Hostname: page-component-8448b6f56d-m8qmq Total loading time: 0 Render date: 2024-04-25T05:53:57.357Z Has data issue: false hasContentIssue false

Bioconvection in suspensions of oxytactic bacteria: linear theory

Published online by Cambridge University Press:  26 April 2006

A. J. Hillesdon
Affiliation:
Department of Applied Mathematical Studies, University of Leeds, Leeds LS2 9JT, UK
T. J. Pedley
Affiliation:
Department of Applied Mathematical Studies, University of Leeds, Leeds LS2 9JT, UK Present address: Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Silver Street, Cambridge CB3 9EW, UK.

Abstract

When a suspension of the bacterium Bacillus subtilis is 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.

Type
Research Article
Copyright
© 1996 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Cash, J. R. & Moore, D. R. 1980 A high order method for the numerical solution of two-point boundary value problems. BIT 20, 4452.Google Scholar
Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability. Oxford University Press.
Chapman, C. J. & Proctor, M. R. E. 1980 Nonlinear Rayleigh—Bénard convection between poorly conducting boundaries. J. Fluid Mech. 101, 759782.Google Scholar
Childress, S., Levandowsky, M. & Spiegel, E. A. 1975 Pattern formation in a suspension of swimming micro-organisms; equations and stability theory. J. Fluid Mech. 63, 591613.Google Scholar
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, 509543.Google Scholar
Hillesdon, A. J. 1994 Pattern formation in a suspension of swimming bacteria. PhD dissertation, University of Leeds.
Hillesdon, A. J., Pedley, T. J. & Kessler, J. O. 1995 The development of concentration gradients in a suspension of chemotactic bacteria. Bull. Math. Biol. 57, 299344 (referred to herein as HPK).Google Scholar
Keller, E. F. & Segel, L. A. 1971a Model for chemotaxis. J. Theor. Biol. 30, 225234.Google Scholar
Keller, E. F. & Segel, L. A. 1971b Travelling bands of chemotactic bacteria. J. Theor. Biol. 30, 235249.Google Scholar
Keller, H. B. 1974 Accurate difference methods for nonlinear two-point boundary value problems. SIAM J. Numer. Anal. 11, 305320.Google Scholar
Kessler, J. O. 1989 Path and pattern — the mutual dynamics of swimming cells and their environment. Comments Theor. Biol. 1, 85108.Google Scholar
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.
Kessler, J. O., Strittmatter, R. P., Swartz, D. L., Wieley, D. A. & Wojciechowski, M. F. 1995 Paths and patterns: the biology and physics of swimming bacterial populations. In SEB Symposium 49: Biological Fluid Dynamics (ed. C. P. Ellington & T. J. Pedley). Cambridge, Company of Biologists.
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, 223237.Google Scholar
Pedley, T. J. & Kessler, J. O. 1990 A new continuum model for suspensions of gyrotactic microorganisms. J. Fluid Mech. 212, 155182.Google Scholar
Pedley, T. J. & Kessler, J. O. 1992 Hydrodynamic phenomena in suspensions of swimming microorganisms. Ann. Rev. Fluid Mech. 24, 313358.Google Scholar
Stix, M. 1970 Two examples of penetrative convection. Tellus 22, 517520.Google Scholar
Veronis, G. 1963 Penetrative convection. Astrophys. J. 137, 641663.Google Scholar
Zahn, J.-P., Toomre, J. & Latour, J. 1982 Nonlinear model analysis of penetrative convection. Geophys. Astrophys. Fluid Dyn. 22, 159193.Google Scholar