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1.
王维  杨兰均  高洁  刘帅 《物理学报》2013,62(7):75205-075205
本文搭建了一种无摩擦气垫悬浮测试平台测量了19针和31针-网电极离子风激励器产生的推力特性, 为多针-网电极离子风激励器作为新型动力源提供动力控制方法. 通过研究多针-网间隙、针-针间距、针尖曲率半径和电晕电压电流对离子风激励器推力特性的影响, 提出了在低功耗下产生较大推力的方法, 改善离子风激励器对低功耗与大推力的需求不能同时满足的现状. 关键词: 多针-网电极 离子风 推力 推功比  相似文献   

2.
李小华  包伟伟  王静  蔡忆昔  李慧霞 《发光学报》2015,36(10):1195-1200
针对大功率LED芯片的散热问题,提出了一种基于电晕放电原理的离子风散热方案。通过试验,研究了电晕放电的电学性能,同时探寻了放电电压对制冷效果的影响以及温降随电晕放电功率的变化规律。结果表明,放电间距相同时,对发生器施加负电晕能够在较低的电压下产生离子风,降温效果显著。电晕电流平方根与放电电压呈线性关系。电晕放电功率为1.5 W、放电间距为10 mm时,散热效果最好。  相似文献   

3.
以发射光谱法为基础,检测了常压状态线-板式脉冲电晕放电过程OH自由基在反应器内的空间分布;研究了线电极直径,线线间距以及线板间距对生成OH自由基的影响;从而明确脉冲电晕放电反应器的性能。结果显示:OH自由基浓度沿线电极X轴方向逐渐降低,活化区域半径20mm左右,沿Y轴方向先升高后降低,活化区域半径大于30mm;线电极的直径小于2mm时,OH自由基的光谱强度基本不变,线电极直径继续增大,发射光谱强度随之迅速下降。线线间距逐渐增大,OH自由基的发射光谱强度随之增强。OH自由基的发射光谱强度随着线板间距的增大而降低。  相似文献   

4.
电场对火焰形状及碳烟沉积特性的影响   总被引:2,自引:0,他引:2  
王宇  姚强 《工程热物理学报》2007,28(Z2):237-239
建立了三种类型的直流电场分别作用于层流扩散火焰,研究了电场类型、电场强度对火焰形态及所产生的碳烟颗粒在电极上的沉积特性的影响.实验表明,针状电极由于离子风的作用会使火焰高度变短;平板状电极由于电场力的作用可使火焰顶部向阴极板倾斜,证明了有一部分碳烟颗粒本身荷正电.同时,由于环形电极同时产生离子风和电场力,影响火焰形态.而荷正电的中心电极对碳烟颗粒的排放起到抑制作用.  相似文献   

5.
利用光谱学方法,对针-水电极和针-板电极直流辉光放电特性进行了比较研究。结果发现两种装置产生的放电都有明显的分区现象, 从阴极到阳极分别为负辉区、阴极暗区、正柱区和阳极辉区。针-板电极放电中可以清晰地观测到阳极暗区, 而针-水电极放电阳极暗区不明显。对比两种放电的伏安特性曲线,发现放电电压均随电流增大而减小,但相同电流下针-水电极间的电压大于针-板电极间的电压。由于伏安特性具有负斜率,且放电电流密度介于10-5~10-4 A·cm-2,说明两种装置中的放电均处于正常辉光放电阶段。在正常辉光放电的范围内比较两种放电的发射光谱, 发现发射光谱中都包含N2的第二正带系(含波长为337.1 nm的谱线)和N+2的第一负带系(含波长为391.4 nm的谱线),但相对强度不同。利用光谱学方法对放电发射谱的谱线强度比I391.4I337.1和振动温度进行了空间分辨测量,发现相同位置处针-水电极放电的谱线强度比要比针-板电极放电的大,并且相同位置处针-水电极放电的振动温度高。  相似文献   

6.
为了提高板式逆流气-气换热器的显热效率,根据新风换气机实物原型,提出三种模型结构方案。通过CFX数值模拟软件计算,参照实验工况,分别对板间距为5mm、7mm、9mm的国际象棋式换热器温度变化和压力变化进行分析,为换气机的设计和生产提供参考。结果表明:新风口出口温度随送风速度的增加而降低;新风(排风)速度恒定时,换热效率随板间距的增加而明显升高,随室内外温差的增大而变大;随着送风速度的增加,新风侧通道内压力降显著增加。芯体压力降几乎不受室内外温差变化影响。  相似文献   

7.
自行研制的等离子体针在大气压下通过介质阻挡放电产生的等离子体,再由喷嘴处安装的漏斗形装置聚焦形成针状等离子体. 然后对针状等离子体的基本特性和杀Enterococcus faecalis(E. faecalis)菌进行了研究,E. faecalis菌是一种引起完善充填根管再感染的主要微生物. 当等离子体针功率为5-28W时,对等离子体的温度进行了测量,表明它不同于其他热杀菌方式. 通过改变等离子体针内电极末端注入的氧气量,发现适当的氧气量,不仅增加等离子体内含氧粒子的浓度而且对等离子体的长度影响也不明显. 实验表明最佳参数为功率15W,0.1m3·h-1氦和2.5%氧气,间距12mm,处理时间30 s. 为了找出杀菌的关键粒子,进一步比较了大气压下的等离子体针的发射光谱与agar(琼脂)2mm下的光谱并找出关键粒子.  相似文献   

8.
本文对不同结构微型燃气轮机回热器的回热效率及阻力等性能进行了比较分析。研究表明:随回热效率的提高, 板式及板翅式回热器总体积上升,阻力升高。另外,板式换热器在满足阻力条件下,可以通过改变板间距取到最小体积。在同等回热效率要求下,板翅式回热器体积远小于板式,其紧凑度更高,而阻力上升也不明显。  相似文献   

9.
采用对比测量方法研究了微通道板结构参数,即开口比、板厚、电极深度、离子阻挡膜、输入增强膜对其噪声因子的影响。结果表明,开口比增大,噪声因子减小;板厚增加,噪声因子增加;输入电极深度增加,噪声因子增加;离子阻挡膜会增加噪声因子;输入增强膜会降低噪声因子。其中,离子阻挡膜对噪声因子的影响最大,板厚对噪声因子的影响最小。微通道板的结构参数不仅对噪声因子产生影响,而且对其他参数,如增益、均匀性等性能均会产生影响。要降低微通道板噪声因子,比较可行的方法是将微通道板的开口比提高到68%,在此基础上,再在微通道板的输入端制作一层高二次电子发射系数的MgO2输入增强膜,使微通道板的噪声因子接近1,从而达到理想微通道板的水平。  相似文献   

10.
研究了常压空气中针-石蜡液面 50Hz 交流电晕放电离子风特性。交流电晕离子风能够引起液体石蜡 显著变形,随着电压升高,变形从漏斗状发展到盆状。在石蜡层厚度为 5mm 时,盆状变形最大,深度达到 5.3mm, 最大作用范围半径 18.8mm,变形产生的压强达到 48.9Pa,远远超过直流针-水电晕放电情况。随着电压升高,从 电晕放电过渡到流注放电时盆状变形依然存在,这一点明显不同于直流针-水电晕放电。研究表明交流电晕离子风 具有优良的驱动绝缘液体介质的巨大潜力。  相似文献   

11.
We report on the results of experimental investigations of the kinematic structure of ionic wind from a wire electrode placed near a heated plate, which plays the role of the earthed electrode. Experiments are carried out in a wide range of voltages for different polarities of the wire for several values of the electrode gap. We compare the structures of the flows emerging as a result of natural convection in open air for different positions of the plate and in the presence of a fast ionic wind jet that considerably intensifies heat transfer in the boundary layer at the heated planar electrode. Local temperature distributions over the plate surface are obtained, as well as the integral dependences of the effective heat removal on the electric parameters of the corona discharge. The velocity of air flows with ionic wind reaches 4 m/s, and the heat power removed from the plate for fixed overheating increases ninefold compared to the situation with natural convection.  相似文献   

12.
文中针对三维坐标系下,圆翅片叉排热管散热器的流动和传热特性进行数值模拟研究。分析了三个主要影响因素:翅片间距、翅片厚度和排间距对平均换热系数、流动摩擦系数和热阻的影响。翅片间距分别为6mm、7mm和8mm,翅片厚度分别为0.8mm、1mm和1.2mm,排间距分别为21.7mm、23mm和24.3mm。模拟结果表明:随着迎面风速增加,摩擦系数减小,传热热阻减小;随着翅片厚度的增加,摩擦系数减小、换热能力增强,热阻在大Re时增大明显。随着翅片间距的增大,摩擦系数增大,换热能力提高,热阻增大;随着排间距的增大,摩擦系数在正三角形管排布时的值上下变动,且只有排间距显著增大时,换热能力和热阻才会增大。  相似文献   

13.
Technical Physics - We have investigated experimentally the cooling of a heated plate playing the role of a grounded electrode by a narrow intense ionic wind jet produced by a needle electrode and...  相似文献   

14.
Needle–cylinder electrodes designed to generate ionic wind have been explored experimentally. The increase of the gap distance between needle and cylinder from 4 mm to 16 mm cause an increase of the ionic wind velocity from 1.1 m/s to 2.46 m/s. The opposite behavior was observed when this distance lengthened from 18 to 28 mm. At the same time, a step voltage was used to increase the ionic wind velocity up to 3.6 m/s. These results indicate that electrode arrangement is very important to maximize the ionic wind velocity.  相似文献   

15.
Transient heat transfer coefficients for helium gas flowing over a horizontal plate (ribbon) were measured under wide experimental conditions. The platinum plate with a thickness of 0.1 mm was used as the test heater and heated by electric current. The heat generation rate was exponentially increased with a function of Q0 exp(t/τ). The gas flow velocities ranged from 4 to 10 m/s, the gas temperatures ranged from 290 to 353 K, and the periods of heat generation rate, τ, ranged from 50 ms to 17 s. The surface superheat and heat flux increase exponentially as the heat generation rate increases with the exponential function. It was clarified that the heat transfer coefficient approaches the quasi-steady-state one for the period τ longer than about 1 s, and it becomes higher for the period shorter than around 1 s. Empirical correlation for transient heat transfer was also obtained based on the experimental data.  相似文献   

16.
The DC corona discharge in air and the induced ionic wind were investigated in the needle-to-water system at atmospheric pressure. The water deformation was measured under various conditions, and wind pressure and active areas were estimated accordingly. The effects of applied voltage, gap spacing and tip radius on the corona ionic wind were studied and the qualitative analysis was provided. Self-rotation of corona discharge was observed in experiments. The results show that higher voltage or electric field strength results in a stronger ionic wind. The active area increases with applied voltage below a voltage threshold. There is an optimal gap distance for a wider as well as stronger ionic wind and blunter needle we used leads to an enhancement on both the active area and the wind strength. The wind velocity reaches 7 m/s at optimized condition in the present system. The rotation of corona discharge helps to improve the active area and uniformity of the treating area which may be associated with the chemical reaction of the water surface.  相似文献   

17.
Spray cooling is an effective tool to dissipate high heat fluxes from hot surfaces. This article thoroughly investigates the effect of thickness of a hot stainless steel plate on the cooling time, cooling rate, heat flux, and heat transfer coefficient under constant mass flow rate maintained at 1 MPa using water as the coolant. Cylindrical samples of stainless steel with constant diameter (D = 25 mm) and thickness (δ = 7.5, 12, 16.5, and 21 mm) were used in the present study. Critical droplet diameter to achieve an ultra-fast cooling rate of 300°C/s was estimated by using an analytical model for samples of varying thicknesses. The analytical model (one side spray cooling) showed good agreement with experimental results with a relative error of 3.2% in the plate thickness range of 1–12 mm. An increasing trend in maximum heat flux was found with increasing thickness of the plate. Maximum heat flux as high as 1,800 kW/m2 was achieved for a 21-mm-thick sample. Heat transfer coefficients in the range 0.092–96.24 kW/m2K, 0.111–98.9 kW/m2K, 0.074–63.4 kW/m2K, and 0.127–55.63 kW/m2K were reported for sample of varying thicknesses in the present study. Limited published work is available with reference to water spray cooling dynamics and thickness of stainless steel plate. Therefore, the present study focuses on the correlation between the thickness of the plate and spray dynamics of water spray cooling.  相似文献   

18.
An electrohydrodynamic investigation has been carried out in a pin-to-plate gas discharge system to clarify the mechanism of repulsive force generation between a pin and plate electrode at corona discharge. Numerical calculations have been conducted in two steps. First, the axi-cylindrical static corona discharge field was calculated with the finite-element method to deduce the Coulombic body force ρ E applied to the air, where ρ is the charge density and E is the electric field, and then the induced ionic wind was calculated with the finite differential method. The calculated pressure distribution on the plate electrode was on the order of 10 Pa which was in good agreement with the measured pressure distribution. The calculated air velocity at the center was several m/s and was confirmed by a time-of-flight experiment and the velocity distribution near the pin electrode also agreed with measurements using a laser Doppler velocimeter. Pressure and wind velocity were increased at high-applied voltage. These results confirm that the ionic wind is the cause of the repulsive force to the pin electrode at the corona discharge.  相似文献   

19.
纳秒脉冲空气辉光放电等离子体及应用   总被引:1,自引:0,他引:1       下载免费PDF全文
采用基于半导体断路开关的纳秒脉冲高压电源,在两个金属电极之间产生放电区间为1 600mm×100 mm×25 mm的常压辉光空气等离子体。等离子体发生器采用负高压针电极阵列与平板阳极结构,针电极的直径为1 mm,长度为20 mm,针电极之间的间隔为20 mm,针电极与平板零电位之间的距离为25mm,在每个负高压针电极末端周围同时形成圆锥形辉光放电,在平板地电极则形成大面积辉光放电。采用电压探针测量了该新型等离子体的放电特性,结果表明:放电脉冲的上升时间为26 ns,最高脉冲输出峰值电压为27 kV;利用该辉光等离子体对幅宽为1 000 mm聚四氟乙烯薄膜进行了表面改性处理,处理后其表面接触角由原来的124°降到69°,亲水性能大为提高。  相似文献   

20.
Experimental visualization for ionic wind motion originated from DC corona discharges in a needle-plate electrode system has been investigated. A vapor-phase biacetyl tracer with laser-induced phosphorescence emission is used for optically characterizing the ionic wind profile. The ionic wind blows the excited biacetyl molecules away in continuing the visible phosphorescence emission for a long radiative lifetime. The captured image with elapsing time from the excitation presents the shifting location of radiative tracer along the ionic wind direction. The experimental results show the ionic wind profile enhanced in the electric field direction corresponding to the corona discharge progress. Especially, the ionic wind near an initiating point of corona discharges is focused as an advantage of this optical technique. The ionic wind velocity along the electrode axis can be obtained at the location close enough to the corona discharge initiation point, and the velocity at 0.5 mm from the discharge point is figured out as 9.3 to 19.2 m/s under the condition of the EHD Reynolds number of 0.95×103 to 2.1×103.  相似文献   

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