,无须繁琐的搅拌和脱泡过程,提高生产效率的同时,大幅度降低施工成本。     

Formation Reaction of ZrO2 Scatterers in ZrF4-Based Fluoride Fibers

This paper clarifies the formation reaction of ZrO₂ crystals which appear as extrinsic scatterers in fluoride fibers. EPMA analysis indicates that BaO exists at grain boundaries of BaF₂ purified by sublimation. BaO reacts with ZrF₄ to form ZrO₂ at 600°C during a glass-melting process. The ZrO₂ formation reaction is influenced by H₂O. Ba(OH)₂, which is formed by the reaction between BaO and water vapor, melts at 370° to 420°C and reacts with ZrF₄ to form ZrO₂ at 450° to 520°C. When low-oxide-content BaF₂ is used for fiber preparation, scatterers significantly decrease.     

Effect of ZrO2 Inclusions on the Sinterability of Al2O3

The sinterability of Al₂O₃/ZrO₂ composite powder compacts containing 2 and 10 vol% ZrO₂ was compared to the sinterability of their single-phase constituents through constant-heating-rate experiments. The ZrO₂ inclusion phase delayed the initiation of bulk shrinkage and the temperature of maximum strain rate by 100°C. The ZrO₂ inclusion phase also significantly inhibited grain growth. These results, discussed with regard to the thermodynamics of pore disappearance, suggest that phenomena inhibiting grain growth may also inhibit densification.     

类金刚石纤维砂轮的开发及其磨削特性

为了获得高精度加工表面，最近磨具市场上有一种Al2O3纤维砂轮问世^[1]。该砂轮克服了磨粒砂轮中磨粒易于脱落的缺点，但其硬度仍受到一定限制。近十年来，由于类金刚石薄膜具有接近金刚石的硬度、高耐磨性和很低的摩擦系数等优良的机械、物理、化学和光电特性，因而被广泛地应用于精密零部件和涂附刃具的制造^[2]。如果能将类金刚石薄膜形成类金刚石纤维，然后将其代替Al2O3纤维作为磨料，就可以满足纤维砂轮的硬度要求。因此，1999年以来，日本山口胜美教授和中国魏源迁教授成功地将类金刚石纤维植入基体并与树脂结合剂结合，开发了一种类金刚石纤维砂轮^[3-5]。该砂轮中的类金刚石纤维按同一方向排列且与砂轮磨削面相垂直，纤维的端部可用作为切削刃。为了考察这种新型砂轮的磨削特性，本文作者对难加工材料如模具钢SKD11及硬脆材料如硅片、光学玻璃、石英和大理石进行了大量的磨削试验。试验结果表明能获得纳米级加工表面，例如被磨硅片和模具钢的表面粗糙度分别为Ra2nm(Ryl5nm)和Ra2nm(Ry23nm)。     

‘Jishu Kanri’ activities in the Japanese steel industry Small group activities being promoted by the industry as a whole

The group activities called ‘ Jishu Kanri ’ by foremen and workers in the forefront of production has been actively promoted in the Japanese Steel Industry by establishing a committee for ’ Jishu Kanri’ activities in the Japan Iron and Steel Federation, with the positive cooperation of its member companies. Nearly 8 years have elapsed since the establishment of this committee, and during this period the ability and skill of the group leaders and members in managing group activities and their awareness of problems and solutions have been greatly improved, thereby contributing much to the improvement of quality, attainment of production targets, reduction in the production costs, and improvement of safety

This report describes the ’ Jishu Kanri ’ activities being carried out by the industry as a whole.     

Window functions obtained by convolution integrals of rectangular windows

The rectangular, triangular, and Parzen windows, which have been defined independently of each other, are obtained by repeating convolution integrals of the rectangular window with itself. They are extended to make a series of window functions. This series has the advantage that the sidelobe fall-off is variable though it has the disadvantage that the mainlobe band-width for the same highest sidelobe level is 1–1·3 times those of the gaussian, Kaiser, Dolph–Chebyshev or Blackman–Harris windows. Moreover, this series has a desirable mainlobe bandwidth of 0·85–1 times that of cos^x x windows for the same highest sidelobe level and sidelobe fall-off. Thus, this series is useful in designing window functions whose mainlobe bandwidth is in between that of the gaussian or Kaiser windows and that of cos^x x windows and whose sidelobe fall-off is as good as that of the cos^x x windows.     

Precise Determination of the 3CaO·SiO2 Cells and Interpretation of Their X-Ray Diffraction Patterns

The cell dimensions of pure triclinic 3CaO·SiO₂ and monoclinic 3CaO·SiO₂ solid solution (54CaO·16SiO₂·Al₂O₃·MgO) were determined and the powder diffraction patterns were indexed by the method of precise measurement of the spacings. The lattice constants are expressed in terms of triclinic or monoclinic cells corresponding to pseudo-orthorhombic cells derived from Jeffery's trigonal cell. The apparent lattice constants for pure 3CaO·SiO₂ are a = 12.195 a.u., b = 7.104 au., c = 25.096 a.u., α= 90°, β= 89°44'γ= 89°44'; for 54CaO·16SiO₂.-Al₂O₃MgO, a = 12.246 a.u., b = 7.045 a.u., c = 24.985 a.u., β= 90°04'. Precise lattice constants of Jeffery's monoclinic lattice for 54CaO.-16SiO₂-Al₂O₃·MgO are derived as a = 33.091 a.u., b = 7.045 a.u., c = 18.546 a.u., β= 94°08'. High-temperature X-ray patterns showed that pure triclinic 3CaO·SiO₂ transformed to a monoclinic form at about 920°C. and then to a trigonal form at about 970°C. Monoclinic 54CaO.16SiO₂·Al₂O₃–MgO transformed to trigonal at about 830°C. These transitions were reversible and reproducible and were accompanied by only slight deformation of the structure forms.     

Kinetic Studies of Eutectoid Decomposition of CuFe5O8

The kinetics and mechanism of eutectoid decomposition of CuFe₅O₈ were studied by X-ray diffractometer, electron probe microanalyzer, and reflecting-light microscope techniques. The isothermal decomposition curves were sigmoidal and the maximum rate of decomposition occurred at ∼600°C. Sigmoidal-type curves indicated that the decomposition proceeded by a process of nucleation and growth. Kinetic data were best expressed by Avrami's equation with n≃2 and n≃4 below and above 850°C, respectively. A "site saturation" mechanism is suggested. Bainite-type and pearlite-type microstructures were observed below and above 800°C, respectively. Grain boundaries were active sites in the nucleation process.