Bioconvection in suspensions of oxytactic bacteria: linear theory

Author:

Hillesdon A. J.,Pedley T. J.

Abstract

When a suspension of the bacteriumBacillus subtilisis placed in a chamber with its upper surface open to the atmosphere, complex bioconvection patterns form. These arise because the cells (a) are denser than water, and (b) swim upwards on average so that the density of an initially uniform suspension becomes greater at the top than at the bottom. When the vertical density gradient becomes large enough an overturning instability occurs which evolves ultimately into the observed patterns. The cells swim upwards because they are oxytactic, i.e. they swim up gradients of oxygen, and they consume oxygen. These properties are incorporated in conservation equations for the cell and oxygen concentrations, which, for the pre-instability stage of the pattern formation process, have been solved in a previous paper (Hillesdon, Pedley & Kessler 1995). In this paper we carry out a linear instability analysis of the steady-state cell and oxygen concentration distributions. There are intrinsic differences between the shallow-and deep-chamber cell concentration distributions, with the consequence that the instability is non-oscillatory in shallow chambers, but must be oscillatory in deep chambers whenever the critical wavenumber is non-zero. We investigate how the critical Rayleigh number for the suspension varies with the three independent parameters of the problem and discuss the most appropriate definition of the Rayleigh number. Several qualitative aspects of the solution of the linear instability problem agree with experimental observation.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference19 articles.

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2. Kessler, J. O. , Hoelzer, M. A. , Pedley, T. J. & Hill, N. A. 1994 Functional patterns of swimming bacteri. In Mechanics and Physiology of Animal Swimming (ed. L. Maddock , Q. Bone & J. M. V. Rayner ).Cambridge University Press.

3. Pedley, T. J. , Hill, N. A. & Kessler, J. O. 1988 The growth of bioconvection patterns in a uniform suspension of gyrotactic micro-organisms.J. Fluid Mech. 195,223–237.

4. Hill, N. A. , Pedley, T. J. & Kessler, J. O. 1989 Growth of bioconvection patterns in a suspension of gyrotactic micro-organisms in a layer of finite depth.J. Fluid Mech. 208,509–543.

5. Keller, E. F. & Segel, L. A. 1971b Travelling bands of chemotactic bacteria.J. Theor. Biol. 30,235–249.

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