Abstract
We study the statistics of the relative separation
$$R$(t)$ between two fluid particles in a random
flow. We confine ourselves to the Batchelor regime, i.e.~we only
examine the evolution of distances smaller than the smallest
active scale of the flow. Here, the latter is spatially smooth and
the linearized equation reads $\mbox\boldmath
$R$=\sigma(t)\cdot$R$$. The Lagrangian strain
(scalar or matrix) $\sigma$ is assumed as given in its statistics
and is modelled by a telegraph noise. This is a stationary random
Markov process, which can only take two values with known
transition probabilities. The presence of two independent
parameters (intensity of velocity gradient and flow correlation
time) allows the definition of their ratio as the Kubo number,
whose infinitesimal and infinite limits describe the
delta-correlated and quasi-deterministic cases, respectively.
However, the simplicity of the model enables us to write closed
equations for the interparticle distance in the presence of a
finite-correlated, i.e.~coloured, noise.
In 1D, the flow is locally compressible in every single
realization, but the average `volume' must keep finite. This
provides us with a mathematical constraint, which physically
reflects in the fact that, in the Lagrangian frame, particles
spend longer time in contracting regions than in expanding ones.
Imposing this condition consistently, we are able to find
analytically the long-time growth rate of the
interparticle-distance moments and, consequently, the senior
Lyapunov exponent, which coherently turns out to be negative.
Analysing the large-deviation form of the joint probability
distribution, we also show the exact expression of the Cramér
function, which happens to satisfy the well-known
Gallavotti--Cohen relation despite the time irreversibility of the
strain statistics.
The 2D incompressible isotropic case was also studied. The
evolution of the linear and quadratic components was analysed
thoroughly, while for higher moments, due to high computational
cost, we focused on a restricted, though exact, dynamics. As a
result, we obtained the moment asymptotic growth rates and the
Lyapunov exponent (positive) in the two above-mentioned limits,
together with the leading corrections. The quasi-deterministic
limit turns out to be singular, while a perfect agreement was
found with the already-known delta-correlated case.
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