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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

Squirming motion in a Brinkman medium

TL;DR: In this paper, the authors analyse the characteristics of swimming in a porous medium modelled by the Brinkman equation via a spherical squirmer model and calculate the power dissipation and hence the swimming efficiency of the squirmers.
Posted Content

Elastohydrodynamic Synchronization of Adjacent Beating Flagella

TL;DR: An asymptotic analysis of the hydrodynamic coupling between two extended filaments in the regime d/L ≪ 1 is presented, and it is found that the form of the coupling is independent of the microscopic details of the internal forces that govern the motion of the individual filaments.
Journal ArticleDOI

Effective shear viscosity and dynamics of suspensions of micro-swimmers from small to moderate concentrations.

TL;DR: These findings prove that a physically observable decrease of viscosity for a suspension of self-propelled microswimmers can be explained purely by hydrodynamic interactions and self-propulsion and interaction of swimmers are both essential to the reduction of the effective shear viscosities.
Journal ArticleDOI

A coordinate-based proof of the scallop theorem ∗

TL;DR: With an exact definition of deformation of a swimmer, a coordinate-based proof is first given to Purcell's scallop theorem including the body rotation to reconsider fluid dynamics for a self-propulsive swimmer in Stokes flow.
Journal ArticleDOI

Propulsion of an artificial nanoswimmer: a comprehensive review

TL;DR: A review of various propulsion mechanisms for moving a nanoswimmer using chemical fuel, magnetic fields, ultrasonic pulses and thrust force generated by bacteria in the presence of external stimuli including laser light, and thermal and chemical gradients is presented in this article.
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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