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在对化学振荡的研究中,无论是溶液均相氧化还原形成的振荡反应,还是界面扩散受阻形成的界面振荡,都普遍采取各种电极法来监测。前文[1,2]研究了各种不同电极监测液膜振荡的变化,本文将讨论不同的电极方法在监测盐水振荡现象过程中的新发现。1970年,地球物理学家Martin[3]发现把 相似文献
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阴极表面温度是真空弧等离子体放电过程中一个重要参数,对真空弧等离子体的形成、电极腐蚀预测、热传导以及离子源的寿命都有重要影响。真空弧离子源的阴极具有目标小,放电过程快等特点,其温度的测量,对于时间分辨率和空间分辨率要求都很高,阴极表面温度的测量技术的欠缺,使得仅靠理论解析获得的结果难以得到验证。并且等离子体放电过程中测量仪器极易受到弧光的影响,如何避免放电过程中等离子体的辐射也是采用辐射法测量阴极表面温度要考虑的问题。这无疑给其温度场的测试研究带来困难。针对脉冲真空弧等离子体开展阴极表面温度测试实验有着重要意义,在分析了真空弧等离子体放电特性以及背景辐射特性和等离子体放电阴极测温的实际需求,本文基于高速CCD相机研制了一种新型的多光谱高温计。该高温计采用单色高速CCD相机,主要避免RGB彩色相机不能完全滤除背景辐射的弧光。为使用单色CCD相机实现多光谱辐射测温,设计了高温计的光学系统,该系统采用4孔径分光系统。将4种不同波长的滤光片嵌入到1个滤光片中。该研究设计的高温计可用于2 000~6 000 K的等离子体温度测量。并在中国工程物理研究院电子工程研究所进行现场测试,测试过程中将研制的高温计,通过外部触发形式对等离子体放电过程进行跟踪拍摄,高温计完全拍摄到等离子体放电过程。利用真空弧等离子体金属电极阴极放电的实测数据对高温计进行了验证。实验结果表明,设计的新型多光谱高温计能够用于测量真空弧等离子体放电时阴极温度场信息,测量的温度值低于放电电极的沸点温度,与等离子体放电过程中出现气化现象相符,说明高温计测的是等离子体放电阴极的温度。 相似文献
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本文讨论了不同的预处理对Pt电极 pH 响应的影响 。经阴极 极 化或火焰上红热后, Pt电极以Pt(OH)2+Ze-Pt+2OH响应溶液的pH。而经+1.5V(vs.SCE)阳极极化后, 由于Pt电极表面PtO2的快速分解,电极的电位值很快下降, 并逐渐达到稳定值, 稳定后的Pt电极仍以上式响应溶液的pH。用KMnO4溶液浸泡后, Pt电极表面有MnO~2沉积, 并以MnO2+4H^++Ze-Mn^2^++2H2O(PH2-7)ZMnO2+2H^++Ze-Mn2O3+H2O(PH8-12)响应溶液的pH。 相似文献
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金属电极上中和滴定的研究(Ⅰ)——零电流示波双电位滴定法 总被引:4,自引:0,他引:4
研究了在Hg(Ag)、Pt、Sb、W4种金属电极上的零电流示波双电位中和滴定法。从阳极极化的Hg(Ag)、Pt电极和经蒸馏水浸泡的Sb、W电极中,任取两支相同或相异金属作成的一对电极皆可用于酸碱滴定;对更稀的酸碱,可用一支经阳极极化和一支未极化的电极。该法简单、准确、直观、快速。初步探讨了Cl-影响Hg(Ag)、Pt电极电位滴定曲线的机理。 相似文献
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Rui-Qiang Wang Li Sheng Liang-Bin Hu Mou Yang Baigeng Wang D. Y. Xing 《Frontiers of Physics》2014,9(4):477-482
Single-particle sequential tunneling is studied through a negative-U center hybridized with a superconducting, a ferromagnetic, and a normal metal electrodes. In stark contrast to the case of positive U, the single-particle tunneling in attractive charging energy is usually prohibited by ground states with electrons in pairs. We find a microscopic mechanism to induce single-particle sates from pair states. As a consequence, in the nonpolarized metal terminal a remarkable pure spin current with no charge currents survives over a wide range of gate- and bias- voltages, which is rather crucial for experimental observation and design of spintronic devices. In addition, a significant spin-filter effect is presented in certain bias regime. 相似文献
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The dynamical processes of the electric charge injection and transport from a metal electrode to the copolymer are investigated by using a nonadiabatic dynamic approach. The simulations are performed within the framework of an extended version of the one-dimensional Su-Schrieffer-Heeger (SSH) tight-binding model. It is found that the electric charge can be injected into the copolymer by increasing the applied voltage. For different structures of the copolymer, the critical voltage biases are different and the motion of the injected electric charge in the copolymer varies obviously. For the copolymer with a barrier-well-barrier configuration, the injected electric charge forms a wave packet due to the strong electron-lattice interaction in the barrier, then comes into the well and will be confined in it under a weak electric field. Under a medium electric field, the electric charge can go across the interface of two homopolymers and enter into the other potential barrier. For the copolymer with a well-barrier-well configuration, only under strong enough electric field can the electric charge transfer from the potential well into the barrier and ultimately reach a dynamic balance. 相似文献