Abstract
A new type of instability during the laminar-turbulent transition of a viscous incompressible fluid flow in the gap between two concentric spheres, where only the inner sphere rotates (spherical Couette flow), was detected. In case of two relatively wide gap widths (β = 0.33 and β = 0.5) it was found that the well-known Taylor-instability does not exist. At the stability threshold, where the laminar basic flow loses its stability, the first instability manifests itself as a break of the spatial symmetry and non-axisymmetric secondary waves with spiral arms appear. They spread from the pole to the equator. With increasing the Reynolds number above the critical one, the number of secondary waves with spiral arms decreases. Flow visualization studies and simultaneously laser-Doppler-velocimeter measurements show that the transition of the secondary wave flow with spiral arms is periodic and quasi-periodic before small scale turbulent structures occur.
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Egbers, C., Rath, H.J. (1996). LDV—measurements on wide gap instabilities in spherical Couette flow. In: Adrian, R.J., Durão, D.F.G., Durst, F., Heitor, M.V., Maeda, M., Whitelaw, J.H. (eds) Developments in Laser Techniques and Applications to Fluid Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-79965-5_4
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DOI: https://doi.org/10.1007/978-3-642-79965-5_4
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