Development And Characterization Of Composite Ni-Cr-C-Caf2 Laser Cladding On Gamma-Tial Intermetallic Alloy

A process of laser cladding Ni-CF-C-CaF2 mixed powders to form a multifunctional composite coatingd on gamma-TiAl substrate was carried out. The microstructure of the coating was examined using XRD, SEM and EDS. The coating has a unique microstructure consisting of primary dendrite or short-stick TiC and block Al4C3 carbides reinforcement as well as fine isolated spherical CaF2 solid lubrication particles uniformly dispersed in the NiCrAlTi (gamma) matrix. The average microhardness of the composite coatings is approximately HV 650 and it is 2-factor greater than that of the TiAl substrate. (C) 2008 Elsevier B.V. All rights reserved.

A novel short neurotoxin, cobrotoxin c, from monocellate cobra (Naja kaouthia) venom: isolation and purification, primary and secondary structure determination, and tertiary structure modeling

A novel short neurotoxin, cobrotoxin c (CBT C) was isolated from the venom of monocellate cobra (Naja kaouthia) using a combination of ion-exchange chromatography and FPLC. Its primary structure was determined by Edman degradation. CBT C is composed of 61 amino acid residues. It differs from cobrotoxin b (CBT B) by only two amino acid substitutions, Thr/Ala11 and Arg/Thr56, which are not located on the functionally important regions by sequence similarity. However, the LD50 is 0.08 mg/g to mice, i.e. approximately five-fold higher than for CBT B. Strikingly, a structure-function relationship analysis suggests the existence of a functionally important domain on the outside of Loop III of CBT C. The functionally important basic residues on the outside of Loop III might have a pairwise interaction with alpha subunit, instead of gamma or delta subunits of the nicotinic acetylcholine receptor (nAChR). (C) 2002 Elsevier Science Inc. All rights reserved.

Multi-electron processes in C-13(6+) ions with neon collisions in energy region 4.15-11.08 keV/u

The cross-section ratios of double-, triple-, quadruple-, and the total multi-electron processes to the single electron capture process sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC)) as well as the relative ratios among reaction channels in double-electron active, triple-electron active and quadruple- electron active are measured in C-13(6+) -Ne collision in the energy region of 4.15-11.08 keV/u by employing position-sensitive and time-of-flight coincident techniques. It is determined that the cross-section ratios sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC) are approximately the constants of 0.20 +/- 0.03, 0.16 +/- 0.04, 0.06 +/- 0.02 and 0.42 +/- 0.05. These values are obviously smaller than the predictions of the molecular Coulomb over-the-barrier model (MCBM) [J. Phys. B 23 (1990) 4293], the extended classical over-the-barrier model (ECBM) [J. Phys. B 19 (1986) 2925] and the semiempirical scaling laws (SL) [Phys. Rev. A 54 (1996) 4127]. However, the relative ratios among partial processes of DE, TE and QE are found to depend on collision energy, which suggests that the collision dynamics depends on the collision velocity. The limitation of velocity-independent character of ECBM, MCBM and SL is undoubtedly shown.

Molecular vibration spectroscopy study of irradiation effect in C-60 films induced by low energy ion

Irradiation effect in C-60 films induced by 170 keV B ion was investigated by means of Fourier transform infrared (FTIR) and Raman spectroscopies. The damage cross section sigma and the effective damage radius R are deduced from the experimental data of all four IR active modes and evident four Raman active modes of C-60 molecule. The differences on irradiation sensitivity and structural stability of the different active modes of C-60 molecule are compared. The results indicate that T-1u (4) of infrared active mode and A(g) (1) of Raman active mode are most sensitive for B ion irradiation. On the other hand T-1u (2) of infrared active mode and H-g (3) of Raman active mode are comparatively stable under B ion irradiation. (C) 2010 American Institute of Physics. [doi:10.1063/1.3512968]

Electrochemical studies of cytochrome c disulfide at gold electrodes

The electrochemistry of disulfide in cytochrome c on gold electrodes was reported. The observed electrochemical response was used to explain why the electrochemical reaction of cytochrome c is irreversible at gold electrodes. Disulfide bonds in cytochrome c were strongly adsorbed onto the surface of gold electrodes and caused slow rate of electron transfer of the heme group. It was found that the presence of disulfides in cytochrome c was responsible for the lack of electrochemical response of the heme group on a gold electrode. The mechanisms for this effect were studied using electrochemistry and photoelectron spectroscopy. (C) 1999 Elsevier Science B.V. All rights reserved.

THE CLEAVAGE REACTION OF THE MO-MO TRIPLE BOND - THE CRYSTAL-STRUCTURES OF MOLYBDENUM COMPLEXES [CPMO(CO)(2)(C(5)H(4)NS)], [CPMO(CO)(2)(C(9)H(6)NS)]O=PPH(3) AND [CPMO(CO)(2)(S(2)CNME(2)]

The reactions of [Cp2Mo2(CO)4] (1) with 2,2'-dipyridyl disulphide (C5H4NS-)2, 8,8'-diquinolyl disulphide (C9H6NS-)2 and tetramethyl thiuram disulphide (Me2NC(S)S-)2 in toluene solution resulted in the cleavage of the Mo-Mo triple bond to yield molybdenum complexes [CpMo(CO)2(C5H4NS)] (2), [CpMo(CO)2(C9H6NS)] (3) and [CpMo(CO)2(S2CNMe2)] (4), respectively. The molecular structures of 2, 3 . O=PPh3 and 4 were determined by X-ray diffraction studies. Crystals of 2 are monoclinic, space group P2(1)/n, with Z = 4, in a unit cell of dimensions a = 6.448(1), b = 12.616(2), c = 14.772(2) angstrom, beta = 92.85(1)-degrees. The structure was refined to R = 0.028 and R(w) = 0.039 for 1357 observed reflections. Crystals of 3 . O=PPh3 are triclinic, space group P1BAR, with Z = 2, in a unit cell of dimensions a = 11.351(3), b = 13.409(3), c = 9.895(2) angstrom, alpha = 94.59(2), beta = 90.35(2), gamma = 78.07(2)-degrees. The structure was refined to R = 0.033 and R(w) = 0.037 for 3260 observed reflections. Crystals of 4 are monoclinic, space group P2(1)/a and Z = 4 with a = 12.468(5), b = 7.637(2), c = 13.135(4) angstrom, beta = 96.62(3). The structure was refined to R = 0.032 and R(w) = 0.042 for 1698 observed reflections. Each of complexes 2-4 contains a cyclopentadienyl ligand, a cis pair of carbonyls and a chelate ligand (S,N donor or S,S donor). All the compounds have distorted square-pyramid structures.

扬子地块周边C、P硅岩建造中硒的富集机理对比研究-以渔塘坝、紫阳富硒区为例

在自然界中存在一套由硅质岩、泥质岩／页岩或板岩、碳酸盐岩和粉砂岩组成的沉积建造，并以富含有机质和菌藻微生物等为特征，沉积厚度较大，岩石类型以硅岩为主，称之为“硅岩建造”。硅岩建造中的硅质岩不仅是许多重要矿种（如金、硒、铀、钒、磷、锰、铂族元素、重晶石和黄铁矿等）的赋存层和含矿岩系的重要岩类，而且由于它形成于特定的地球化学条件下，能够反映出某些沉积相带特殊的地质背景，另外，硅质岩本身就是一种生物岩，对探讨生物成岩、成矿作用有重要意义。所以对硅岩建造及其内硅质岩研究具有十分重要的理论意义和实用价值。因此，本论文选择扬子地块周边寒武系（南秦岭紫阳硒富集区）、二叠系（湖北恩施双河渔塘坝硒矿床）富硒硅岩建造为研究对象。通过岩石地球化学、同位素地球化学、矿物学以及流体包裹体等方法从含硒规律、岩石成因、沉积环境、成矿流体性质等方面，分别对对两个不同时代或不同层位的富硒硅岩建造开展了系统的地球化学对比研究；并从矿物学、包裹体成分及物理化学条件等方面对渔塘坝硒矿床的成因作了探讨。通过研究，取得了以下主要认识：1渔塘坝硒矿区和紫阳硒富集区富硒硅岩建造岩石以硅质岩为主，硅质岩中5102含量范围分别为64.2％-95.84％和63.62％-95.24％。同时包括部分碳质硅质岩丫碳质页岩 和碳、硅板岩及含腐泥层的石煤；渔塘坝硒矿床硅质岩中Se含量大于80ug/g的样品均采自下二叠统茅口组的硅质岩段内，紫阳下寒武统硒富集体中硅质岩中硒的含量最高（可达278ppm）。2微量元素研究表明，两地区富硒硅质岩中均含有较高的Cu，Ni、V、As、Sb、Cr，且U／Th＞1。在U-Th、Zr-Cr和P2O5-Y相关图以及Fe-Mn-（Cu+Co+Ni）三角图上，两研究区内硅质岩样品点均落于热水沉积区。渔塘坝硒矿区硅质岩的REE总量较低，平均为38.9×10-6，紫阳硒富集区硅质岩REE总量除个别较高（达110×10-6以上）外，总体也较低（12.0-37.6）×l0-6；另外，从稀土元素配分模式看，两地区硅质岩均有较明显的Ce负异常，且Eu从无明显Eu异常到出现正Eu异常。都反映出热水沉积硅质岩的特征。从si和O同位素组成来看，两个地区硅质岩的δ3051和δ18O值也总体位于热水成因硅质岩区域内。根据隧石一水的氧同位素分馏方程计算得知，两研究区硅质岩的形成温度分别为46℃-72℃和78.6℃-126.20℃。地球化学特征表明，两地区富硒硅质岩均来自热水沉积作用。另外，渔塘坝硒矿区硅质岩中Cr含量较高，且存在腕足类生物化石；紫阳硒富集区硅质岩中Ba及有机质含量较高，且存在叶琳生物标志化合物。结合两地区碳同位素组成特征（渔塘坝地区δ13c为正值，可能和上扬子区早、晚二叠世之间多期次喷发的火山活动，造成地球史上二叠纪生物大灭绝有关；紫阳地区δ13C为负值，说明碳同位素来源于沉积有机物质），暗示两地区硅质岩的成因可能与火山沉积作用有关，且在成岩过程中有部分生物的参与。3渔塘坝赋矿硅质岩硫同位素组成具有较高的负值，表明矿床形成于缺氧的海盆内：紫阳硒富集区形成黄铁矿的硫主要来自海水硫酸盐。4系统研究了渔塘坝硒矿区硒的矿物学，显示硒以自然硒、独立矿物、类质同像及有机吸附四种形式赋存于矿床中。废弃石煤堆中的自然硒矿物，是自然因素和人为活动共同干预的结果，并非石煤的缓慢自燃的结果。5对研究区成矿流体中包裹体均一温度、盐度和密度进行了系统研究，结果显示：两地区的流体包裹体以原生包裹体为主，数量较多且形态复杂；研究区（渔塘坝硒矿和紫阳硒富集区）成矿流体处于中一低温（ 190-250）℃和（120-155）℃条件。渔塘坝硒矿区石英和方解石包裹体内的流体盐度分别为（5.9-10.l）B％和（3.9-4.5）WB％，紫阳硒富集区流体盐度为（1.2-2.8）WB％，后者流体盐度明显低于前者。流体密度经计算分别为0.79-0.79／cm3和0.69-0.969／cm3。重点对渔塘坝硒矿区的石英和方解石包裹体进行了拉曼光谱成分测试，结果显示：包裹体成分以H2O和N2为主，含少量 CH4、C2H4、C2H6、C3H5、C4H6、C4H4和C6H6等成分，说明成矿溶液介质主要为具有还原性质的水溶液，其成矿条件具还原性的特点。6渔塘坝硒矿区成矿物理化学条件的研究表明，即富硒成矿流体为中低温（190-250）℃、压力平均为60Mpa。成矿早期02、eZ相对较低，乃较高，且fS2/fSe2＞l，有利于硫化物沉淀在成矿主阶段，随着硫化物的沉淀，fS2和fSe2相应增大，且fO2较高。高的fO2阻止了硒进入硫化物，而有利于硒化物的形成。 7系统研究了富硒硅岩建造的沉积环境和构造环境特征，认为渔塘坝硒矿床中富硒硅质岩主要形成于浅海滞留的盆地沉积环境，紫阳下寒武统硅质岩沉积环境属于深水滞留沉积环境；渔塘坝硒矿床主要形成于拉张的断陷盆地中，紫阳硒富集体则形成于拉张的裂谷环境。