Abstract
We study the enhanced dissipation for the two-jet Kolmogorov type flow which is a stationary solution to the Navier–Stokes equations on the two-dimensional unit sphere given by the zonal spherical harmonic function of degree two. Based on the pseudospectral bound method developed by Ibrahim, Maekawa, and Masmoudi [14] and a modified version of the Gearhart–Prüss type theorem shown by Wei [50], we derive an estimate for the resolvent of the linearized operator along the imaginary axis and show that a solution to the linearized equation rapidly decays at the rate \(O(e^{-c\sqrt{\nu }\,t})\) when the viscosity coefficient \(\nu \) is sufficiently small as in the case of the plane Kolmogorov flow.
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Acknowledgements
The work of the first author was supported by JSPS KAKENHI Grant Numbers 20K03698, 19H05597, 20H00118. Also, the work of the second author was supported by Grant-in-Aid for JSPS Fellows No. 19J00693. The authors would like to thank an anonymous referee for a careful reading and valuable comments on this work.
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Maekawa, Y., Miura, TH. Rate of the Enhanced Dissipation for the Two-jet Kolmogorov Type Flow on the Unit Sphere. J. Math. Fluid Mech. 24, 92 (2022). https://doi.org/10.1007/s00021-022-00718-y
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DOI: https://doi.org/10.1007/s00021-022-00718-y