Menzel Andreas M, Saha Arnab, Hoell Christian, Löwen Hartmut
Institut für Theoretische Physik II, Weiche Materie, Heinrich-Heine-Universität Düsseldorf, 40225 Düsseldorf, Germany.
J Chem Phys. 2016 Jan 14;144(2):024115. doi: 10.1063/1.4939630.
Dynamical density functional theory (DDFT) has been successfully derived and applied to describe on one hand passive colloidal suspensions, including hydrodynamic interactions between individual particles. On the other hand, active "dry" crowds of self-propelled particles have been characterized using DDFT. Here, we go one essential step further and combine these two approaches. We establish a DDFT for active microswimmer suspensions. For this purpose, simple minimal model microswimmers are introduced. These microswimmers self-propel by setting the surrounding fluid into motion. They hydrodynamically interact with each other through their actively self-induced fluid flows and via the common "passive" hydrodynamic interactions. An effective soft steric repulsion is also taken into account. We derive the DDFT starting from common statistical approaches. Our DDFT is then tested and applied by characterizing a suspension of microswimmers, the motion of which is restricted to a plane within a three-dimensional bulk fluid. Moreover, the swimmers are confined by a radially symmetric trapping potential. In certain parameter ranges, we find rotational symmetry breaking in combination with the formation of a "hydrodynamic pumping state," which has previously been observed in the literature as a result of particle-based simulations. An additional instability of this pumping state is revealed.
动态密度泛函理论(DDFT)已成功推导出来,并一方面应用于描述被动胶体悬浮液,包括单个粒子之间的流体动力学相互作用。另一方面,自驱动粒子的活性“干”群体已使用DDFT进行了表征。在此,我们更进一步,将这两种方法结合起来。我们建立了一种用于活性微游动者悬浮液的DDFT。为此,引入了简单的最小模型微游动者。这些微游动者通过使周围流体运动来实现自我推进。它们通过主动自诱导的流体流动以及通过共同的“被动”流体动力学相互作用,在流体动力学上相互作用。还考虑了有效的软空间排斥作用。我们从常见的统计方法出发推导DDFT。然后,通过表征微游动者的悬浮液来测试和应用我们的DDFT,这些微游动者的运动被限制在三维体流体中的一个平面内。此外,游动者受到径向对称的捕获势的限制。在某些参数范围内,我们发现旋转对称性破缺与“流体动力学泵送状态”的形成相结合,这在文献中先前已通过基于粒子的模拟观察到。揭示了这种泵送状态的另一种不稳定性。