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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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Rotational dynamics of a soft filament: Wrapping transition and propulsive forces

TL;DR: In this article, the shape of a long elastic filament rotating in a viscous liquid was analyzed and the authors identified a continuous but sharp transition from a straight to an helical shape, resulting from the competition between viscous stresses and elastic forces.
Journal ArticleDOI

Exact solutions for hydrodynamic interactions of two squirming spheres

TL;DR: In this paper, exact solutions of the Stokes equations for a squirming sphere close to a no-slip surface, both planar and spherical, and for the interactions between two squirmers, in three dimensions were provided.
Journal ArticleDOI

Breakup of a Fluid Thread in a Confined Geometry: Droplet-Plug Transition Perturbation Sensitivity and Kinetic Stabilization With Confinement .

TL;DR: In this article, the authors investigate the influence of geometrical confinement on the breakup of long fluid threads in the absence of imposed flow using a lattice Boltzmann model and find that the relative surface energies of the liquid components influence this effect.
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A laminar roughness boundary condition

TL;DR: In this paper, a modified slip boundary condition is obtained to represent the effects of small roughness-like perturbations to an otherwise-plane fixed wall which is acting as a boundary to steady laminar flow of a viscous fluid.
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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