Abstract

It has long been known that some microswimmers seem to swim counter-intuitively faster when the viscosity of the surrounding fluid is increased, whereas others slow down. This conflicting dependence of the swimming velocity on the viscosity is poorly understood theoretically. Here we explain that any mechanical microswimmer with an elastic degree of freedom in a simple Newtonian fluid can exhibit both kinds of response to an increase in the fluid viscosity for different viscosity ranges, if the driving is weak. The velocity response is controlled by a single parameter Γ, the ratio of the relaxation time of the elastic component of the swimmer in the viscous fluid and the swimming stroke period. This defines two velocity–viscosity regimes, which we characterize using the bead-spring microswimmer model and analyzing the different forces acting on the parts of this swimmer. The analytical calculations are supported by lattice-Boltzmann simulations, which accurately reproduce the two velocity regimes for the predicted values of Γ.

Highlights

  • It was discovered a few decades ago that many micro-organisms swim faster in more viscous fluids than in less viscous ones

  • We explain that any mechanical microswimmer with an elastic degree of freedom in a simple Newtonian fluid can exhibit both kinds of response to an increase in the fluid viscosity for different viscosity ranges, if the driving is weak

  • In this work we have shown that for a fluid-active particle system involving an elastic degree of freedom, the competition between the characteristic time scales associated with the driving and with the elastic relaxation is sufficient for a non-monotonic velocity–viscosity response

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Summary

26 May 2017

Division of Physical Chemistry, Ruđer Bošković Institute, Bijenička cesta 54, 10000 Zagreb, Croatia licence

Introduction
Analytical swimmer model
Characteristics of the swimming regimes
Conclusion
Details of the different simulations presented in figure 4
Velocity expression for unequal spring constants

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