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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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Geometry of locomotion of the generalized Purcell's swimmer : Modelling and controllability.

Sudin Kadam, +1 more
- 16 Nov 2016 - 
TL;DR: This work proposes and study a generalized 3-link robotic swimmer inspired by the planar Purcell's swimmer at low Reynolds number, and presents a local controllability analysis of the Swimmer at the low ReynoldsNumber regime using weak controllable results of the planars.
Journal ArticleDOI

Propulsive Effect of Wall Vibrations

TL;DR: In this article , a model consisting of two parallel plates free to move with respect to each other was used to assess the effectiveness of wall vibrations in the form of travelling waves, and three types of responses were identified: a sloshing response for long waves, a moving wall response for short waves and an intermediate response for in-between waves.
Journal ArticleDOI

Simple analytic model for peristaltic flow and mixing

TL;DR: In this paper, a simple analytic model for small-amplitude peristaltic flows was presented, validated using simulations and measurements from a laboratory model of the inner ear. And they demonstrated that Lagrangian transport dynamics can be accurately reproduced accurately with their simple analytical model.
Posted Content

Effect of body deformability on microswimming

TL;DR: In this paper, the authors consider a microswimmer model composed of deformable beads connected with springs and determine the velocity of the swimmer analytically, starting from the forces driving the motion and assuming that the oscillations in the effective radii of the beads are known and are much smaller than the radii themselves.
Journal ArticleDOI

Frequency dependence of surface acoustic wave swimming.

TL;DR: Improved understanding of SAW swimming provides a test-bed for exploring the science of microorganism swimming, and could bring new insight to the evolutionary significance for the length and beating frequency of swimming microbial flagella.
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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