共查询到17条相似文献,搜索用时 171 毫秒
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旋转工作的机械零部件和机械设备的润滑系统工作过程中普遍存在着油滴和油膜的碰撞行为,这一行为易引起气泡夹带现象.气泡将对油滴撞击油膜时的运动过程和附壁油膜层的形成质量造成不可忽视的影响.基于耦合的水平集-体积分数方法,对油滴撞击含气泡油膜的行为进行数值模拟研究,考察油膜层内气泡的变形运动过程,分析气泡大小和位置等因素对撞击过程中气泡变形特征参数的影响规律,并探讨气泡破裂的动力学机制.研究表明,随着气泡直径的增大,油滴撞击含气泡油膜后气泡会依次出现自由表面破裂、稳定变形以及油膜内部破裂等现象;直径d=20μm的气泡能较稳定地存在于油膜层内,同时该值也是气泡发生自由表面破裂和油膜内部破裂的临界值.此外,气泡所在位置同样对气泡变形历程有一定影响,气泡越接近油膜表面,其变形量越大;位于油膜底层的气泡会附着在壁面上.在自由表面破裂和油膜内部破裂过程中,气泡破裂是由气-液界面不稳定引起的,表面张力对这两种现象起重要作用;而黏性剪切力对油膜内部破裂现象也有着不可忽视的影响. 相似文献
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为探究闪蒸喷雾冷却的微观机理, 设计并搭建了液滴悬挂式真空闪蒸实验装置, 利用可视化窗口探究Tween20 液滴闪蒸过程中的闪蒸特性及气泡生长机理. 液滴在快速降压过程中形态会经历气泡成核、气泡生长、伴随气泡生长、爆裂这四个阶段的变化, 并反复循环这一过程直至液滴稳定蒸发. 对于液滴温度的变化, 闪蒸室的终态压力起到了决定性的作用, 并且其终态温度随压力的升高明显上升. 同时通过液滴闪蒸过程形态图分析发现, 液滴在剧烈爆炸阶段其温度也发生明显下降; 在稳定蒸发阶段, 其温度也将开始稳定不变. 因此可知液滴的剧烈爆炸会带走其自身的大量热量. 而 Tween20 浓度对液滴温度的影响微乎其微, 但其会使液滴内气泡的初始成核时间发生明显滞后, 并抑制液滴内的气泡发生破裂. 相似文献
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采用高速摄像仪以10000 帧/s的拍摄速度对液滴低速撞击润湿球体表面过程进行了实验观测, 分析了液滴撞击后的反弹、局部反弹和铺展等现象, 考察了黏度对撞击过程的影响; 在此基础上, 定量讨论了液滴铺展特征参数随撞击速度、球体直径和黏度的变化规律. 观测发现: 黏度较大且撞击速度较低时, 撞击后可能出现反弹和局部反弹, 黏度较小时则不发生; 铺展面积随撞击速度的增大而增大; 黏度增大时, 铺展因子减小; 在球体直径为4–20 mm范围内, 随着球体直径的增加, 铺展因子呈上升趋势.
关键词:
液滴撞击
润湿球面
铺展
黏度 相似文献
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本文以光滑石墨膜作为加热表面,在标准大气压下以去离子水为工质进行了饱和池式沸腾实验。实验研究表明,在热流密度达到1.83 MW/m^2时,石墨膜发生膨胀并使其表面局部破裂,随着热流密度的进一步升高,破裂的面积逐渐扩大,石墨膜的电阻呈现阶跃式升高。在2.40 MW/m^2的热流密度下,石墨膜表面全部破裂,此后随着热流密度增加,电阻上升幅度变小,最终,在热流密度达到3.17 MW/m^2时,石墨膜发生烧毁。可见,石墨膜通过膨胀破裂的方式能自适应地强化沸腾传热临界热流密度,强化比例达到73%。同时,通过高速摄像机的观察发现,在相同热流密度条件下,与光滑表面相比,膨胀表面的气化核心数增多,气泡脱离直径变小,气泡脱离频率变大。 相似文献
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Yoshiyuki Suzuki Takuji Harada Hirotatsu Watanabe Masakazu Shoji Yohsuke Matsushita Hideyuki Aoki Takatoshi Miura 《Proceedings of the Combustion Institute》2011,33(2):2063-2070
The effect of aggregation of dispersed water droplets on secondary atomization of emulsified fuel droplets in a heating process was investigated. Secondary atomization was observed using a single droplet experiment in which a water-in-oil (W/O) emulsified fuel droplet prepared using colored water was heated by a halogen heater. The initial diameter of dispersed water droplets before heating was controlled, and the change in the diameter of dispersed water droplets was measured by image analysis. As a result, the aggregation process of dispersed water droplets in the heating process was successfully visualized. The dispersed water droplet diameter increased with an increase in W/O emulsified fuel droplet temperature. The occurrence probability of micro-explosion increased with an increase in the dispersed water droplet diameter in emulsified fuel droplets. It is suggested that the occurrence probability of micro-explosion can be increased by accelerating the aggregation and coalescence of dispersed water droplets below 430 K, which is the average temperature of the starting point of puffing. 相似文献
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以水气两相流为研究对象, 采用大涡模拟和流体体积法, 结合破碎准则和第三代涡识别方法对双气泡碰撞过程进行数值模拟。采用单一变量法, 研究气泡直径比、相对偏心距及气泡间相对距离对气泡破碎程度的影响。双气泡碰撞过程中, 两气泡的直径越接近时, 碰撞过程中的气泡破碎程度越弱, 偏心距的变化对气泡破碎程度影响不大。而相对距离小于1时, 随着其增大, 气泡碰撞过程中的破碎程度更加明显。当气泡相对距离大于1时, 气泡破碎程度趋于平缓。研究表明: 第三代涡识别方法能够很好地捕捉两相流湍流流场中漩涡位置, 并能敏锐地反映出湍流的变化。 相似文献
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The growth and departure of bubbles on a vertical heated wall of an annular channel in flow boiling were observed by a high-speed camera, and the bubble contact diameter and bubble departure diameter were measured. It was found that bubble departure diameters were different among different nucleation sites in the same boiling area (same test condition, same surface roughness). Force balance on a single bubble attached to the heated surface was also analyzed to explain this phenomenon. The theoretical research results show that bubble contact diameter has a significant influence on bubble departure diameter, and the corresponding departure diameter is larger as the bubble contact diameter is larger. This agrees with the visual experimental results. 相似文献
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The dynamics of growth and interaction of vapor bubbles in droplets of pure water and LiBr water solution on a horizontal wall were investigated in a wide superheating range. The growth rates of bubbles were determined both in a distillate droplet and in a salt solution droplet. The bubble growth rate in a pure water droplet at the final stage is somewhat lower than in pool boiling. The bubble growth rate in a salt solution is substantially lower than for pure water. Due to the bubble density maldistribution, the vapor flow density is appreciably higher at the droplet edges than on the droplet axis. Collective behavior of the bubbles possesses both stochastic character and elements of self-organization. The thermal measurements were carried out by means of high-speed video and blowup thermal imager. 相似文献
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在通过引入精确差分方法的单组分多相格子Boltzmann模型的基础上耦合能量方程,并考虑流体与固壁间的相互作用力来调节气泡与固壁间的接触角,从而建立了一种新的描述气液相变的格子Boltzmann理论模型. 为验证该模型的正确性,利用其对工质为水的相变过程进行了模拟,发现模拟结果与实验值符合良好;进而利用其验证Laplace定律,发现计算所得的水的表面张力与实验值甚为符合. 为考察该模型处理复杂相变问题的能力,利用其对工质为水的池沸腾中的气泡生长过程进行模拟,发现气泡脱离直径与g-0
关键词:
格子Boltzmann方法
池沸腾
气泡生长过程
接触角 相似文献
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The effect of the heating rate on the nucleation of metallic glass in a rapid heating process starting from the glass transition temperature is investigated. The critical nucleus radius increases with the increase of the temperature of the undercooling liquid. If the increment rate of the critical nucleus radius, owing to the heating process, is higher than the growth rate of the nuclei, the nuclei generated at the low temperature will become the embryos at the high temperature. This means that the high heating rate can make no nucleation happen in the heating process. In consideration of the interfacial energy, the growth rate of the nuclei increases with the increase of their size and the growth rate of the critical nucleus is zero. Thus, the lower heating rate can also make the nuclei decline partially. Finally, this theory is used to analyze the nucleation process during laser remelting metallic glass. 相似文献
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《中国物理 B》2021,30(5):54703-054703
Partial coalescence is a complicated flow phenomenon. In the present study, the coalescence process is simulated with the volume of fluid(VOF) method. The numerical results reveal that a downward high-velocity region plays a significant role in partial coalescence. The high-velocity region pulls the droplet downward continuously which is an important factor for the droplet turning into a prolate shape and the final pinch-off. The shift from partial coalescence to full coalescence is explained based on the droplet shape before the pinch-off. With the droplet impact velocity increasing, the droplet shape will get close to a sphere before the pinch-off. When the shape gets close enough to a sphere, the partial coalescence shifts to full coalescence. The effect of film thickness on the coalescence process is also investigated. With large film thickness,partial coalescence happens, while with small film thickness, full coalescence happens. In addition, the results indicate that the critical droplet impact velocity increases with the increase of surface tension coefficient but decreases with the increase of viscosity and initial droplet diameter. And there is a maximum critical Weber number with the increase of surface tension coefficient and initial droplet diameter. 相似文献