Abstract
Representing the fluid flow as a collection of coherent structures of various size, the statistical temperature of the flow state is determined as a function of the Reynolds number. It is shown that at small Reynolds numbers, associated with laminar states, the temperature is positive, while at large Reynolds numbers, associated with turbulent states, it is negative. At intermediate Reynolds numbers, the temperature changes from positive to negative as the size of the coherent structures increases, similar to what was predicted by Onsager for a system of parallel point-vortices in an inviscid fluid. It is also shown that in the range of intermediate Reynolds numbers the temperature exhibits a critical divergence.
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Acknowledgments
I thank R. Khairulin for useful discussions of the critical phenomena.
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Chekmarev, S.F. Laminar-Turbulent Transition: The Change of the Flow State Temperature with the Reynolds Number. J Stat Phys 157, 1019–1030 (2014). https://doi.org/10.1007/s10955-014-1112-x
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DOI: https://doi.org/10.1007/s10955-014-1112-x