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1.
非等温液滴蒸发燃烧的传热传质特性   总被引:1,自引:0,他引:1  
对无重力、相对静止热环境中碳氢燃料单液滴的蒸发燃烧过程,建立了非等温液滴蒸发-火焰面燃烧耦合模型。考虑了液滴内导热、液滴表面蒸发、火焰面化学反应以及气相区对流传热传质的瞬态耦合作用。将整个耦合系统分解为液滴、火焰面内气相区、火焰面外气相区三个相对独立的计算域,采用固定计算域法与随动坐标系,结合耦合界面条件,进行数值求解。分析了液滴蒸发燃烧过程中的传热传质特性以及环境压力的影响。结果表明,液滴蒸发与燃烧强烈耦合,过程后期的蒸发和火焰面动态特性与初期明显不同。  相似文献   

2.
为考察溶液注入热等离子体喷涂过程中喷雾参数对涂层质量的影响,本文建立了溶液液滴在热等离子体中运动蒸发的数学模型。模拟了液滴在不同参数下的运动和蒸发的过程,考虑了液滴、热等离子气流及液滴表面气体混合物随温度及组分的物性变化以及斯蒂芬流的影响,得到液滴的运动轨迹,蒸发速率以及半径和表面温度的变化。结果表明在一定范围内增大液...  相似文献   

3.
激波诱导液滴变形和破碎现象实验研究   总被引:3,自引:0,他引:3  
本文介绍了用于激波诱导液滴变形和破碎现象研究的实验系统及方法,详细分析了激波与液滴相互作用以及液滴加速、变形和破碎过程,为进一步研究激波诱导的液滴内流场性质及气液相间相互作用对液滴变形和破碎的影响机制提供了基础实验数据。  相似文献   

4.
本文通过单光束梯度力光学镊子-拉曼光谱系统,对硫酸镁单液滴随着相对湿度变化的反应进行了探究。当硫酸镁单液滴被光镊捕获之后,通过相对湿度的梯度变化探究了捕获液滴的蒸发动力学变化。发生在与耳语回音模相称波长的受激拉曼散射可以用来准确地确定液滴半径,因此,可以通过腔增强拉曼散射得到在不同湿度下处于平衡的液滴半径信息。本研究通过光镊对硫酸镁单液滴的实时监测,阐述了在某个相对湿度范围内该液滴的粒径变化的过程和结果,在此之前的硫酸镁吸湿性研究中没有先例。研究结果表明在相对湿度逐渐降低至40%的过程中硫酸镁液滴半径的变化速率逐渐变小。而当相对湿度低于40%时,液滴半径的减小会被严重抑制。这种现象表示在高浓度条件下硫酸镁液滴中水的蒸发扩散速率会降低。另一方面,在蒸发过程后的相对湿度上升过程中,硫酸镁液滴尺寸的增加明显缓慢于湿度增长速度。这一现象显示液滴的尺寸变化是不可逆的。说明胶态的形成导致了传质受阻,从而阻碍了液滴中水分子的交换。  相似文献   

5.
激光手术喷雾冷却中单液滴蒸发理论模型的比较   总被引:2,自引:0,他引:2  
制冷剂喷雾可对激光治疗葡萄酒色斑过程进行有效冷却以保护表皮不受热损伤,其瞬态喷雾冷却过程涉及复杂的液滴蒸发、强烈的对流换热和质量传递.本文对描述制冷剂喷雾平衡蒸发阶段单个液滴蒸发的理论模型进行改进,比较了基于各种假设的七个气相传质模型对R-134a喷雾冷却过程中单个液滴蒸发特性的影响,发现考虑过热影响的气相模型所预测的蒸发过程最接近实验结果,用该模型研究了液滴初始直径和速度等参数对液滴蒸发特性的影响.  相似文献   

6.
液滴的流动蒸发换热是一个即常见又基础的问题,对液滴的流动蒸发换热进行准确的描述对许多工程实际及科学研究都有很重要的意义。对于这样一个多相、多组分输运的物理过程,本文使用VOF方法对液滴形态进行描述,建立动力学蒸发模型对液滴的蒸发过程进行刻画,同时在气相中使用组分输运方程最大程度上还原了液滴蒸发的物理过程。本文使用所建立的数值方法对正庚烷液滴的自然对流蒸发及强迫对流蒸发进行了数值模拟计算,与实验结果吻合良好。  相似文献   

7.
为了揭示低温条件下天然气中硫化氢气体超声速凝结特性,为实现天然气超声速旋流分离技术在天然气脱硫化氢领域的应用提供理论依据,建立了甲烷-硫化氢双组分气体超声速凝结流动数学模型,对Laval喷管内不同组分比例条件下甲烷-硫化氢双组分气体凝结流动进行了数值模拟,得出了Laval喷管内温度、压力、速度、成核率、液滴数目、液滴半径、液相质量分数的分布情况。结果表明,随着入口硫化氢含量的增加,入口过冷度增加,更容易达到凝结所需要的极限过冷度,成核发生位置越靠近喉部,且成核区间变窄,极限成核率增大;硫化氢气体凝结释放的潜热对流场产生影响,使得马赫数和过冷度略有降低,之后几乎保持稳定至出口;入口硫化氢含量较高时,硫化氢液滴半径较大,Laval喷管出口液相所占比重较大;而当入口硫化氢含量较低时,液滴半径明显减小,Laval喷管出口液相硫化氢所占比重几乎为0,硫化氢的脱除效率较低。  相似文献   

8.
《工程热物理学报》2021,42(10):2625-2632
为了了解液滴表面热流型演变规律及其对蒸发速率的影响,采用稳态蒸发实验研究了加热基底上乙醇和水滴的蒸发过程。液滴半径固定在R=2.5 mm,高度变化范围为0.4至1.4 mm。结果表明,随着液滴高度降低,乙醇液滴表面出现了中心不均匀的温度波动、热流体波及Bénard-Marangoni流胞,而水滴表面则没有明显温度波动。随着基底温度升高,液滴内部热对流增强;随着液滴高度降低,乙醇液滴蒸发速率先减小、后增大,而水滴蒸发速率则无明显变化。实验结果证实热对流对液滴蒸发速率具有明显促进作用。  相似文献   

9.
针对高温气流中燃料液滴的受热蒸发过程,以正十二烷液滴为例,建立了考虑液滴受热膨胀、表面张力及气流热物性变化的分析模型。采用移动网格法,并通过温度插值减小网格移动产生的偏差,编制了计算程序。在与文献结果对比验证的基础上,数值模拟了高温对流环境中的液滴蒸发过程;探讨了高温气流加热条件下,液滴表面张力变化对液滴蒸发的影响。结果表明,是否考虑液滴表面张力及其随温度变化,对液滴内压和蒸发过程的影响不大。  相似文献   

10.
燃料液滴高压蒸发理论   总被引:2,自引:0,他引:2  
本文提出了一个燃料液滴在高压环境下的蒸发理论,该理论考虑了液滴表面的内移、液滴不定常加热以及高压非理想气体效应的影响等因素。计算了C_(12)H_(26)液滴在1.8—90大气压、2000—3200°K的N_2气介质中蒸发时的滴温、半径随时间变化的关系。计算结果表明,存在一个划分亚临界蒸发和超临界蒸发的压力极限,在亚临界蒸发时,液滴生存时间随压力增加而减少,超临界蒸发时,液滴生存时间随压力增加而增加,在本例情况下,此极限压力值为2.23p_c。  相似文献   

11.
液滴撞击圆柱内表面的数值研究   总被引:1,自引:0,他引:1       下载免费PDF全文
李玉杰  黄军杰  肖旭斌 《物理学报》2018,67(18):184701-184701
针对液滴撞击圆柱内表面的过程,利用基于相场的格子Boltzmann方法模拟液滴以不同初速度、从不同初始高度、撞击不同大小的圆柱内表面时液滴的形态变化,分析了液滴自身物性(如密度和黏性等)和圆柱内表面润湿性等因素对撞击现象的具体影响.研究发现:撞击韦伯数、密度比及动力黏性比、圆柱半径等对液滴撞击后沿圆柱内表面的铺展均有一定影响,较高的韦伯数下液滴可能会发生分裂;液滴初始高度对大密度比和动力黏性比的撞击影响较小;液滴反弹现象可能出现在接触角较大时;重力作用会抑制撞击后液滴的振荡.  相似文献   

12.
The main purpose of this paper is to numerically study the effect of droplet radius, temperature, and surface wettability on droplet surface tension. Moreover, the validity of Young-Laplace equation (Y-L) for nano-droplet is examined. Simulations of droplet surrounded by its vapor and droplet on solid surface are carried out and the results are compared to each other in order to comprehend the role of surface wettability on droplet surface tension. The pair potential for the liquid-liquid and liquid-solid interaction is considered using Lennard-Jones model. Different numbers of atoms and surface wettabilities are employed to generate droplet of different radiuses. In addition, contact angle of droplet on solid surface is computed. Pressure tensor and density profile is locally calculated. Furthermore, liquid pressure is evaluated far from the interface using the virial theorem and gas pressure is obtained using an equation of state. In order to calculate the surface tension, two different approaches are employed; Young-Laplace equation and direct molecular dynamics (MD) simulation. The surface tension increases with increase in droplet radius and it is seen that the surface wettability does not directly influence the surface tension.  相似文献   

13.
Presented are results of experimental investigations concerned with formation of a nonstationary and essentially nonuniform temperature field of a water droplet (initial radius of 1 mm to 2 mm) under intensive heating in a flow of heated air (from 50?C to 1000?C). The method used for this purpose was a noncontact optical planar laser-induced fluorescence (PLIF) method. It is shown that temperature distribution in a water droplet is essentially inhomogeneous even under prolonged heating (to several tens of seconds). Reliability of the results of measurements by the noncontact PLIF method was analyzed by applying a group of fast miniature thermocouples. Restrictions of using the PLIF method for studying temperatures fields of evaporating droplets under high-temperature heating (over 800?C) were marked out. Characteristic times of droplet existence (complete evaporation) were determined. It was analyzed how the temperature difference in a water droplet affects this parameter during heating and intensive phase transitions. It was substantiated that it is expedient to consider essentially inhomogeneous and nonstationary temperature field of a water droplet inmathematical modeling of the heat andmass transfer processes in high-temperature gas–vapor-droplet systems (corresponding, e.g., to burning or heat cleaning of liquids, firefighting, production of composite and gaseous fuels, their combustion, etc.).  相似文献   

14.
A system of equations for electron gas and lattice around and along the trajectory of a heavy uranium ion with an energy of 700 MeV in nickel at constant heat capacity and heat conduction taken at room temperature is solved numerically in an axially symmetric cylindrical coordinate system. On the basis of the lattice temperature obtained as a function of radius around the ion trajectory and depth, a conclusion is made that the ionization energy losses of a uranium ion in nickel are sufficient for melting and evaporating the material from the surface. The maximum radius and depth of the region in which melting and evaporation take place are estimated.  相似文献   

15.
16.
Fundamental understanding of the wettability of curved substrates is crucial for the applications of microdroplets in colloidal science, microfluidics, and heat exchanger technologies. Here we report via lattice Boltzmann simulations and energetic analysis that microdroplets show an ability of transporting selectively to appropriate substrates solely according to substrate shape(curvature), which is called the substrate-curvature-dependent droplet targeting because of its similarity to protein targeting by which proteins are transported to the appropriate destinations in the cell. Two dynamic pathways of droplet targeting are identified: one is the Ostwald ripening-like liquid transport between separated droplets via evaporating droplets on more curved convex(or less curved concave) surfaces and growing droplets on less curved convex(or more curved concave) surfaces, and the other is the directional motion of a droplet through contacting simultaneously substrates of different curvatures. Then we demonstrate analytically that droplet targeting is a thermodynamically driven process. The driving force for directional motion of droplets is the surface-curvature-induced modulation of the work of adhesion, while the Ostwald ripening-like transport is ascribed to the substrate-curvature-induced change of droplet curvature radius. Our findings of droplet targeting are potentially useful for a tremendous range of applications, such as microfluidics, thermal control, and microfabrication.  相似文献   

17.
The energy transport mechanisms of a sessile-water droplet evaporating steadily while maintained on a Cu substrate are compared. Buoyancy-driven convection is eliminated, but thermal conduction and thermocapillary convection are active. The dominant mode varies along the interface. Although neglected in previous studies, near the three-phase line, thermocapillary convection is by far the larger mode of energy transport, and this is the region where most of the droplet evaporation occurs.  相似文献   

18.
为实现微流控芯片上微液滴的检测与计数,设计了光纤式检测与计数单元,使用TracePro软件进行建模仿真以便为检测信号处理提供依据。根据液滴通过检测区域时引起的光强变化来实现计数,分析了照明光束准直性、液滴尺寸、液滴相对溶液折射率以及接收光纤相距芯片距离对光强变化的影响。仿真实验结果表明,照明光束准直性越差,液滴半径越大,相对溶液折射率越低,接收光纤距离越近,相对光强变化越明显,并且液滴大小决定着光强变化曲线中是否会出现双波谷现象,液滴半径小于13 μm时,液滴检测信号为明显的单波谷,半径大于17 μm时,液滴信号为明显双波谷。根据仿真结果提出了检测信号的处理方法,表明该单元可以实现微流控芯片上微液滴的检测与计数功能。  相似文献   

19.
In the present study, a framework for modeling two-phase evaporating flow is presented, which employs an Eulerian–Lagrangian–Lagrangian approach. For the continuous phase, a joint velocity-composition probability density function (PDF) method is used. Opposed to other approaches, such PDF methods require no modeling for turbulent convection and chemical source terms. For the dispersed phase, the PDF of velocity, diameter, temperature, seen gas velocity and seen gas composition is calculated. This provides a unified formulation, which allows to consistently address the different modeling issues associated with such a system. Because of the high dimensionality, particle methods are employed to solve the PDF transport equations. To further enhance computational efficiency, a local particle time-stepping algorithm is implemented and a particle time-averaging technique is employed to reduce statistical and bias errors. In comparison to previous studies, a significantly smaller number of droplet particles per grid cell can be employed for the computations, which rely on two-way coupling between the droplet and gas phases. The framework was validated using established experimental data and a good overall agreement can be observed.  相似文献   

20.
The process of water drop evaporation in a field of intense laser radiation is examined on the basis of the hydro-thermodynamics equations under the assumption of quasistationarity in the conditions in the surrounding medium and in the radius. The influence of the accommodation coefficient on heating of the drops on the magnitude of the surface jump in water vapor density and on the position of the upper bound of the convective evaporation region is analyzed. It is shown that the surface jump in the vapor does not alter the rate of convective evaporation of the drop in practice, but can result in substantially different time dependences of the radius of a diffusely evaporating drop as compared with those found without it. The solution obtained is compared with the solution of the problem of evaporation in a Stefan approximation.  相似文献   

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