Abstract
We study the passive transport of a scalar field by a spatially smooth but white-in-time incompressible Gaussian random velocity field on \(\mathbb {R}^d\). If the velocity field u is homogeneous, isotropic, and statistically self-similar, we derive an exact formula which captures non-diffusive mixing. For zero diffusivity, the formula takes the shape of \(\mathbb {E}\ \Vert \theta _t \Vert _{\dot{H}^{-s}}^2 = \textrm{e}^{-\lambda _{d,s} t} \Vert \theta _0 \Vert _{\dot{H}^{-s}}^2\) with any \(s\in (0,d/2)\) and \(\frac{\lambda _{d,s}}{D_1}:= s(\frac{\lambda _{1}}{D_1}-2s)\) where \(\lambda _1/D_1 = d\) is the top Lyapunov exponent associated to the random Lagrangian flow generated by u and \( D_1\) is small-scale shear rate of the velocity. Moreover, the mixing is shown to hold uniformly in diffusivity.
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Notes
The physical dimensions of \(D_1\) are inverse time and it can be regarded as a proxy for the shear rate at small scales. See the discussion of Kraichnan, e.g. [23, Eq. (3.5)] This shows that \(D_1\) is essentially a square of the fine-scale turbulent shear-rate times a Lagrangian correlation time of the shear rate. We note that our notation differs slightly different from that used in recent literature which replaces \(D_1\rightarrow (d-1) D_1\).
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Acknowledgements
We thank G. Eyink, A. Frishman and S. Punshon-Smith and the anonymous referee for useful comments. The research of MCZ was partially supported by the Royal Society URF\(\backslash \)R1\(\backslash \)191492 and EPSRC Horizon Europe Guarantee EP/X020886/1. The research of TDD was partially supported by the NSF DMS-2106233 grant and NSF CAREER award #2235395. The research of RSG was partially supported by the Deutsche Forschungsgemeinschaft through the SPP 2410/1 Hyperbolic Balance Laws in Fluid Mechanics: Complexity, Scales, Randomness. RSG’s research took place within the scope of the NCCR SwissMAP which was funded by the Swiss National Science Foundation (grant number 205607).
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Coti Zelati, M., Drivas, T.D. & Gvalani, R.S. Mixing by Statistically Self-similar Gaussian Random Fields. J Stat Phys 191, 61 (2024). https://doi.org/10.1007/s10955-024-03277-w
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DOI: https://doi.org/10.1007/s10955-024-03277-w