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Dynamics of ferrofluidic flow in the Taylor-Couette system with a small aspect ratio

机译:纵横比较小的Taylor-Couette系统中的铁磁流体动力学

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摘要

We investigate fundamental nonlinear dynamics of ferrofluidic Taylor-Couette flow - flow confined be-tween two concentric independently rotating cylinders - consider small aspect ratio by solving the ferro-hydrodynamical equations, carrying out systematic bifurcation analysis. Without magnetic field, we find steady flow patterns, previously observed with a simple fluid, such as those containing normal one- or two vortex cells, as well as anomalous one-cell and twin-cell flow states. However, when a symmetry-breaking transverse magnetic field is present, all flow states exhibit stimulated, finite two-fold mode. Various bifurcations between steady and unsteady states can occur, corresponding to the transitions between the two-cell and one-cell states. While unsteady, axially oscillating flow states can arise, we also detect the emergence of new unsteady flow states. In particular, we uncover two new states: one contains only the azimuthally oscillating solution in the configuration of the twin-cell flow state, and an-other a rotating flow state. Topologically, these flow states are a limit cycle and a quasiperiodic solution on a two-torus, respectively. Emergence of new flow states in addition to observed ones with classical fluid, indicates that richer but potentially more controllable dynamics in ferrofluidic flows, as such flow states depend on the external magnetic field.
机译:我们研究了铁磁流体Taylor-Couette流动的基本非线性动力学-限制在两个同心独立旋转的圆柱体之间的流动-通过求解铁磁流体动力学方程来考虑小长宽比,进行系统的分叉分析。在没有磁场的情况下,我们会找到稳定的流动模式,这种流动模式以前是用简单的流体观察到的,例如包含正常的一或两个涡流池的流体,以及异常的一池和双池流动状态。但是,当存在破坏对称性的横向磁场时,所有流动状态均表现出受激有限的两倍模式。可能会在稳态和非稳态之间发生各种分歧,这对应于两个单元状态和一个单元状态之间的转换。虽然可能会出现不稳定的轴向振荡流动状态,但我们也检测到新的不稳定流动状态的出现。特别是,我们发现了两个新的状态:一个仅包含双池流动状态配置中的方位角振荡解,另一个包含旋转流动状态。在拓扑上,这些流动状态分别是一个极限环和一个在两个环上的拟周期解。除了观察到的经典流体外,新的流态的出现还表明铁磁流体中的动力学更丰富,但可能更可控,因为这种流态取决于外部磁场。

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