Korobko A V, van den Ende D, Agterof W G M, Mellema J
Physics of Complex Fluids, Institute of Mechanics, Processes and Control-Twente (IMPACT) and J.M. Burgerscentrum, Department of Science and Technology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands.
J Chem Phys. 2005 Nov 22;123(20):204908. doi: 10.1063/1.2121627.
The coalescence frequency in emulsions containing droplets with a low viscosity (viscosity ratio approximately 0.005) in simple shear flow has been investigated experimentally at several volume fractions of the dispersed phase (2%-14%) and several values of the shear rate (0.1-10 s(-1)). The evolution of the size distribution was monitored to determine the average coalescence probability from the decay of the total number of droplets. Theoretically models for two-droplet coalescence are considered, where the probability is given by P(c)=exp(-tau(dr)tau(int)). Since the drainage time tau(dr) depends on the size of the two colliding droplets, and the collision time tau(int) depends on the initial orientation of the colliding droplets, the calculated coalescence probability was averaged over the initial orientation distribution and the experimental size distribution. This averaged probability was compared to the experimentally obtained coalescence frequency. The experimental results indicate that (1) to predict the average coalescence probability one has to take into account the full size distribution of the droplets; (2) the coalescence process is best described by the "partially mobile deformable interface" model or the "fully immobile deformable interface" model of Chesters [A. K. Chesters, Chem. Eng. Res. Des. 69, 259 (1991)]; and (3) independent of the models used it was concluded that the ratio tau(dr)tau(int) scales with the coalescence radius to a power (2+/-1) and with the rate of shear to a power (1.5+/-1). The critical coalescence radius R(o), above which hardly any coalescence occurs is about 10 microm.
在简单剪切流中,针对分散相体积分数为2%-14%且剪切速率为0.1-10 s⁻¹的几种情况,对含有低粘度液滴(粘度比约为0.005)的乳液中的聚并频率进行了实验研究。监测尺寸分布的演变,以根据液滴总数的衰减确定平均聚并概率。考虑了两液滴聚并的理论模型,其中概率由P(c)=exp(-τ(dr)τ(int))给出。由于排水时间τ(dr)取决于两个碰撞液滴的尺寸,而碰撞时间τ(int)取决于碰撞液滴的初始取向,因此计算得到的聚并概率是在初始取向分布和实验尺寸分布上进行平均的。将这种平均概率与实验获得的聚并频率进行比较。实验结果表明:(1) 要预测平均聚并概率,必须考虑液滴的完整尺寸分布;(2) 聚并过程最好用切斯特斯的“部分可移动可变形界面”模型或“完全不可移动可变形界面”模型来描述 [A. K. 切斯特斯,《化学工程研究与设计》69, 259 (1991)];(3) 无论使用何种模型,都得出τ(dr)τ(int)的比值与聚并半径的幂次方(2±1)以及剪切速率的幂次方(1.5±1)成比例的结论。几乎不发生聚并的临界聚并半径R(o)约为10微米。