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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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Hydrodynamic Impedance Correction for Reduced-Order Modeling and Real-Time Control of Spermatozoa-Like Soft Micro-Robots for Medicine

TL;DR: In this study, an analysis strategy is proposed to improve the RFT-based analysis, particularly for spermatozoa and spermatoozoa-inspired micro-swimmers with elastic slender tails, in order to present a practical solution to the problem.
Journal ArticleDOI

Modelling of energy expended by free swimming spermatozoa in temperature-dependent viscous semen

TL;DR: The results suggest that the probability of spermatozoa colliding in relatively lower viscous semen increases for a denser concentration of spermutozoa due to the limited semen volume available to manoeuvre, and the described derivations herein can assist in the understanding of work done by a normal motile spermatozoon in a pool of semen.
Journal ArticleDOI

Two-dimensional Brinkman flows and their relation to analogous Stokes flows

TL;DR: In this paper, it was shown that Brinkman flows do not exhibit a Stokes-like paradox and that they can flow past a rigid circular cylinder and flow through a thin rigid strip.
Journal ArticleDOI

Swimming near Deformable Membranes at Low Reynolds Number

TL;DR: In this paper, the speed of an infinitely long swimmer close to a flexible surface separating two fluids was investigated, and the deformation and swimming speed of the flexible surface was also calculated.
Posted Content

On the locomotion and control of a self-propelled shape-changing body in a uid

TL;DR: In this paper, the authors study the locomotion of a shape-changing body swimming in a two-dimensional perfect manifold of infinite extent. And they show how the control problem, consisting in associating with each shape-change the resulting trajectory of the swimming body, can be analyzed within the framework of geometric control theory.
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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