Hostname: page-component-586b7cd67f-t7czq Total loading time: 0 Render date: 2024-12-01T00:19:42.676Z Has data issue: false hasContentIssue false

Plane poloidal-toroidal decomposition of doubly periodic vector fields. Part 1. Fields with divergence

Published online by Cambridge University Press:  17 February 2009

G. D. McBain
Affiliation:
School of Aerospace, Mechanical and Mechatronic Engineering, The University of Sydney, Australia; e-mail: [email protected].
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.

It is shown how to decompose a three-dimensional field periodic in two Cartesian coordinates into five parts, three of which are identically divergence-free and the other two orthogonal to all divergence-free fields. The three divergence-free parts coincide with the mean, poloidal and toroidal fields of Schmitt and Wahl; the present work, therefore, extends their decomposition from divergence-free fields to fields of arbitrary divergence. For the representation of known and unknown fields, each of the five subspaces is characterised by both a projection and a scalar representation. Use of Fourier components and wave coordinates reduces poloidal fields to the sum of two-dimensional poloidal fields, and toroidal fields to the sum of unidirectional toroidal fields.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 2005

References

[1]Backus, G., “Poloidal and toroidal fields in geomagnetic field modelling”, Rev. Geophysics 24 (1) (1986) 75109.Google Scholar
[2]Busse, F. H., “On Howard's upper bound for heat transport by turbulent convection”, J. Fluid Mech. 37 (1969) 457477.Google Scholar
[3]Chandrasekhar, S., Hydrodynamic and Hydromagnetic Stability (Dover, New York, 1981).Google Scholar
[4]Clever, R. M. and Busse, F. H., “Tertiary and quaternary solutions for plane Couette flow”, J. Fluid Mech. 344 (1997) 137153.CrossRefGoogle Scholar
[5]Drazin, P. G. and Reid, W. H., Hydrodynamic Stability, 2nd ed. (Cambridge University Press, Cambridge, 2004).Google Scholar
[6]Elsasser, W. M., “Induction effects in terrestrial magnetism. I. Theory”, Phys. Rev. 69 (1946) 106116.Google Scholar
[7]Hochstrasser, U. W., “Orthogonal polynomials”, in Handbook of Mathematical Functions (Eds. Abramowitz, M. and Stegun, I.), (Dover, New York, 1965) Ch. 22, 771802.Google Scholar
[8]Holt, C. A., Introduction to Electromagnetic Fields and Waves (Wiley, New York, 1963).Google Scholar
[9]Joseph, D. D., Stability of Fluid Motions I (Springer, Berlin, 1976).Google Scholar
[10]Lamb, H., Hydrodynamics, 6th ed. (Cambridge University Press, Cambridge, 1932).Google Scholar
[11]Mallinson, G. D. and de Vahl Davis, G., “The method of the false transient for the solution of coupled elliptic equations”, J. Comput. Phys. 12 (1973) 435461.CrossRefGoogle Scholar
[12]McBain, G. D., “Fully developed laminar buoyant flow in vertical cavities and ducts of bounded section”, J. Fluid Mech. 401 (1999) 365377.Google Scholar
[13]McBain, G. D., “Convection in a horizontally heated sphere”, J. Fluid Mech. 438 (2001) 110.Google Scholar
[14]McBain, G. D. and Armfield, S. W., “Natural convection in a vertical slot: Accurate solution of the linear stability equations”, ANZIAM J. 45(E) (2004) C92–C105.Google Scholar
[15]Mityushev, V. and Adler, P. M., “Longitudinal permeability of spatially periodic rectangular arrays of circular cylinders I. A single cylinder in the unit cell”, Z Angew. Math. Mech. 82 (5) (2002) 335345.Google Scholar
[16]Moffatt, H. K., Magnetic Field Generation in Electrically Conducting Fluids (Cambridge University Press, Cambridge, 1978).Google Scholar
[17]Nagata, M., “Bifurcations in Couette flow between almost corotating cylinders”, J. Fluid Mech. 169 (1986) 229250.Google Scholar
[18]Perry, A. E. and Chong, M. S., “A description of eddying motions and flow patterns using critical point concepts”, Ann. Rev. Fluid Mech. 19 (1987) 125155.CrossRefGoogle Scholar
[19]Rauh, A., Page, S. and Stille, A., “Energy inconsistency of Galerkin approximations for plane Couette flow”, Rep. Math. Phys. 54 (2004) 2340.Google Scholar
[20]Rayleigh, , Lord, , “On convection currents in a horizontal layer of fluid, when the higher temperature is on the underside”, Lond., Edin. & Dubl. Phil. Mag. & J. Sci. 32 (192) (1916) 529546.Google Scholar
[21]Reynolds, O., “On the theory of lubrication and its application to Mr. Beauchamp Tower's experiments, including an experimental determination of the viscosity of olive oil”, Phil. Trans. R. Soc. Lond 177 (1886) 157234.Google Scholar
[22]Ruth, D. W., “On the transition to transverse rolls in an infinite vertical fluid layer—a power series solution”, Intl J. Heat Mass Transfer 22 (1979) 11991208.Google Scholar
[23]Schmitt, B. J. and von Wahl, W., “Decomposition of solenoidal fields into poloidal fields, toroidal fields and the mean flow. Applications to the Boussinesq-equations”, Lecture Notes in Math. 1530 (1992) 291305.Google Scholar
[24]Segel, L. A., “The non-linear interaction of a finite number of disturbances to a layer of fluid heated from below”, J. Fluid Mech. 21 (1965) 359384.Google Scholar
[25]Sherman, M., “Toroidal and poloidal field representation for convective flow within a sphere”, Phys. Fluids 11 (1968) 18951900.Google Scholar
[26]Squire, H. B., “On the stability for three-dimensional disturbances of viscous fluid between parallel walls”, Proc. R. Soc. Lond., Ser. A 142 (841) (1933) 621628.Google Scholar
[27]von Neumann, J., Mathematical Foundations of Quantum Mechanics, Trans. Beyer, R. T. (Princeton University Press, Princeton, New Jersey, 1955).Google Scholar
[28]Waldmann, L., “Zur Theorie des Gastrennungsverfahrens von Clusius und Dickel”, Die Naturwissenschaften 27 (14) (1939) 230231.Google Scholar