4.6 Article

Buckling of elastic fibers in a shear flow

Journal

NEW JOURNAL OF PHYSICS
Volume 24, Issue 1, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1367-2630/ac43eb

Keywords

Stokes flow; flexible fibers; bending; buckling; orientational order

Funding

  1. National Science Centre [UMO-2018/31/B/ST8/03640]
  2. NSF [CMMI-1661672]
  3. Princeton Center for Complex Materials (PCCM)
  4. National Science Foundation (NSF)-MRSEC program [DMR-2011750]
  5. Polish National Agency for Academic Exchange [PPI/APM/2018/1/00045]

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The study focuses on the three-dimensional dynamics of flexible fibers in shear flow, showing that fibers rotate along effective Jeffery orbits and become aligned with the flow direction in the flow-vorticity plane. Compressional buckling of fibers can occur in a short time, indicating differences between local and compressional bending and their dependence on the initial fiber orientation and the bending stiffness ratio A.
Three-dimensional dynamics of flexible fibers in shear flow are studied numerically, with a qualitative comparison to experiments. Initially, the fibers are straight, with different orientations with respect to the flow. By changing the rotation speed of a shear rheometer, we change the ratio A of bending to shear forces. We observe fibers in the flow-vorticity plane, which gives insight into the motion out of the shear plane. The numerical simulations of moderately flexible fibers show that they rotate along effective Jeffery orbits, and therefore the fiber orientation rapidly becomes very close to the flow-vorticity plane, on average close to the flow direction, and the fiber remains in an almost straight configuration for a long time. This 'ordering' of fibers is temporary since they alternately bend and straighten while tumbling. We observe numerically and experimentally that if the fibers are initially in the compressional region of the shear flow, they can undergo compressional buckling, with a pronounced deformation of shape along their whole length during a short time, which is in contrast to the typical local bending that originates over a long time from the fiber ends. We identify differences between local and compressional bending and discuss their competition, which depends on the initial orientation of the fiber and the bending stiffness ratio A. There are two main finding. First, the compressional buckling is limited to a certain small range of the initial orientations, excluding those from the flow-vorticity plane. Second, since fibers straighten in the flow-vorticity plane while tumbling, the compressional buckling is transient-it does not appear for times longer than 1/4 of the Jeffery period. For larger times, bending of fibers is always driven by their ends.

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