Hydromechanics of low-Reynolds-number flow. Part 5. Motion of a slender torus

Author:

Johnson Robert E.,Wu Theodore Y.

Abstract

In order to elucidate the general Stokes flow characteristics present for slender bodies of finite centre-line curvature the singularity method for Stokes flow has been employed to construct solutions to the flow past a slender torus. The symmetry of the geometry and absence of ends has made a highly accurate analysis possible. The no-slip boundary condition on the body surface is satisfied up to an error term of O2 In ε), where ε is the slenderness parameter (ratio of cross-sectional radius to centre-line radius). This degree of accuracy makes it possible to determine the force per unit length experienced by the torus up to a term of O2). A comparison is made between the force coefficients of the slender torus to those of a straight slender body to illustrate the large differences that may occur as a result of the finite centre-line curvature.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference11 articles.

1. Johnson, R. E. 1977 Sleuder-body theory for Stokes flow and flagellar hydrodynamics. Ph.D. thesis, California Institute of Technology, Pasadena, CA.

2. Kaplun, S. 1967 Fluid Mechanics and Singular Perturbations. Academic.

3. Wu, T. Y. & Yates, G. 1976 Finite-amplitude unsteady slender-body flow theory. 11th Symp. on Naval Hydrodyn. , University College London.

4. Keller, J. B. & Rubinow, S. I. 1976 Slender-body theory for slow viscous flow.J. Fluid Mech. 75,705–714.

5. Cox, R. G. 1970 The motion of long slender bodies in a viscous fluid. Part 1. General theory.J. Fluid Mech. 44,791–810.

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