Hostname: page-component-cd9895bd7-jkksz Total loading time: 0 Render date: 2024-12-18T22:18:22.492Z Has data issue: false hasContentIssue false

Spectral study of the laminar—turbulent transition in spherical Couette flow

Published online by Cambridge University Press:  21 April 2006

Koichi Nakabayashi
Affiliation:
Department of Mechanical Engineering, Nagoya Institute of Technology, Nagoya 466, Japan
Yoichi Tsuchida
Affiliation:
Department of Mechanical Engineering, Nagoya Institute of Technology, Nagoya 466, Japan

Abstract

The laminar—turbulent transition of the Taylor—Görtler (TG) vortex flow in the clearance between two concentric spheres with only the inner sphere rotating (spherical Couette flow) is investigated by velocity measurement and simultaneous spectral and flow-visualization measurements by measuring the intensity of light scattered by the aluminium flakes used in flow visualization in the case of a relatively small ratio of the clearance to inner-sphere radius (clearance ratio β = 0.14). An azimuthal velocity component has been measured by a constant-temperature hotwire anemometer at two different colatitudes (meridian angles) θ; θ = 80° and 90° (the equator). A critical Reynolds number, some transition Reynolds numbers, flow regimes and flow states are obtained by the simultaneous spectral and flow-visualization measurements. The flow state is expressed by the number of toroidal TG vortex cells N, that of spiral TG vortex pairs Sp, the wavenumber of the travelling azimuthal waves on the toroidal TG vortices m and the wavenumber of shear waves SH. The mean velocity distribution and the characteristic values of the fluctuating velocity, such as autocorrelation coefficient, power spectrum and turbulence intensity (r.m.s. value), are considered over a great range of Reynolds number Re. Three kinds of fundamental frequencies of the velocity fluctuation are discovered and their characteristics are clarified by means of the velocity measurement and the simultaneous spectral and flow-visualization measurements. The three kinds of fundamental frequencies expressed by fS, fW and fH correspond to the spiral TG vortices, the travelling azimuthal waves and the shear waves, respectively. These fundamental frequencies are independent of both θ and wall distances from the inner sphere, but depend strongly on Re. Although the rotation frequency of the travelling azimuthal waves (or wave speed) in the circular Couette flow decreases monotonically with increasing Reynolds number until it reaches a plateau, the values of the rotation frequencies of the spiral TG vortices, the travelling azimuthal waves and the shear waves in the spherical Couette flow, fS/SP, fW/m and fH/SH, are nearly constant as the Reynolds number is increased, and differ slightly from one another.

Type
Research Article
Copyright
© 1988 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

Barters, F. 1982 Taylor vortices between two concentrie rotating spheres. J. Fluid Mech. 119, 1.Google Scholar
Belyaev, Vu. N., Monakhov, A. A., Scherbakov, S. A. & Vavorskaya, I. M. 1979 Onset of Sturbulence in rotating fluids. J. Exp. Theor. Phys. Lett. 29, 329.Google Scholar
Belyaev, Yu. N., Monakhov, A. A., Scherbakov, S. A. & Vavorskaya, I. M. 1984 Some routes to turbulence in spherical Couette flow. In Laminar—Turbulent Transition (ed. V. V. Kozlov), p. 669. Springer.
Bouabdallah, A. & Cognet, G. 1980 Laminar-turbulent transition in Taylor—Couette flow. In Laminar—Turbulent Transition (ed. R. Eppler & H. Fasel). p. 368. Springer.
Bühler, K. & Zierep, J. 1983 Transition to turbulence in a spherical gap. Proc. 4th Intl Symp. on Turbulent Shear Flows. University of Karlsruhe.
Bühler, K. & Zierep, J. 1984 New secondary flow instabilities for high Re-number flow between two rotating spheres. In Laminar—Turbulent Transition (ed. V. V. Kozlov). p. 677. Springer.
Coles, D. 1965 Transition in circular Couette flow. J. Fluid Mech. 21, 385.Google Scholar
Dennis, S. C. R. & Quartapelle, L. 1984 Finite difference solution to the flow between two rotating spheres. Comp. Fluids 12, 77.Google Scholar
Fenstermacher, P. R., Swinney, H. L. & Gollub, J. P. 1979 Dynamical instabilities and the transition to chaotic Taylor vortex flow. J. Fluid Mech. 94, 103.Google Scholar
Gorman, M. & Swinney, H. L. 1982 Spatial and temporal characteristics of modulated waves in the circular Couette system. J. Fluid Mech. 117, 123.Google Scholar
King, G. P., Li, V., Lee, W. & Swinney, H. L. 1984 Wave speeds in wavy Taylor-vortex flow. J. Fluid Mech. 141, 365.Google Scholar
Krause, E. 1980 Taylor—Görtler vortices in spherical gaps. Comp. Fluid Dyn. 2, 81.Google Scholar
Munson, B. R. & Menguturk, M. 1975 Viscous incompressible flow between concentric rotating spheres. Part 3. Linear stability and experiments. J. Fluid Mech. 69, 705.Google Scholar
Nakabayashi, K. 1976 Study on the flow between rotating spheres. 1st report. Theoretical study. Trans. Japan Soc. Mech. Engrs (in Japanese) 42, 1839.Google Scholar
Nakabayashi, K. 1978 Frictional moment of flow between two concentric spheres, one of which rotates. Trans. ASME I: J. Fluids Engng 100, 281.Google Scholar
Nakabayashi, K. 1983 Transition of Taylor—Görtler vortex flow in spherical Couette flow. J. Fluid Mech. 132, 209.Google Scholar
Nakabayashi, K., Nishida, H. & Onishi, S. 1981 Numerical studies of the flow between two concentric rotating spheres in the great range of Reynolds numbers. Bull. Japan Soc. Mech. Engrs 24, 1787.Google Scholar
Newhouse, S., Ruelle, D. & Takens, F. 1978 Occurrence of strange Axion A attracters near quasi-periodic flows on Tm, m > 3. Commun. Math. Phys. 64, 35.Google Scholar
Sato, H. & Saito, H. 1975 Fine-structure of energy spectra of velocity fluctuations in the transition region of a two dimensional wake. J. Fluid Mech. 61, 539.Google Scholar
Sawatzki, O. & Zierep, J. 1970 Das Stromfeld im Spalt zwischen zwei konzentrischen Kugelflächen, von denen die innere rotiert. Acta Mechanica 9, 13.Google Scholar
Schrauf, G. 1986 The first instability in spherical Taylor—Couette flow. J. Fluid Mech. 166, 287.Google Scholar
Schrauf, G. & Krause, E. 1984 Symmetric and asymmetric Taylor vortices in a spherical gap. In Laminar—Turbulent Transition (ed. V. V. Kozlov), p. 659. Springer.
Townsend, A. A. 1984 Axisymmetric Couette flow at large Taylor numbers. J. Fluid Mech. 144, 329.Google Scholar
Tuckerman, L. S. 1983 Formation of Taylor vortices in spherical Couette flow. PhD thesis, Massachusetts Institute of Technology.
Waked, A. M. & Munson, B. R. 1978 Laminar—turbulent flow in spherical annulus. Trans. ASME I: J. Fluids Engng 100, 281.Google Scholar
Walden, R. W. & Donnelly, R. J. 1979 Re-emergent order of chaotic circular Couette flow. Phys. Rev. Lett. 42, 301.Google Scholar
Wimmer, M. 1976 Experiments on a viscous fluid flow between concentric rotating spheres. J. Fluid Mech. 78, 317.Google Scholar
Yahata, H. 1978 Temporal development of the Taylor vortices in a rotating fluid. Prog. Theor. Phys. Suppl. 64, 165.Google Scholar
Yahata, H. 1978 Temporal development of the Taylor vortices in a rotating fluid. II. Prog. Theor. Phys. Suppl. 61, 791.Google Scholar
Yahata, H. 1978 Temporal development of the Taylor vortices in a rotating fluid. III. Prog. Theor. Phys. Suppl. 64, 782.Google Scholar
Yavorskaya, I. M., Belyaev, Yu. N., Monakhov, A. A., Astaf'Eva, N. M., Scherbakow, S. A. & Vvedenskaya, N. D. 1980 Stability, nonuniqueness and transition to turbulence in the flow between two rotating spheres. Rep. no. 595. Space Research Institute of the Academy of Science, USSR.