含氘电极真空弧等离子体空间分布特性诊断研究

真空弧放电等离子体含有多种离子成分,并且各离子在空间上具有不同的分布规律.本文针对金属氘化物电极真空弧离子源,搭建了一台紧凑型磁分析装置,用来研究放电等离子体中氘离子与金属离子的空间分布.当离子源弧流为100 A左右时,该装置能有效地传输引出束流,并且具有较好的二次电子抑制效果,可准确获得各离子流强.利用该装置测量并获得了氘化钛含氘电极真空弧放电等离子体内氘离子和钛离子空间分布规律,结果表明:径向上,氘离子和钛离子都呈高斯分布,但氘离子分布均匀,而钛离子相对集中在轴线附近,导致轴线附近氘离子比例最低;轴向上,所有离子数量都以自然指数函数减少,而且相对幅度接近,所以氘离子比例几乎不变.本文研究结果不仅有助于理解真空弧放电等离子体膨胀过程,还可以指导金属氘化物电极真空弧离子源及其引出设计.     

Synthesis and Crystal Structure of Methyl 3-（5- Bromo-1-ethyl-1H-indole-3-carbonyl）aminopropionate

Methyl 3-(5-bromo-1-ethyl-1H-indole-3-carbonyl)aminopropionate has been syn-thesized by the acylation of 5-bromo-3-trichloroacetylindole with β-alanine methyl ester,followed by alkylation with ethyl iodide,in 82.6% yield.Its crystal structure was gotten and determined by X-ray diffraction method.The crystal is of monoclinic,space group P2 1 /c with a=11.7927(8),b=14.9342(8),c=9.0060(5),β=101.558(6)°,V=1553.93(16)3,Z=4,D c=1.510 g/cm 3,λ=0.71073,μ(MoKα)=2.656 mm-1,M r=353.22 and F(000)=720.The structure was refined to R=0.0401 and wR=0.0825 for 1704 observed reflections with I > 2σ(I).In the crystal structure,intermolecular N(2)-H(2)···O(1) hydrogen bond and weak intermolecular bonds (C(1)-H(1) O(1) and C(10)-H(10B) O(2)) are formed,and π-π stacking also exists.     

新体系Fe（Ⅲ）－KIO＿4－偶氮氯磷Ⅲ催化动力学光度法测定食品中痕量铁的研究

研究了在硫酸介质中，痕量Ｆｅ（Ⅲ）催化高碘酸钾氧化氨氯磷Ⅲ的褪色反应及其动力学条件。本法检测限为８．７８×１０￣（０９）ｇ／Ｌ，测Ｆｅ（Ⅲ）范围０～１．４μｇ／１０ｍＬ，采用硫基葡聚糖凝胶分离富集，使本法选择性大大提高，建立了一种高灵敏、高选择性测定痕量Ｆｅ（Ⅲ）的新方法，用于食品中痕量Ｆｅ（Ⅲ）的测定，结果满意。     

Mode Transition of Vacuum Arc Discharge and Its Effect on Ion Current

The mode transition of a pulsed vacuum arc discharge, which is from vacuum surface flashover to non-surface vacuum breakdown or vice versa, is studied by simply adjusting a trigger resistor. This approach provides a possibility to research the transition discharge process. Since the transition process is smooth and controllable, the transition mechanism and its effect on the performance of an ion source can be investigated via various diagnosis experiments. The experimental results show that the mode transition occurs when the resistance is in the range of 0- 10Ω. With the mode transition from surface flashover to non-surface vacuum breakdown, the vacuum arc discharge becomes more intense and the ion current produced by the Ti cathode ion source increases by two times. The related physical mechanism is also discussed in detail.     

真空弧放电TiH合金阴极表面形貌分析

TiH合金电极是一种含氢量非常高的金属材料,用它作真空弧离子源的电极,可在真空环境下产生强度非常高的氢离子流。相比纯金属材料电极,TiH电极除了出现真空弧放电特有的融蚀现象外,还存在气体释放过程,所以它的表面形貌具有一定的独特性。利用扫描电子显微镜观察了单次放电和多次放电后阴极表面形貌,发现阴极斑在阴极表面微裂纹附近连续分布,气体释放生成很多小孔,使阴极斑区域呈絮状结构;弧流越大,阴极斑数量越多;多次放电后,阴极斑朝含氢量多的地方移动。该结果有助于了解含氢电极的真空弧放电过程,对该类放电的应用具有一定参考意义。