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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

Strategies for locating the female gamete: the importance of measuring sperm trajectories in three spatial dimensions.

TL;DR: It is concluded that full insight into flagellar beat dynamics, swimming paths and chemotaxis under physiological conditions will eventually require quantitative imaging of flageLLar form, ion flux changes, cell trajectories and modelling of free-swimming spermatozoa in 3D.
Journal ArticleDOI

Untethered Miniature Soft Robots: Modeling and Design of a Millimeter-Scale Swimming Magnetic Sheet.

TL;DR: For the first time, a model from underlying physical principles is developed to explain and predict the sheet deformation, which enables it to swim at air-water interfaces and generate propulsive forces under water with an additional stiff frame.
Journal ArticleDOI

Swimming with magnets: From biological organisms to synthetic devices

TL;DR: The field of the magnetic microswimmers is reviewed, which as indicated by the adjective, represents a dedicated branch of the general microswimming where magnetism plays a role either for the orientation or for the locomotion of the swimmers.
Journal ArticleDOI

Hydrodynamics of linked sphere model swimmers.

TL;DR: The importance of time reversal symmetry in determining the far field flow around a swimmer is emphasized and the interactions between swimmers are highly dependent on the relative phase of their swimming strokes.
Journal ArticleDOI

Modelling the fluid mechanics of cilia and flagella in reproduction and development

TL;DR: The model of the embryonic node reveals how particle transport associated with morphogenesis is modulated by the gradual emergence of cilium posterior tilt, and the model of swimming makes use of force distributions within a body-conforming finite-element framework, allowing the solution of nonlinear inertialess Carreau flow.
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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