Hostname: page-component-586b7cd67f-rcrh6 Total loading time: 0 Render date: 2024-12-04T09:59:25.877Z Has data issue: false hasContentIssue false

Diffusion and the torsion parameter

Published online by Cambridge University Press:  17 February 2009

Alex McNabb
Affiliation:
Department of Mathematics, Massey University, Palmerston North, New Zealand.
Grant Keady
Affiliation:
Mathematics Department, University of Western Australia, Nedlands, 6009, Western Australia.
Rights & Permissions [Opens in a new window]

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

The parameters describing the trapping kinetics of a linear model for diffusion, in solids involving a captured immobile phase of the diffusing entity, can be determined by measuring mean residence times for matter in the systems and evaluating the exponents for the final exponential decay rates of the diffusing entity from various shaped solids. The mean residence time for matter in a given region can be expressed in terms of a “torsion parameter” S which in the case of Dirichlet boundary conditions and cylindrical geometries, coincides with the torsional rigidity of the cylinder. The final decay rate is given by the first eigenvalue μ of a Helmholtz problem. Expressions and inequalities are derived for these parameters S and μ for general linear boundary conditions and for geometries relevant to diffusion experiments.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 1994

References

[1]Higgins, H. T. J., “A comprehensive review of Saint Venant's torsion problem”, Am. J. Phys. 10 (1942) 248259.Google Scholar
[2]Keady, G. and McNabb, A., “Some explicit solutions of – Δw = 1 with zero boundary data”, Department of Mathematics Research Report No. 42, University of Western Australia, Dec 1988.Google Scholar
[3]Keady, G. and McNabb, A., “The torsion problem in a lens: a case-study in symbolic-numeric computation using SENAC”, Department of Mathematics Research Report No. 191, University of Waikato, Hamilton, New Zealand, 1989.Google Scholar
[4]Keady, G. and McNabb, A., “The elastic torsion problem: solutions in some convex domains”, N.Z. J. Maths (1993) in press.Google Scholar
[5]Keady, G. and McNabb, A., “Functions with constant Laplacian satisfying homogeneous Robin boundary conditions”, J. M. A. J. Appl. Math. (1993) in press.Google Scholar
[6]McNabb, A. and Wake, G. C., “Some explicit solutions of –Δw = 1 with Robin boundary data”, Occasional publication series No. 17, Massey University, Department of Mathematics and Statistics, Palmerston North, New Zealand, 1989.Google Scholar
[7]McNabb, A. and Wake, G. C., “Heat conduction and finite transition times between steady- states”, I. M. A. J. Appl. Math. 47 (1991) 193206.Google Scholar
[8]Milne-Thompson, L. M., Antiplane elastic systems (Springer-Verlag, Berlin, 1962).CrossRefGoogle Scholar