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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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Proceedings ArticleDOI

Controllability and optimal strokes for N-link microswimmer

TL;DR: This paper uses the Resistive Force Theory to express the equation of motion in a fluid with a low Reynolds number and proves that the swimmer is controllable in the whole plane for N ≥ 3 and for almost every set of stick lengths.
Posted Content

Metachronal waves in a chain of rowers with hydrodynamic interactions

TL;DR: It is found that metachronal waves with wavelengths of 7-10 rower distances emerge, when the range of hydrodynamic interactions is restricted either artificially to nearest neighbors or by the presence of a bounding surface as in any relevant biological system.
Book ChapterDOI

Hydromechanics of Swimming

Journal ArticleDOI

Advances in colloidal manipulation and transport via hydrodynamic interactions.

TL;DR: This review article highlights many recent advances in the field of micromanipulation of colloidal particles using hydrodynamic interactions (HIs), namely solvent mediated long-range interactions and focuses on different strategies where externally operated microstructures generate local flow fields that induce the advection and motion of the surrounding components.
Journal ArticleDOI

The effect of gait on swimming in viscoelastic fluids

TL;DR: In this paper, the reciprocal theorem is used to calculate the swimming velocity due to small-amplitude deformations on the simplest two-dimensional sheet, to explore general conditions on the swimming gait under which the sheet may move faster, or slower, in a viscoelastic fluid compared to a Newtonian 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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