钛型药芯焊丝配方研制

本文阐述的是钛型药芯焊丝实际研制生产及应用过程中遇到的几个问题，并阐述了解决的途径和措施。     

PS3.0微机极谱法测定勾调用水中微量铁

采用PS3.0微机极谱法测定了勾调用水中微量铁，检测下限达到5μg/Al，线笥范围10-250ug/L，相对标准偏差为4.8%，锌、锰、铅、铜、镉不干扰测量，铁的PAR催化波与锰的催化波完全分离。分析结果令人满意。     

正交偶极声波测井技术在碎屑岩储层评价中的应用初探

正交偶极声波测井是一种测量地层岩石声学信息，进而分析地层各向异性的测井新技术，首次在渤海海域NB35—2—8井碎屑砂泥岩地层中应用，不仅获得了明下段主要砂体储层内部的非均质性特征信息，而且还获得了地应力方向和古流向等信息。这些信息的获得，有助于储层的精细描述与评价。     

Formation of composites fabricated by exothermic dispersion reaction in A1-TiO2-B2O3 system

The formation of aluminum matrix composites fabricated by exothermic dispersion reaction in A1-TiO2-B2O3 system was investigated. The thermal analysis results show that the reactions are spontaneous and exothermic. The Gibbs free energy of α-Al2O3 is the lowest among all the combustion products, followed by TiB2 and Al3Ti. It is noted that when the B2O3/TiO2 mole ratio is below 1, the reaction products are composed of particle-like α-Al2O3, TiB2 and rod-like Al3Ti. The α-Al2O3 crystallites, resulting from the reaction between A1 and TiO2 or B2O3, are segregated at the grain boundaries due to a lower wettability with the matrix. SEM micrographs show that rod-like Al3Ti phase distributes uniformly in the matrix. When the BEO3/TiO2 mole ratio is around 1, the Al3Ti phase almost disappears in the composites, and the distribution of α-Al2O3 particulates is improved evidently.     

松软厚煤层轻放工作面切眼锚杆支护实践

针对朱仙庄矿 84 15工作面切眼特殊的地质条件 ,介绍了高强锚杆 (索 )支护技术成功应用于特厚极软煤层的经验 ,并对巷道支护成本进行了分析     

“国际钛产业发展高峰论坛”举行

6月28日～29日，“国际钛产业发展高峰论坛”在江苏省东海县举行，此次论坛由香港新时代国际实业有限公司、东海县人民政府、东海新时代应用材料有限公司主办。国内外200多位钛产业相关人士出席了会议，本次论坛深入探讨了中国钛产业的现状及发展趋势，并探索如何深入挖掘钛产业的潜在市场。会议讨论了国内的钛产业发展格局和主要问题，     

钛的应用及前景展望

从传统应用及新兴应用两方面对钛的应用进行了综述,并对钛的应用前景进行了展望。     

Spin Dependent Hopping in Ti Doped La0.67 Ca0.33 MnO3

A systematic investigation of the magnetic and transport properties of Ti doped La0.67Ca0.33MnO3 was reported. The Ti substitution for Mn ions results in a reduction in ferromagnetism and conductivity. The metal-insulator transition temperature is close to Curie temperature which decreases from 274 to 82 K as x increases from 0 to 0.17. The most important effect of Ti doping is to introduce spin clusters in the samples due to the distortion of local lattice and the inhomogeneous magnetic structure induced primarily by the random distribution of Mn ions. A maximum magnetoresistance ratio as large as 90% in 1 T at 122 K was obtained for the sample with x =0. 055, which is four times larger than that obtained for LCMO sample at 272 K. There is a remarkable field-history dependent MR in the cooling process for the doped samples while such phenomenon disappears in the warming run. The resistivity follows well the variable range hopping behavior in paramagnetic state. Both the size effect and spin dependent hopping of carriers between the spin clusters should be considered in this system.