Abstract

The three-dimensional dynamics of a single non-Brownian flexible fiber in shear flow is evaluated numerically, in the absence of inertia. A wide range of ratios A of bending to hydrodynamic forces and hundreds of initial configurations are considered. We demonstrate that flexible fibers in shear flow exhibit much more complicated evolution patterns than in the case of extensional flow, where transitions to higher-order modes of characteristic shapes are observed when A exceeds consecutive threshold values. In shear flow, we identify the existence of an attracting steady configuration and different attracting periodic motions that are approached by long-lasting rolling, tumbling, and meandering dynamical modes, respectively. We demonstrate that the final stages of the rolling and tumbling modes are effective Jeffery orbits, with the constant parameter C replaced by an exponential function that either decays or increases in time, respectively, corresponding to a systematic drift of the trajectories. In the limit of C→0, the fiber aligns with the vorticity direction and in the limit of C→∞, the fiber periodically tumbles within the shear plane. For moderate values of A, a three-dimensional meandering periodic motion exists, which corresponds to intermediate values of C. Transient, close to periodic oscillations are also detected in the early stages of the modes.

Highlights

  • In nature and modern technologies, there are many systems containing elongated, flexible, micrometer- and nanometerscale objects deforming and moving in a fluid flow [1]

  • It has been shown that the typical pattern of a fiber’s evolution in extensional flow is related to consecutive threshold values of the characteristic ratio of bending to hydrodynamic forces exerted by the fluid flow

  • In this article we provide a new perspective on the threedimensional evolution of flexible fiber shapes in shear flow

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Summary

INTRODUCTION

In nature and modern technologies, there are many systems containing elongated, flexible, micrometer- and nanometerscale objects deforming and moving in a fluid flow [1]. We show that after a relaxation phase, a flexible fiber is attracted to one of several stationary, periodic, or close to periodic solutions, with different typical sequences of shapes and orientations Features of these characteristic solutions, their presence or absence, stability or instability, and basins of attraction depend on the ratio A of local bending E π d2/64 to hydrodynamic π ηγd forces, where E is the Young’s modulus, d is the fiber diameter, and η is the fluid’s dynamic viscosity. As we document in this article, in shear flow (in contrast to extensional flow), the value of the bending-to-hydrodynamic ratio A does not uniquely determine the type of the fiber shape This conclusion is based on two main features of the dynamics. Longlasting, chaotic transients are typical: we document close to periodic motions that later spontaneously change into periodic or effective Jeffery motions with different shape sequences

Elastic fiber
Initial fiber configurations
Fiber dynamics in flow
ATTRACTING MODES OF THE DYNAMICS
THE ATTRACTORS
DEPENDENCE OF THE DYNAMICS ON THE
COMPARISON WITH JEFFERY ORBITS
Jeffery orbits
Rolling and tumbling modes
Meandering modes
Physical interpretation
DISCUSSION AND CONCLUSIONS
Findings
653. Supplemental
Full Text
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