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1.
纳秒脉冲气体放电机理探讨   总被引:7,自引:3,他引:4  
 经典Townsend机理和流注理论是气体放电研究的基础,但在解释纳秒脉冲气体放电时均存在一定缺陷。基于经典气体放电理论,探讨纳秒脉冲气体放电机理,分析流注理论判据在纳秒脉冲气体放电中的有效性,解释纳秒脉冲下电子逃逸现象和基于电子逃逸的快速电离波击穿理论,仿真计算高能快电子的逃逸过程。结果认为基于高能量快电子的逃逸击穿将是可能解释纳秒脉冲下气体放电现象的依据。  相似文献   

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In this work, an analytical model is used to study the formation of the anodic streamer in high pressure electrical discharge. This model enabled us to see the space variations of the characteristics of the streamer such as the electric field and the propagation velocity of streamer. The validity of the analytic approach is demonstrated by comparing the model results to the data from the literature. A qualitative concord was found. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

3.
温嘉烨  王亚桢  肖正光  王骏东  李元  张冠军 《强激光与粒子束》2024,36(10):105003-1-105003-10
水中流注放电为击穿前放电通道起始与发展的关键过程,但由于涉及物理机制较为复杂且尚不明确,制约了水中放电应用效率的提升。探究了水中正极性丝状流注放电的模式转化特性、重燃特性与分叉特性,明确了通道界面沉积电荷与空间电荷分布对流注发展过程的影响。研究结果表明,水中正极性放电可分为第一类与第二类丝状流注,流注模式转化特性受气液界面电荷弛豫过程影响较大。当外施电压达到加速电压时,第一类流注迅速转化为第二类流注。第一类丝状流注通道内电离形成、熄灭及重燃过程与通道内部电场及气/液界面电荷密度关系密切。第二类丝状流注通道空间电荷分布受电压上升沿与电极表面结构影响较大。电压上升沿时间越长,主通道头部电荷密度与电场强度越低,通道发展速度随之降低。随电极表面微凸结构半径增大,流注分叉点位置将电极表面过渡为主通道根部。受主通道空间电荷分布影响,分支通道发展速度在微凸结构半径为5 μm时呈现先降后升趋势。  相似文献   

4.
The aim of this work is to report the achievement of a light weight, compact, high power CO2 laser which can be used in industry. The construction and operation of a CO2 gas transport laser with cylindrical geometry and two parallel electrical discharges are presented. Using a 600 mm diameter, 1400 mm length, 250 kg laser head, we have obtained more than 1.6 kW laser power with 2% stability and 2 mrad full angle divergence. For comparison the results are presented for one electrical discharge laser.  相似文献   

5.
利用微机电系统(MEMS)工艺制备了5~40 m间隙的金属铝薄膜电极,测取了不同间隙下施加纳秒方波脉冲时的击穿电压,得到击穿电压和平均场强随电极间隙的变化规律,研究了脉宽、极性对击穿电压的影响,结合击穿后微电极扫描电镜观察结果讨论了其击穿机理,并与相同试样在直流下的结果进行了对比。研究表明:击穿电压随微间隙距离的增大而增大,击穿场强则随着间隙的增大迅速减小;与直流同间隙的击穿电压相比,脉冲作用下的击穿电压并不像宏观尺度下那样高出很多;试样击穿机理应为流注理论。在脉冲作用下,阳极出现了分层熔化现象,由于作用时间很短,阳极表面并未出现类似于直流击穿时留下的坑洞;阴极则出现了溅射沉积现象,只是沉积物质相对较少。  相似文献   

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7.
郭风祥  吕婷  贾燕  田学雷 《物理学报》2011,60(7):77204-077204
根据费米面实验数据修正Behari关于液态铅的模型赝势,构建新的模型赝势,结合实验结构因子及硬球结构因子,计算不同温度下液态铅的电阻率,计算结果与实验数据较为符合,并对计算过程中的误差及模型赝势的适用性进行了分析.关键词:电阻率计算电子输运液态铅模型赝势  相似文献   

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This paper highlights the electrical properties of two new complex tungsten bronze ceramics (K2Pb2Eu2W2Ti4Nb4O30 and K2Pb2Pr2W2Ti4Nb4O30) which were prepared by high temperature mixed oxide method. Variation of impedance parameters with temperature (27–500 °C) and frequency (1 kHz to 5 MHz) shows the grain and grain boundary effects in the samples. The variation of dielectric parameters with frequency is also studied. The ac conductivity variation with temperature clearly exhibits that the materials have thermally activated transport properties of Arrhenius type.  相似文献   

10.
利用微机电系统(MEMS)工艺制备了5~40 m间隙的金属铝薄膜电极,测取了不同间隙下施加纳秒方波脉冲时的击穿电压,得到击穿电压和平均场强随电极间隙的变化规律,研究了脉宽、极性对击穿电压的影响,结合击穿后微电极扫描电镜观察结果讨论了其击穿机理,并与相同试样在直流下的结果进行了对比。研究表明:击穿电压随微间隙距离的增大而增大,击穿场强则随着间隙的增大迅速减小;与直流同间隙的击穿电压相比,脉冲作用下的击穿电压并不像宏观尺度下那样高出很多;试样击穿机理应为流注理论。在脉冲作用下,阳极出现了分层熔化现象,由于作用时间很短,阳极表面并未出现类似于直流击穿时留下的坑洞;阴极则出现了溅射沉积现象,只是沉积物质相对较少。  相似文献   

11.
    
Producing alloy nanoparticles by discharge‐assisted erosion of electrodes immersed in liquid nitrogen is possible in the cobalt–nickel system. Several electrode configurations are tested. When one nickel electrode faces one cobalt electrode, CoxNi1−x alloy nanoparticles are produced with nickel cubic nanoparticles and cobalt round‐shaped faceted nanoparticles. The possibility of forming alloys is attributed to a sufficiently long residence time of both parent clusters within the discharge and to their total miscibility. It is also possible to form submicrometric CoxNi1−x alloy particles when discharges between cobalt electrodes are run in liquid nitrogen loaded with nickel nanoparticles produced in a former step. Starting by discharges between Co electrodes before Ni electrodes do not produce any alloy. The two mechanisms responsible for alloy synthesis are discussed.  相似文献   

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Summary: Experimental results obtained by emission spectroscopy on dielectric barrier discharges (DBD) in helium/air and helium/nitrogen gas mixtures are presented. The transition between the glow mode and filamentary mode of the dielectric barrier discharge was determined, and the electrical power transferred to the discharge was calculated. Dependence of the rotational temperature versus nitrogen gas‐flow rate was investigated.

Even with a peak power of 2.1 kW and a total energy of 2.3 × 10−4 J per pulse for the FD mode (in comparison to a peak power of 270 W and 5 × 10−5 J per pulse for the GD mode) the line intensity and number of excited species are larger for the GD mode than those of the FD mode.  相似文献   


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The formation of vapor layers around an electrode immersed in a conducting liquid prior to generation of a plasma discharge is studied using numerical simulations. This study quantifies and explains the effects of the electrode geometry and applied voltage pulses, as well as the electrical and thermal properties of the liquids on the temporal dynamics of the pre‐breakdown conditions in the vapor layer. This model agrees well with experimental data, in particular, the time needed to reach the electrical breakdown threshold. Because the time needed for discharge ignition can be accurately predicted from the model, the parameters such as the pulse shape, voltage, and electrode configuration can be optimized under different liquid conditions, which facilitates a faster and more energy‐efficient plasma generation.

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14.
设计了液体介质快脉冲击穿试验装置和电压电流测量系统,研究了重复频率、电极形状及电极间距与介质击穿场强、击穿电压和击穿时延等击穿特性参数的关系,比较了变压器油、十二烷基苯、蓖麻油三种典型液体绝缘介质在直流及快脉冲电压作用下的绝缘性能。结果表明:短脉冲持续时间下液体绝缘材料有异常高的击穿场强;重复脉冲串作用下的击穿场强比单个脉冲下明显减小,重复频率2 kHz时击穿场强减小了约30%;电极头半径大小对击穿也有影响,半径R=5 mm时,击穿电压最高;击穿时延随击穿场强减小而变长,在其他条件相同的情况下,测得击穿时延随机波动;蓖麻油的快脉冲电压绝缘性能最好,变压器油次之。  相似文献   

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Emission spectra of microwave discharge in liquid hydrocarbons (hexane (C6H14), n‐heptane (С7Н16), decane (С10Н22), pentadecane (C15H32), cyclohexane (С6Н12), toluene (С6Н5–СН3), ortho‐xylene (С6Н5–(СН3)2), and petroleum solvent nefras S2 80/120 [mixture of light hydrocarbons with boiling temperature ranging between 33°C and 205°C]) were studied in the range of wavelength 200–700 nm. The pressure above the surface of the liquid was equal to the atmospheric pressure. It was shown that in the spectra measured in aromatic hydrocarbons (toluene and ortho‐xylene) the sequence of the Swan band with = 0 was overlapped with the molecular emission band with a maximum at 511 nm never observed before. Analysis of known data allowed us to hypothesize that this emission can be attributed to the emission of linear carbon cluster C5 . This cluster was previously observed only in absorption. Rotational temperatures determined by modeling of the sequence Δυ = −1 of the Swan band were equal to 2,000 ± 300 K for all studied hydrocarbons.  相似文献   

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Understanding the mechanism of plasma build‐up in vacuum arcs is essential in many fields of physics. A one‐dimensional particle‐in‐cell computer simulation model is presented, which models the plasma developing from a field emitter tip under electrical breakdown conditions, taking into account the relevant physical phenomena. As a starting point, only an external electric field and an initial enhancement factor of the tip are assumed. General requirements for plasma formation have been identified and formulated in terms of the initial local field and a critical neutral density. The dependence of plasma build‐up on tip melting current, the evaporation rate of neutrals and external circuit time constant has been investigated for copper and simulations imply that arcing involves melting currents around 0.5–1 A/μm2, evaporation of neutrals to electron field emission ratios in the regime 0.01 – 0.05, plasma build‐up timescales in the order of ~ 1 – 10 ns and two different regimes depending on initial conditions, one producing an arc plasma, the other one not. Also the influence of the initial field enhancement factor and the external electric field required for ignition has been explored, and results are consistent with the experimentally measured local field value of ~ 10 GV/m for copper (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

17.
水中流光放电是研究水中放电基本物理、化学过程的主要研究对象.本文利用四分幅超高速相机、采用针-板电极结构、在20—800μS/cm水电导率范围内研究了水中微秒脉冲流光放电流光丝的再发光和暂停行为,探讨了高水电导率下观测不到流光丝的再发光的原因.结果发现:再发光在不同的流光丝之间交替发生并存在两种模式:一种为整根丝熄灭后再发光;一种为只有先端部分发光熄灭随后恢复发光.随着水电导率的增大,观测到流光丝的再发光现象的频度急剧减小, 540μS/cm水电导率时降到零;在20—800μS/cm水电导率条件下都可观测到流光丝伴生冲击波串分段现象,冲击波串分段现象的出现频度在65%以上,表明在20—800μS/cm水电导率条件下流光丝的暂停是一种普遍行为.通过测量两段冲击波的半径差得到流光的暂停时间平均为157 ns,几乎不受水电导率的影响;随着水电导率的增大,流光丝的发光强度显著增大,水电导率大于350μS/cm时,流光丝暂停期间内流光丝的光强度无法衰减到相机分辨水平以下,在相机获得的发光图像上看上去是持续发光的,难以分辨出流光丝\"熄灭-再发光\"过程.  相似文献   

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The field-emission–related effects play a significant role in the deviation of the breakdown voltage from that predicted by Paschen's law in the range of micrometer gaps. Beginning from a certain gap spacing, breakdown voltage diverges from the climbing curve seen in the left half of the Paschen curve. In this paper, the equation governing the DC breakdown in microgaps has been solved analytically. The derived analytical relation indicates that the DC breakdown voltage in microgaps depends on the gap size d and the pressure p, particularly, rather than on the product pd. The new theoretical expression allows key features to be identified suggesting that the inclusion of the field emission at micron and submicron gaps is necessary to describe properly the experimental data. The expression presented here can receive a wider interest due to its applicability to the breakdown voltage for a series of gases, gaps and pressures and can serve as ready-to-use guidelines for system engineers and designers.https://doi.org/10.1209/0295-5075/83/25001  相似文献   

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