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1.
The application of the Lorentzian plasma theory for the calculation of the properties of multicomponent electric arc plasma is considered. It is shown that this model gives satisfactory results in the temperature range, which is corresponding to the weakly ionized arc plasma and arc plasma with dominant first ionization. The calculations are provided for the arc plasmas of noble gases and their mixtures between them and also that with metals. It is also pointed that the discrepancy between the electron temperature and gas temperature can be significant even at relatively weak electric fields, that fact must be taken into account under the simulation of arc discharges.  相似文献   

2.
In this paper the influence of a radial instreaming gas on electric arcs is investigated. An axial or an azimuthal mass flow may be superimposed to the radial one. Using the basic equations of the single-fluid model of plasma physics the important properties and parameter dependences are numerically calculated and discussed. The results are compared with those of a corresponding arc without an instreaming radial mass flow. Using an arc heater with radial mass flow it is possible to reach much higher axis temperatures and enthalpy densities. Choosing a set of well selected working conditions nearly the whole electric input may be transformed into axial enthalpy flux of the gas to be heated. The paper illustrates the mutual interaction between the dynamic and thermic functions of an electric arc.  相似文献   

3.
Experimental investigation of an electric arc stabilized by a water vortex was carried out in a DC arc plasma torch for the power range 90-200 kW. Volt-ampere characteristics of the arc as well as the power balance were determined separately for the part of the arc column stabilized by water and for the remaining part between the nozzle exit and the external anode. The temperature of arc plasma close to the nozzle exit was determined by emission spectroscopy. Negatively biased electric probes in the ion collecting regime were used for determination of the plasma flow velocity. The measured temperatures up to 27000 K, and velocities up to 7 km/s are higher than the values commonly reported for plasma torches with DC arcs stabilized by a gas flow. Mass and energy balances within the arc chamber were determined from the experimental results. The radial transport of the energy by radiation was identified as a decisive process controlling the arc and plasma properties. The balance of radial energy transport was studied. The ratio of energy spent for evaporation of the water to the energy absorbed in the evaporated mass is very low in the water stabilized arc. This is the principal cause of high plasma temperatures and velocities found by the measurements  相似文献   

4.
Experiments have been performed to demonstrate the influence of the location of the electric power connection to the anode nozzle on the efficiency of DC plasma torches. The DC plasma torch used in these experiments offers the flexibility to work with different anode geometries and the possibility of connecting the electrical power to the anode at two different locations. For each set of experiments, the controllable parameters such as total gas flow rate, gas composition, and electric current were kept constant, changing only the location of the electrical connection to the anode nozzle. The efficiency of the torch, derived from a conventional energy balance, shows a significant change as the location of the electrical connection to the anode nozzle is changed. The measured mean voltage as well as the amplitude of the voltage fluctuations were also affected by the location of the electrical connection to the anode nozzle. An explanation for the arc behavior is given, based on an analysis of the forces acting on the anode arc column and their influeuce on the variation of the arc column length. Experimental data are in good agreement with analytical predictions  相似文献   

5.
Simple solutions of 1Dt gas-dynamical equations based on similarity analysis are possible for the gas surrounding a point source of mass and energy such as an electrode (cathode) arc spot. To obtain nontrivial (non-zero temperature) solutions throughout, two-scale formulation is used that permits an additional boundary condition near the source. Three generalised gas flow variables, R, Z and V, related to gas density, temperature and velocity are calculated and presented as functions of a single similarity parameter, λ, related to position and time. The computational results are compared with data from two gas discharge experiments: on gas disturbances due to an electric arc of micrometer length in atmospheric air and on expansion of a metal-vapour plasma cloud generated by a low-pressure cold-cathode arc.  相似文献   

6.
Contrarily to well known cylindrical, whirl-stabilized electric arcs with rotating walls or with nearly tangential gas inlets, we discuss a new geometry of an electric arc for producing a whirl around the axis. These investigations have been performed for transferring the theory to a torus arc in a similar way. By using a numerically calculated temperature distribution the hydrodynamic properties are studied taking into consideration the single-fluid model of plasma physics. The results are compared with our experiments and those of other institutes. They agree well and give hope to a stabilizing effect for an electric arc of this geometry. The analytical distributions of the velocities and the pressure are calculated on the basis of perturbation theory. The results are applied to a nitrogen arc at a pressure of one atmosphere and for a definite set of parameters.  相似文献   

7.
An electric arc quickly moved magnetically forms a closed plasma cone or plasma ring between two concentrically arranged electrodes. Aerosols and suspended matters can be brought into the plasma in an optimum manner with a little carrier gas flow, and can be excited to emission. The dates applied and attained till now are: Arc current 5…?20 A, magnetic field strength 104…?4 · 105 A/m, magnetic induction 0.1…?0.3 T, rotation frequency 8…?15 kc, carrier gas air or argon maximum flow 0.5 1/min, intensity increase for CuI-lines up to factor 100. Further applications are possible for special lamps and electric arc diagnostics.  相似文献   

8.
In this paper the analysis of gas heating phenomena in wallstabilized toroidal electric arcs is derived and the results are applied to a nitrogen arc at a pressure of one atmosphere. These investigations have been performed on the basis of the single-fluid model of plasma physics taking into consideration the thermal properties of the wall material. By using a differential method it is outlined how the equation of energy is solved not only in the arc but also in the wall.  相似文献   

9.
Plasma generation for the plasma cutting process   总被引:1,自引:0,他引:1  
This study is an attempt to estimate the overall properties, viz. the thermal power and force, of an intense plasma jet produced by a plasma cutting torch, and to relate the properties of the plasma to the diameter of the nozzle of the plasma torch and the flow rate of plasma-forming gas. For cutting metallic plates using a thermal plasma, a narrow plasma jet is produced by means of a transferred electric are between an electrode in a plasma torch and the material to be cut. The power density and pressure exerted by the plasma jet on the material at the region of cut needs to be high so that a straight cut, without dress at the bottom of the plate, can be obtained. A simple theory to describe the behavior of the arc in a plasma cutting torch has been developed to predict the are radius, pressure, and arc voltage at the nozzle exit as a function of are current for a range of nozzle sizes and air flow rates. The results obtained are in good agreement with the measured values for an air plasma cutting torch nominally rated for 100-A operation. The relationships between the mass flow rate of plasma gas, plasma power, and arc force have been discussed in the light of design of plasma torches for plasma cutting  相似文献   

10.
采用气液滑动弧放电非平衡等离子体进行降解高浓度苯酚模拟废水(初始浓度为872 mg/L)的研究。实验研究表明:由于液滴的存在改变了电极间的介电常数和局部电场,气液滑动弧放电的电压波形比纯气流滑动弧放电更加不规则,起弧电压更低;采用氧气作为载气能提高苯酚的降解效果,最后TOC值为44 mg/L;增大气液混合比,相应的加强了废水的雾化效果,增大水气接触表面积,进而提高了苯酚的降解效果;在尾气中检测到CO2的存在,最高浓度达到35357 mg/m3。  相似文献   

11.
滑动弧低温等离子体放电特性的数值模拟研究   总被引:1,自引:0,他引:1       下载免费PDF全文
汪宇  李晓东  余量  严建华 《物理学报》2011,60(3):35203-035203
滑动弧等离子体的电弧温度场、电场和导电区域尺寸是确定电子温度、电子密度、化学反应速率以及能量效率的重要参数.对气流量为1.43 L/min和6.42 L/min时50 Hz交流滑动弧放电的电参数进行了测量;用瞬态的电弧模型描述滑动弧的能量传递,并用近似的介质电导率和热扩散系数对模型进行简化,解决了由于电弧结构变化所导致的移动边界问题;模拟求得等离子体的电弧结构、电场强度和动态温度场等参数的演化.其中,电弧电场的模拟值与实验值基本符合,计算得到电弧轴心温度可以达到5700—6700 K.研究结果表明,气流直 关键词: 滑动弧等离子体 温度场 电场强度 导电半径  相似文献   

12.
Based on the phase state reconstruction of welding current in short-circuiting gas metal arc welding using carbon dioxide as shielding gas, the approximate entropy of welding current as well as its standard deviation has been calculated and analysed to investigate their relation with the stability of electric arc and welding process. The extensive experimental and calculated results show that the approximate entropy of welding current is significantly and positively correlated with arc and welding process stability, whereas its standard deviation is correlated with them negatively. A larger approximate entropy and a smaller standard deviation imply a more stable arc and welding process, and vice versa. As a result, the approximate entropy of welding current promises well in assessing and quantifying the stability of electric arc and welding process in short-circuiting gas metal arc welding.  相似文献   

13.
Low-power laser/arc hybrid welding process of magnesium alloy shows that the weld capability of tungsten-inert-gas arc is improved under the action of laser pulses. The effect of laser pulse on arc plasma is analyzed by studying the plasma spectra, plasma shapes, and arc voltage in this paper. On the one hand, laser pulse attracts arc plasma to laser keyhole and improves the stability of arc plasma; on the other hand, laser pulse expands the arc plasma and concentrates the electric conducting route of arc plasma. All these increase the output power and energy density of arc plasma, so the welding penetration is improved. In addition, laser pulses are controlled to act on the negative wave of alternating-current arc (the target metal has negative polarity) in hybrid welding process to improve the stability of arc plasma and weld penetration.   相似文献   

14.
Plasma of electric arc discharge between melted electrodes was experimentally investigated. Diagnostics of electric arc plasma was carried out. Optical emission and absorption spectroscopy was used to obtain radial profiles of temperature, electron density and neutral atoms concentration. The influence of electrode condition on plasma parameters was evaluated. It was found that the copper vapour in plasma tends to be located at the arc axis.  相似文献   

15.
This paper deals with investigations of thermal electric arc plasma in complex gas - metal vapour mixtures. Experimental techniques in the diagnostic were widely discussed. The study of non-steady-state discharges was performed with an appropriate temporal and spatial resolution. Spectroscopy investigations of plasma parameters in some modes of discharge operation were carried out. Spatial profiles of temperatures and electron densities were obtained. Plasma composition was calculated in an assumption of the local thermodynamic equilibrium. The influence of some mechanisms on plasma condition was analysed.  相似文献   

16.
The unipolar arc model is described. Experimental proof that unipolar arcing represents a discharge form which easily leads to explosive plasma formation is provided. Using a laser-produced plasma, it has been demonstrated that unipolar arcs ignite and burn on a nanosecond time scale without any external electric field being applied. Similar unipolar arc craters have been observed on the cathode surface of a pulsed vacuum diode with an externally applied field of 0.5 MV/cm. The experimental results show that cathode spots are formed by unipolar arching. The localized buildup of plasma above an electron-emitting spot naturally leads to a pressure gradient and electric field distribution which drives the unipolar arc. The high current density of a unipolar arc provides explosive plasma formation  相似文献   

17.
Microparticles with sizes up to 130 μm have been confined and the velocity and diameter of particles in a plasma trap of an rf magnetron discharge with an arc magnetic field have been simultaneously measured. The motion of the gas induced by electron and ion cyclotron currents has been numerically simulated using the Navier-Stokes equation. The experimental and numerical results confirm the mechanism of the orbital motion of dust particles in the magnetron discharge plasma that is associated with the orbital motion of the neutral gas accelerated by electron and ion drift flows in crossed electric and magnetic fields.  相似文献   

18.
Plasma jets from conventional non‐transferred arc plasma devices are usually operated in turbulent flows at atmospheric pressure. In this paper, a novel non‐transferred arc plasma device with multiple cathodes is introduced to produce long, laminar plasma jets at atmospheric pressure. A pure helium atmosphere is used to produce a laminar plasma jet with a maximum length of >60 cm. The influence of gas components, arc currents, anode nozzle diameter, and gas flow rate on the jet characteristics is experimentally studied. The results reveal that the length of the plasma jet increases with increasing helium content and arc current but decreases with increasing nozzle diameter. As the gas flow rate increases, the length of the plasma jet initially increases and then decreases. Accordingly, the plasma jet is transformed from a laminar state to a transitional state and finally to a turbulent state. Furthermore, the anode arc root behaviours corresponding to different plasma jet flows are studied. In conclusion, the multiple stationary arc roots that exist on the anode just inside the nozzle entrance are favourable for the generation of a laminar plasma jet in this device.  相似文献   

19.
焊接电弧等离子体的物理特性直接决定了焊接接头的成形形貌,分析双组分保护气体的脉冲钨极惰性气体保护焊(P-TIG)动态电弧物理特性,为深入开展混合气体保护焊的焊缝成形物理过程研究提供理论基础。氩-氮混合气体保护焊电弧具有高热特性可以增加熔深,但在焊接前混合均匀的保护气体,引弧后气体浓度会重新分布,使电弧等离子体物理特性的实时动态变化特点变得复杂。光谱诊断是电弧等离子体物理特性测量的最重要手段,但对双组分气体保护的P-TIG焊电弧特性的研究仍需深入进行,特别是对于易引起缺陷的起弧过程,其动态物理特性亟需深入分析。针对氩-氮混合气体P-TIG焊的引弧过程,以P-TIG焊产生的氩-氮双组分电弧等离子体为研究对象,提出利用窄带滤光片与CCD相结合的高速摄影实验系统采集双组分电弧等离子的动态光谱信息,获取特征谱Ar Ⅰ 794.8 nm和N Ⅰ 904.6 nm的P-TIG焊电弧光谱强度动态分布;提出利用双元素双组分标准温度法计算P-TIG焊引弧过程中距离钨极下方1,2,3和4 mm位置处电弧等离子体的动态温度及浓度,定量分析80%Ar+20%N2保护的P-TIG焊从引弧至电弧稳定过程的电弧等离子体物理特性实时分布。实验结果表明,80%Ar+20%N2保护的P-TIG焊电弧强度、电弧温度及浓度的变化均与脉冲电流的变化同步,焊接电流在3 ms内达到稳定状态,而电弧等离子体的强度、温度及浓度需要更长时间达到平衡状态。从起弧到电弧等离子稳定燃烧的过程中,基值期间和峰值期间的电弧等离子体强度均呈现先升高再降低的趋势;由于阴极的热传导及电流密度的变化,使得电弧等离子体轴向位置的峰值温度及基值温度均出现迅速升高再缓慢降低的现象;由于粒子间碰撞及摩擦力的影响,使得电弧等离子体的峰值及基值期间氩的浓度均呈迅速减小再缓慢增加的趋势,且氩的浓度均低于焊前浓度。  相似文献   

20.
直流纯氩层流等离子体射流的长度变化   总被引:9,自引:0,他引:9  
采用主要由阴极、阳极以及介于阴极和阳极之间的中间段组成的直流非转移式电弧等离子体发生器,在大气压条件下,比较系统地研究了纯氩层流等离子体射流的长度随着弧电流、气体流量以及发生器结构而变化的规律。结果表明:层流射流的长度随弧电流和工作气流量的增加而增长;层流向湍流流动转变的临界气流量值随弧电流增大而提高;在发生器的伏安特性呈大梯度变化的情况下,射流长度随弧电流的变化幅度增大。  相似文献   

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