Laminar-Turbulent Transition: The change of the flow state temperature with the Reynolds number
arXiv:1404.0193 · doi:10.1007/s10955-014-1112-x
Abstract
Using the previously developed model to describe laminar/turbulent states of a viscous fluid flow, which treats the flow as a collection of coherent structures of various size (Chekmarev, Chaos, 2013, 013144), 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 power-law divergence characteristic of second-order phase transitions.
15 pages, 5 figures
References in corpus (5)
- Statistical mechanics and dynamics of solvable models with long-range interactions
- Experimental evidence of a phase transition in a closed turbulent flow
- Hydrodynamic turbulence as a problem in nonequilibrium statistical mechanics
- Tendency to occupy a statistically dominant spatial state of the flow as a driving force for turbulent transition
- Tendency to occupy a statistically dominant spatial state of the flow as a driving force for turbulent transition