用“准三维”数值模拟方法研究吹气发泡法制备泡沫铝的过程中,单个气泡在铝熔液搅拌流场中的运动与变形。液体流场采用多重参考系法进行三维模拟,对气泡运动的二维模拟则在三维流场中的一个通过搅拌轴的特征平面上进行。这样既能捕获气...用“准三维”数值模拟方法研究吹气发泡法制备泡沫铝的过程中,单个气泡在铝熔液搅拌流场中的运动与变形。液体流场采用多重参考系法进行三维模拟,对气泡运动的二维模拟则在三维流场中的一个通过搅拌轴的特征平面上进行。这样既能捕获气泡在搅拌流场中运动的基本特征,又能大大降低计算成本。应用流体体积分数(volume of fluid,VOF)方法对气液两相之间的界面进行追踪。通过对不同表面张力气泡的计算,总结出流场中关于气泡运动路径和导致气泡变形直至破碎的三种主要机理。展开更多
The physical circumstances inside an acoustically driven single gas bubble in water has been intensively explored during the past few years. Starting from the results obtained for a typical case in a well known early ...The physical circumstances inside an acoustically driven single gas bubble in water has been intensively explored during the past few years. Starting from the results obtained for a typical case in a well known early paper (Wu, C. C., Roberts, P. H., Phys. Rev. Lett., 1993, 70(22): 3424) and introducing successively several corrections to the physical model, this paper computes in corresponding order the temporal and spatial distributions of significant physical parameters, including the temperature and the pressure, in the bubble around the moment of the bubble's violent collapse, until expectations in consistence with the present points of view are procured. For the peak temperature our results agree with the prevailing belief that in a typical stable single bubble it is of the order of ten thousand degrees.展开更多
文摘用“准三维”数值模拟方法研究吹气发泡法制备泡沫铝的过程中,单个气泡在铝熔液搅拌流场中的运动与变形。液体流场采用多重参考系法进行三维模拟,对气泡运动的二维模拟则在三维流场中的一个通过搅拌轴的特征平面上进行。这样既能捕获气泡在搅拌流场中运动的基本特征,又能大大降低计算成本。应用流体体积分数(volume of fluid,VOF)方法对气液两相之间的界面进行追踪。通过对不同表面张力气泡的计算,总结出流场中关于气泡运动路径和导致气泡变形直至破碎的三种主要机理。
基金This work was supported by the National Natural Science Foundation of China (Grant No. 19934001).
文摘The physical circumstances inside an acoustically driven single gas bubble in water has been intensively explored during the past few years. Starting from the results obtained for a typical case in a well known early paper (Wu, C. C., Roberts, P. H., Phys. Rev. Lett., 1993, 70(22): 3424) and introducing successively several corrections to the physical model, this paper computes in corresponding order the temporal and spatial distributions of significant physical parameters, including the temperature and the pressure, in the bubble around the moment of the bubble's violent collapse, until expectations in consistence with the present points of view are procured. For the peak temperature our results agree with the prevailing belief that in a typical stable single bubble it is of the order of ten thousand degrees.
