Zhang Xiao, Graham Michael D
Department of Chemical and Biological Engineering University of Wisconsin-Madison, Madison, WI 53706-1691.
Phys Rev Fluids. 2020 Feb;5(2). doi: 10.1103/physrevfluids.5.023603. Epub 2020 Feb 28.
This work investigates the orbital dynamics of a fluid-filled deformable prolate capsule in unbounded simple shear flow at zero Reynolds number using direct simulations. The motion of the capsule is simulated using a model that incorporates shear elasticity, area dilatation, and bending resistance. Here the deformability of the capsule is characterized by the nondimensional capillary number Ca, which represents the ratio of viscous stresses to elastic restoring stresses on the capsule. For a capsule with small bending stiffness, at a given Ca, the orientation converges over time towards a unique stable orbit independent of the initial orientation. With increasing Ca, four dynamical modes are found for the stable orbit, namely, rolling, wobbling, oscillating-swinging, and swinging. On the other hand, for a capsule with large bending stiffness, multiplicity in the orbit dynamics is observed. When the viscosity ratio ≲ 1, the long-axis of the capsule always tends towards a stable orbit in the flow-gradient plane, either tumbling or swinging, depending on Ca. When ≳ 1, the stable orbit of the capsule is a tumbling motion at low Ca, irrespective of the initial orientation. Upon increasing Ca, there is a symmetry-breaking bifurcation away from the tumbling orbit, and the capsule is observed to adopt multiple stable orbital modes including nonsymmetric precessing and rolling, depending on the initial orientation. As Ca further increases, the nonsymmetric stable orbit loses existence at a saddle-node bifurcation, and rolling becomes the only attractor at high Ca, whereas the rolling state coexists with the nonsymmetric state at intermediate values of Ca. A symmetry-breaking bifurcation away from the rolling orbit is also found upon decreasing Ca. The regime with multiple attractors becomes broader as the aspect ratio of the capsule increases, while narrowing as viscosity ratio increases. We also report the particle contribution to the stress, which also displays multiplicity.
本研究通过直接模拟,研究了零雷诺数下无限大简单剪切流中充满流体的可变形扁长胶囊的轨道动力学。使用一个包含剪切弹性、面积膨胀和抗弯性的模型来模拟胶囊的运动。在此,胶囊的可变形性由无量纲毛细管数Ca表征,它代表胶囊上粘性应力与弹性恢复应力之比。对于弯曲刚度较小的胶囊,在给定的Ca下,其取向会随时间收敛到一个与初始取向无关的唯一稳定轨道。随着Ca的增加,稳定轨道出现了四种动力学模式,即滚动、摆动、振荡摆动和摆动。另一方面,对于弯曲刚度较大的胶囊,轨道动力学中观察到了多重性。当粘度比≲1时,胶囊的长轴总是趋向于流梯度平面中的一个稳定轨道,根据Ca的不同,可能是翻滚或摆动。当≳1时,在低Ca下,胶囊的稳定轨道是翻滚运动,与初始取向无关。随着Ca的增加,会出现从翻滚轨道的对称破缺分岔,观察到胶囊根据初始取向采用多种稳定轨道模式,包括非对称进动和滚动。随着Ca进一步增加,非对称稳定轨道在鞍结分岔处消失,在高Ca下滚动成为唯一的吸引子,而在Ca的中间值时,滚动状态与非对称状态共存。在Ca减小时,也发现了从滚动轨道的对称破缺分岔。随着胶囊纵横比的增加,具有多个吸引子的区域变宽,而随着粘度比的增加变窄。我们还报告了颗粒对应力的贡献,其也表现出多重性。