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Journal ArticleDOI

Analysis of the Swimming of Microscopic Organisms

Geoffrey Ingram Taylor
- 22 Nov 1951 - 
- Vol. 209, Iss: 1099, pp 447-461
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TLDR
In this article, it was shown that if the waves down neighbouring tails are in phase, very much less energy is dissipated in the fluid between them than when the waves are in opposite phase.
Abstract
Large objects which propel themselves in air or water make use of inertia in the surrounding fluid. The propulsive organ pushes the fluid backwards, while the resistance of the body gives the fluid a forward momentum. The forward and backward momenta exactly balance, but the propulsive organ and the resistance can be thought about as acting separately. This conception cannot be transferred to problems of propulsion in microscopic bodies for which the stresses due to viscosity may be many thousands of times as great as those due to inertia. No case of self-propulsion in a viscous fluid due to purely viscous forces seems to have been discussed. The motion of a fluid near a sheet down which waves of lateral displacement are propagated is described. It is found that the sheet moves forwards at a rate 2π 2 b 2 /λ 2 times the velocity of propagation of the waves. Here b is the amplitude and λ the wave-length. This analysis seems to explain how a propulsive tail can move a body through a viscous fluid without relying on reaction due to inertia. The energy dissipation and stress in the tail are also calculated. The work is extended to explore the reaction between the tails of two neighbouring small organisms with propulsive tails. It is found that if the waves down neighbouring tails are in phase very much less energy is dissipated in the fluid between them than when the waves are in opposite phase. It is also found that when the phase of the wave in one tail lags behind that in the other there is a strong reaction, due to the viscous stress in the fluid between them, which tends to force the two wave trains into phase. It is in fact observed that the tails of spermatozoa wave in unison when they are close to one another and pointing the same way.

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Citations
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Journal ArticleDOI

Thrifty swimming with shear-thinning

TL;DR: It is demonstrated that failing to account for "out-of-plane" effects when analysing experimental data of undulatory swimming through a shear-thinning fluid results in a significant overestimate of fluid viscosity around the model swimmer C. elegans, a key biophysical quantity important for understanding the internal mechanics of the swimmer.
Journal ArticleDOI

An ALE-based finite element model of flagellar motion driven by beating waves

TL;DR: By taking non-Newtonian fluids into account, a computational model of flagellar motility is presented using the finite element method and it is found that the model microorganism swims much more efficiently in shear-thinning fluids.
Journal ArticleDOI

Two-dimensional flagellar synchronization in viscoelastic fluids

TL;DR: In this article, it was shown that the presence of polymeric stresses removes the geometrical asymmetry constraint, and therefore even symmetric swimmers synchronize on asymptotic faster time scales than in a Newtonian fluid.
Journal ArticleDOI

The role of vibrations for reducing the resistance in the relative movement of parallel plates

TL;DR: In this article , the effect of surface vibrations on the propulsion augmentation and resistance in the relative movement of parallel plates has been studied and the effectiveness of the vibrations was gauged by determining the external force required to maintain the movement of one of the plates at a prescribed velocity.
Proceedings ArticleDOI

Artificial magnetic nano-swimmer in drug delivery

TL;DR: In this paper a nano-swimmer with length between 10 to 100nm consisting of a motor, filament and hinged boundaries is controlled by mathematical simulations successfully and a nanoswimmer that lies in a heterodimer magnetic nano-particle is proposed based on existed nano-robots.
References
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Journal ArticleDOI

Sea-urchin spermatozoa.

Lord Rothschild
- 01 Feb 1951 - 
TL;DR: The head of the sea‐urchin spermatozoon is pear‐shaped and axially symmetrical, and the tail, which terminates in an axial fibre, probably contains spiral or coiled structures, as in mammalian spermatozoa.
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