涂液浓度对Ru-Ti-Ir氧化物阳极涂层性能的影响

应用热分解法制备了由不同浓度涂液形成的Ru-Ti-Ir氧化物阳极涂层,SEM,EDX,XRD、强化电解寿命、极化曲线、循环伏安和电化学阻抗等测试表明,涂液浓度对阳极涂层的表面形貌有着很大的影响,但不甚影响其析氯极化过程.随着涂液浓度的增加,阳极涂层的伏安电量和双电层电容都出现先降低后增加的变化趋势.     

X-ray structure and spectroscopic characterization of doubly-bridged binuclear copper(II) complexes in symmetric and asymmetric coordination environments

μ-1,3-Acetamide or acetate bridged, symmetric and asymmetric dicopper(II) complexes viz [Cu₂(P1-O⁻)(NHAc⁻)](ClO₄)₂ (1), [Cu₂(P2-O⁻)(OAc⁻)](ClO₄)₂ (2) and [Cu₂(P2′-O⁻)(OAc⁻)(H₂O)](ClO₄)₂ (3) were synthesized by employing classic dinucleating ligands; P1-OH, P2-OH (symmetric), and P2′-OH (asymmetric) having trivial differences in their ligand frame work. Solid state structures of these complexes were determined by X-ray crystallography. In solution, they were also characterized by various spectroscopic techniques, which includes ESI-MS, FT-IR, optical, solution magnetic moment, paramagnetic ¹H NMR and EPR. The solution magnetic moment of these complexes at room temperature suggests a weak magnetic interaction between the two Cu(II) centers.     

液相爆炸物荧光化学传感器研究进展

溶液中爆炸物的快速灵敏检测对于防恐、反恐和环境质量监测等都具有十分重要的意义。本文在介绍液相爆炸物探测用均相荧光传感器、薄膜荧光传感器和颗粒荧光传感器的基础上,简要评述了各种方法的优缺点,指出新型化学薄膜荧光传感器的开发和基于这些薄膜的低成本、多功能和高品质液相专用爆炸物探测仪的研制将成为未来液相爆炸物探测研究的一个重...     

溶液阴极辉光放电光谱信号的内标法定量分析研究

溶液阴极辉光放电-原子发射光谱是一种新颖的快速、高效、实时在线的元素分析方法,它可用于水体金属元素的检测。为提高其测量精确度和稳定性,将内标法应用于溶液阴极辉光放电-原子发射光谱技术。对K元素建立了标准定标曲线和以H_β为内标元素的定标曲线,内标法测得样品的相对误差和相对标准偏差分别为1.11%,2.14%,精确度和稳定性较之标准曲线法有一定的提高。实验考察了元素谱线强度在同一时段的波动情况,发现元素K和H_β的谱线强度变化趋势稍有不同,而同主族元素K和Rb,Ca和Mg的谱线强度有相同的变化趋势,提出选择与待测元素同主族且谱线强度变化趋势较为一致的元素作为内标元素能更大化校正实验波动的观点。同时探讨了K以Rb为内标元素、Ca以Mg为内标元素以及Mg以Ca为内标元素时的内标法测量的精确度和稳定性,得其相对误差分别为0.49%,0.02%和0.30%,相对标准偏差分别为1.11%,1.13%和0.87%,与标准曲线法和以H_β为内标元素的内标法相比效果更佳。测得自来水样品中Ca元素以Mg为内标的相对误差和相对标准偏差为0.58%,1.03%,Mg元素以Ca为内标的相对误差和相对标准偏差为1.57%和1.10%。研究结果表明,将溶液阴极辉光放电-原子发射光谱技术应用于水体金属元素检测时,内标法可以有效校正实验波动的影响,提高测量的精确度和稳定性。     

非自治竞争Lotka—Volterra系统的持续生存和全局稳定

本文研究一般ｎ个种群竞争的非自治Ｌｏｔｋａ－Ｖｏｌｔｅｒｒａ系统,得到了系统一致持续生存和全局渐近稳定的新的判别准则,这些准则推广了现有有关文献中的一些结果。     

掠入射较高功率密度驱动Ni-like AgX射线激光的理论研究

 用系列程序对掠入射方式驱动亚稳态类镍银碰撞激发机制进行了研究。继低功率密度驱动获得有效增益系数为23.8 cm^-1结果之后,在4.3×10¹³ W·cm^-2较高功率密度驱动时,增益区移到驱动激光折返点附近,有效增益系数达到40 cm^-1以上,比正入射提高了2.4倍。用50 J激光能量驱动单靶,就能达到有效增益长度积为40的深度饱和增益。     

乙醇添加剂对ICP光源等离子体辐射的增强效应

利用光电检测法,研究了含乙醇水溶液的温度在20,40和60 ℃的条件下,对电感耦合等离子体(ICP)光源发射强度、等离子体参数(激发温度和电子密度)、试液物理性质(表面张力、粘度)及雾化特性(提升量、有效提升量和雾化效率)的影响。实验结果表明,随着乙醇含量及相应溶液温度的提高,分析物进入等离子体的速率增大了,元素Zn,Fe,Mg,Si和Sr的谱线强度有明显增强,而且随着含乙醇样品溶液温度的提高,等离子体中激发能力增强了。在溶液温度为60 ℃时,元素Zn,Fe,Mg,Si和Sr的最大谱线强度比20 ℃时分别高出了55.8%,45.4%,48.9%,17.7%和21.6%,这有利于痕量元素的检测。     

Modeling of the Subsonic–Supersonic Flow and Heat Transfer in a DC Arc Plasma Torch

Two-dimensional modeling results are presented concerning the subsonic–supersonic flow and heat transfer within a DC plasma torch used for low-pressure (or soft vacuum) plasma spraying. The so-called fictitious anode method is used in the modeling in order to avoid inclusion of the complex three-dimensional effects near the anode arc root and also to avoid the forced heating of all the incoming cold gas stream by the arc. A nonorthogonal boundary-conforming grid, nonstaggered variable arrangement and the all-speed SIMPLE algorithm are employed for the solution of the governing equations, including gas viscous effects, temperature-dependent properties, and compressible effects. Good agreement of the predictions with available results for a few benchmarked compressible flow problems shows that the new version of the FAST-2D program can be employed for the present plasma flow modeling. Temperature, axial velocity, Mach number, and static pressure contours, and streamlines within the DC arc plasma torch are presented to show the flow and heat transfer characteristics. The flow transits gradually from upstream subsonic regime into downstream supersonic regime with the subsonic–supersonic transition within the cylindrical segment of the torch nozzle. Additional numerical tests show that gas viscosity and Lorentz force have only a slight effect on the plasma flow.     

无水钾镁矾类复盐(A＋)2Cd2(SO4)3的热化学

The standard molar formation enthalpies of (A＋)2Cd2(SO4)3[A＋ is NH＋ 4 or K＋] are determined from the enthalpies of dissolution (ΔsHm) of [(A＋)2SO 4(s)＋2CdSO4(s)] and (A＋)2Cd2(SO4)3(s) in twice distilled water or 3 mol•L－1 HNO3 solvent respectively,at 298.2 K,as: ΔfHm [(NH4)2Cd2(SO4)3,s,298.2K]=－3031.74±0.08 kJ•mol－1 ΔfHm [K2Cd2(SO4)3,s,298.2K]=－3305.52±0.17 kJ•mol－1     

Algebraic multigrid methods for the solution of the Navier–Stokes equations in complicated geometries

The application of standard multigrid methods for the solution of the Navier–Stokes equations in complicated domains causes problems in two ways. First, coarsening is not possible to full extent since the geometry must be resolved by the coarsest grid used. Second, for semi-implicit time-stepping schemes, robustness of the convergence rates is usually not obtained for convection–diffusion problems, especially for higher Reynolds numbers. We show that both problems can be overcome by the use of algebraic multigrid (AMG), which we apply for the solution of the pressure and momentum equations in explicit and semi-implicit time-stepping schemes. We consider the convergence rates of AMG for several model problems and demonstrate the robustiness of the proposed scheme. © 1998 John Wiley & Sons, Ltd.