Abstract
Motivated by the astrophysical process of primordial star formation, we study
the general problem of the pollution of pristine fluid elements in compressible
turbulence. The faction of unpolluted or slightly-polluted fluid mass
corresponds to the low tail of the concentration probability distribution
function (PDF) with density weighting, and we derive evolution equations for
this faction from a number of PDF closure models for turbulent mixing. To test
and constrain these predictions, we conduct numerical simulations for decaying
passive scalars in isothermal turbulent flows with Mach numbers of 0.9 and 6.2,
and compute the mass fraction, $P(Z_c, t)$, of fluid elements with
pollutant concentration below a small threshold, $Z_c$. In the Mach 0.9
flow, the evolution of $P(Z_c, t)$ goes as $P(Z_c, t)=
P(Z_c, t) łnP(Z_c, t)/\tau_con$ if the mass fraction of
the polluted flow is larger than $0.1.$ If the initial pollutant
fraction is smaller than $0.1,$ an early phase exists during which
$P(Z_c, t) = P(Z_c, t) P(Z_c, t)-1/\tau_int.$
These equations are obtained from the adopted closure models, and the
timescales $\tau_con$ and $\tau_int$, for a continuous convolution
model and a nonlinear integral model, respectively, are measured from our
simulation data. When normalized to the flow dynamical time, the decay of
$P(Z_c, t)$ in the Mach 6.2 flow is slower than at Mach 0.9 because the
timescale for scalar variance decay is slightly larger and the low tail of the
concentration PDF broadens with increasing Mach number. A modified fitting
formula is proposed for $P(Z_c, t)$ in highly supersonic turbulence,
which agrees well with the simulation results from the Mach 6.2 flow.
Description
[1110.0571] The Pollution of Pristine Material in Compressible Turbulence
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