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1.
汽泡在电场作用下的变形   总被引:3,自引:1,他引:2  
为探明外加电场对汽泡形状的影响规律,本文采用人工注射汽泡的方式,对均匀电场作用下单个汽泡的形状进行了可视化试验研究,计算了汽-液两相系统中的电场分布及汽泡所受的电应力。结果表明:电场作用下汽泡表面所受电应力分布的不均匀性导致汽泡沿与电场相平行的方向拉长,变成扁长椭球形。随着场强的增加,汽泡变形量加剧,汽泡与壁面的接触角逐渐变大。此外,讨论了汽泡变形对电场强化沸腾换热的影响。  相似文献   

2.
为探明外加电场作用下,不同工质对强化沸腾换热的影响,本文采用了FC-72、R11、R113和R123四种工质,定量研究了两相系统中汽泡周围电场分布特性,探讨了工质介电常数对汽泡的作用规律.结果表明:随着工质介电常数的增加,电场非均匀性增强,电场对汽泡的作用加剧.这为不同工质对EHD沸腾强化效果不同提供了理论依据.  相似文献   

3.
为明晰电场对两相系统中离散相的作用,本文针对均匀电场作用下两相系统中的单个离散相的行为进行了可视化试验研究及数值模拟。通过建立电场数学模型。得到了均匀电场作用下两相系统的电场分布;运用电应力表面积分的方法求得了离散相所受的电场力。并于试验中观察了不同粒径的离散相在电场作用下的运动情况,其试验结果与数值计算结果基本吻合。  相似文献   

4.
EHD两相系统中的电场数值模拟   总被引:3,自引:1,他引:2  
董伟  李瑞阳  郁鸿凌 《计算物理》2004,21(4):363-366
针对均匀电场作用下两相系统中的单个离散相周围电场分布情况,建立了数学模型.在建模过程中,考虑了离散相的存在对电场分布的影响.通过求解电场控制方程,得到了均匀电场作用下离散相周围及其内部的电势及电场分布的数值解,并理论验证了该数值解的准确性.  相似文献   

5.
针对微槽内饱和沸腾汽泡建立了简化模型,并利用COMSOL Mu ltiphysics软件对电场中汽泡动力学特性进行了数值模拟,分析了微槽道内EHD(electrohydro dynam ics)强化沸腾传热机理。实验以去离子水为工质,研究了外加直流电场下两种规格的矩形微细槽道内饱和沸腾传热强化特性,电压在0~28kV内,EHD技术对微细槽道内的饱和沸腾传热有明显的强化效果。  相似文献   

6.
本文在空气自然冷却条件下,对MEMS硅基并联微通道中蒸汽凝结换热的流型和多通道效应进行了可视化研究,发现在低入口饱和蒸汽压下,通道入口为准静止状态的汽弹、汽弹前端周期性脱离汽泡、通道下游为泡状流;在高入口饱和蒸汽压下,通道内为环状流.汽泡脱离存在单汽丝断裂、双汽丝同步断裂以及双汽丝非同步断裂三种不同模式.汽液界面上表面张力不均匀引起Marangoni对流,使得两侧通道中的汽泡一旦形成,便被推向通道的高温侧.  相似文献   

7.
在汽泡流流型区域内,其汽泡间的相互碰撞和汽泡对周围液体的扰动非常明显。这种作用使得汽液两相流中汽含率的分布具有一定的特征。它在流动沸腾中显得特别重要。前人曾提出汽含率在汽泡流中的分布呈指数函数形式,在圆管中心处有一最大点。但实验证明在向上并流时靠近边界处的汽含率较高,目前已提出一些机理和模型来描述这种现象,但处理的结果尚未十分满意,需作进一步改进。  相似文献   

8.
电场可强化池态沸腾换热已经普遍得到研究者的认可,在电场强化换热的实验研究中,以往研究者主要采取统计学的方法研究电场作用下沸腾汽泡的动态特性,也有研究者研究了冷态注入气泡在电场作用下的动态特性,而直接针对单个沸腾汽泡的研究鲜有报道。本文采用针状电极以R113为实验工质,研究了小加热面上不同热流密度和不同电场强度的情况下单个沸腾汽泡的动态特性,实验中发现在电场的作用下汽泡脱离半径和脱离体积变小,而汽泡成长时间和汽泡等待时间随着电场强度的增加而增大。  相似文献   

9.
微槽群内汽泡动力学行为对接触线的影响   总被引:1,自引:0,他引:1  
针对沸腾情形下毛细微槽群热沉内汽泡对汽液固三相接触线的影响,进行了可视化实验研究。研究结果表明:汽泡动力学行为会直接导致微槽群内三相接触线的形状变化,从而引起蒸发薄液膜的厚度、面积以及汽液界面曲率等对薄液膜的蒸发换热特性有重要影响的物理量的变化。实验证实了在开放式微细尺度槽群结构热沉中,固有弯月面区域里的沸腾与扩展弯月...  相似文献   

10.
本文在经典汽泡动力学理论基础上,提出了描述汽泡生长过程的综合界面模型.本模型的核心在于汽泡内部的热力学过程的详细分析及汽液界面的传热、传质过程的详细描述.并对汽泡生长过程进行了模拟计算,给出了动力学控制阶段的时间范围.本模型对汽泡生长、汽膜发展的理论分析及数值模拟提供了良好的基础.  相似文献   

11.
The electrical breakdown of microwave plasma in water was investigated between 1 and 30 kPa. The dependency of the ignition power for generating plasma on the size of coaxial electrode was measured. The ignition power decreases with a decrease of the diameter of the inner electrode. The behavior of microwave plasma in water was observed using a high-speed camera. The plasma ignites in a bubble generated by microwave heating. The model for calculating the electric field was created on the basis of the captured images of the bubble just before plasma ignition. The method presented can be used to visualize the electrical field distribution in the bubble. The electric field breakdown was calculated using the measured ignition power. The electric field breakdown of plasma in water is of the same order as gas phase plasma.  相似文献   

12.
Based on the Cahn-Hilliard phase field model, a three-dimensional multiple-field coupling model for simulating the motion characteristics of a rising bubble in a liquid is established in a gas-liquid two-phase flow. The gas-liquid interface motion is simulated by using a phase-field method, and the effect of the electric field intensity on bubble dynamics is studied without electric field, or with vertical electric field or horizontal electric field. Through the coupling effect of electric field and flow field, the deformation of a single rising bubble and the formation of wake vortices under the action of gravity and electric field force are studied in detail. The correctness of the results is verified by mass conservation, and the influences of different electric field directions and different voltages on the movement of bubbles in liquid are considered. The results show that the ratio of the length to axis is proportional to the strength of the electric field when the air bubble is stretched into an ellipsoid along the electric field line under the action of electrostatic gravity and surface tension. In addition, the bubble rising speed is affected by the electric field, the vertical electric field accelerates the bubble rise, and the horizontal direction slows it down.  相似文献   

13.
An acoustic radiation force counterbalanced appliance was employed to map the cavitation distribution in water. The appliance was made up of a focused ultrasound transducer and an aluminum alloy reflector with the exactly same shape. They were centrosymmetry around the focus of the source transducer. Spatial–temporal dynamics of cavitation bubble clouds in the 1.2 MHz ultrasonic field within this appliance were observed in water. And they were mapped by sonochemiluminescence (SCL) recordings and high-speed photography. There were significant differences in spatial distribution and temporal evolution between normal group and counterbalanced group. The reflector could avoid bubble directional displacement induced by acoustic radiation force under certain electric power (⩽50 W). As a result, the SCL intensity in the pre-focal region was larger than that of normal group. In event of high electric power (⩾70 W), most of the bubbles were moving in acoustic streaming. When electric power decreased, bubbles kept stable and showed stripe structure in SCL images. Both stationary bubbles and moving bubbles have been captured, and exhibited analytical potential with respect to bubbles in therapeutic ultrasound.  相似文献   

14.
沈壮志  吴胜举 《物理学报》2012,61(12):124301-124301
以液体为工作介质, 利用空化泡的RP控制方程, 模拟分析了无量纲化的电场频率、场强的幅值以及无量纲化的声波频率、 声压幅值的变化对空化泡运动特性的影响. 结果表明: 声场和电场联合作用时, 空化泡运动处于混沌区域范围远高于两者单独作用下空化泡的混沌区域范围. 这不仅对声空化的进一步研究具有重要的理论意义, 而且对于提高和改进空化降解有机污染物的技术也具有指导意义.  相似文献   

15.
Electric field distribution is an important parameter for nanostructure arrays in nanobiosensing appfications. It can influence the sensitivity and the resolution of nanobiosensors. We focus on the effect of media on the electric field distribution of a rhombic silver nanostructure array. The finite-difference time-domain algorithm- based numerical calculation method is used to monitor the electric field distribution of the silver nanostructures when the refractive index of the medium around the nanostructure array is changed. The calculated results show that tuning the refractive index of the medium around silver can have a considerable influence on the electric field distribution in the reflection and transmission directions. This effect can be used to increase the extinction efficiency and to improve the resolution of the spectra for nanobiosensing.  相似文献   

16.
本文主要研究了直流电场对冷态注入氮气气泡和R113沸腾气泡行为的影响.利用高速摄像机拍摄了冷态注入气泡和热态沸腾气泡在不同场强作用下的实验图像,并对气泡的脱离进行了定量分析.实验结果表明:注入氮气气泡和沸腾气泡沿电场方向显著伸长,其脱离长径比随着场强升高而增大,并且电场对沸腾气泡伸长行为的影响更显著.此外,注入气泡和沸腾气泡的脱离体积随着场强增大都具有减小的趋势,而且注入气泡体积随场强减小的行为更明显.  相似文献   

17.
In this study, based on different numberical simulation methods, the gas-liquid two-phase flow is taken as the research object. By coupling the continuity equation of incompressible fluid, Navier-Stokes equation, electric field equation and other control equations, a multi-field coupling model for rising bubbles in viscous fluids is established, and numerical simulations are carried out. The two-phase popularity of coupled electric field is studied, and the effect of electric field on bubble motion is analyzed.The Level-set and phase field method are used to track the changes of deformation and rupture during the rising of the bubble. The accuracy and validity of the two methods are verified by mass conservation. At the same time, the calculation area is determined for the accuracy of calculation, and the optimal mesh size is calculated by using mesh independence test. Compared with the level set method, the phase field method has a certain improvement in the calculation efficiency and accuracy. Among them, the calculation efficiency of the phase field calculation method in the same grid is increased by 5 times, and by 3 times in the vertical electric field environment. Moreover, using the phase field method is easier to capture the bubbles slight changes while they are rising, and the quality of the simulation results is better.The simulation analysis of bubble rising process under coupled electric field by two methods shows that under the interaction of electrostatic force, buoyancy and surface tension, the bubble is stretched into an ellipsoid along the direction of the electric field line, and the ratio of the length to the short axis is proportional to the applied electric field strength. In addition, the bubble rising velocity is affected by the electric field, and the vertical electric field accelerates the rising of the bubble.  相似文献   

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