27 research outputs found
Statistics of the inverse-cascade regime in two-dimensional magnetohydrodynamic turbulence
We present a detailed direct numerical simulation of statistically steady,
homogeneous, isotropic, two-dimensional magnetohydrodynamic (2D MHD)
turbulence. Our study concentrates on the inverse cascade of the magnetic
vector potential. We examine the dependence of the statistical properties of
such turbulence on dissipation and friction coefficients. We extend earlier
work sig- nificantly by calculating fluid and magnetic spectra, probability
distribution functions (PDFs) of the velocity, magnetic, vorticity, current,
stream-function, and magnetic-vector-potential fields and their increments. We
quantify the deviations of these PDFs from Gaussian ones by computing their
flatnesses and hyperflatnesses. We also present PDFs of the Okubo-Weiss
parameter, which distin- guishes between vortical and extensional flow regions,
and its magnetic analog. We show that the hyperflatnesses of PDFs of the
increments of the stream-function and the magnetic vector potential exhibit
significant scale dependence and we examine the implication of this for the
multiscaling of structure functions. We compare our results with those of
earlier studies
Transition from dissipative to conservative dynamics in equations of hydrodynamics
We show, by using direct numerical simulations and theory, how, by increasing
the order of dissipativity () in equations of hydrodynamics, there is a
transition from a dissipative to a conservative system. This remarkable result,
already conjectured for the asymptotic case [U. Frisch et
al., Phys. Rev. Lett. {\bf 101}, 144501 (2008)], is now shown to be true for
any large, but finite, value of greater than a crossover value
. We thus provide a self-consistent picture of how
dissipative systems, under certain conditions, start behaving like conservative
systems and hence elucidate the subtle connection between equilibrium
statistical mechanics and out-of-equilibrium turbulent flows.Comment: 12 pages, 4 figure
Two-dimensional magnetohydrodynamic turbulence with large and small energy-injection length scales
Two-dimensional magnetohydrodynamics (2D MHD), forced at (a) large length
scales or (b) small length scales, displays turbulent, but statistically
steady, states with widely different statistical properties. We present a
systematic, comparative study of these two cases (a) and (b) by using direct
numerical simulations (DNSs). We find that, in case (a), there is energy
equipartition between the magnetic and velocity fields, whereas, in case (b),
such equipartition does not exist. By computing various probability
distribution functions (PDFs), we show that case (a) displays extreme events
that are much less common in case (b)
Multiscaling in Hall-Magnetohydrodynamic Turbulence: Insights from a Shell Model
We show that a shell-model version of the three-dimensional
Hall-magnetohydrodynamic (3D Hall-MHD) equations provides a natural theoretical
model for investigating the multiscaling behaviors of velocity and magnetic
structure functions. We carry out extensive numerical studies of this shell
model, obtain the scaling exponents for its structure functions, in both the
low- and high- power-law ranges of 3D Hall-MHD, and find that the
extended-self-similarity (ESS) procedure is helpful in extracting the
multiscaling nature of structure functions in the high- regime, which
otherwise appears to display simple scaling. Our results shed light on
intriguing solar-wind measurements.Comment: 7 pages, 6 figure
Odd viscosity in chiral active fluids
Chiral active fluids are materials composed of self-spinning rotors that
continuously inject energy and angular momentum at the microscale.
Out-of-equilibrium fluids with active-rotor constituents have been
experimentally realized using nanoscale biomolecular motors, microscale active
colloids, or macroscale driven chiral grains. Here, we show how such chiral
active fluids break both parity and time-reversal symmetries in their steady
states, giving rise to a dissipationless linear-response coefficient called odd
viscosity in their constitutive relations. Odd viscosity couples pressure and
vorticity leading, for example, to density modulations within a vortex profile.
Moreover, chiral active fluids flow in the direction transverse to applied
compression as in shock propagation experiments. We envision that this
collective transverse response may be exploited to design self-assembled
hydraulic cranks that convert between linear and rotational motion in
microscopic machines powered by active-rotors fluids
Hydrodynamic correlation functions of chiral active fluids
The success of spectroscopy to characterize equilibrium fluids, for example the heat capacity ratio, suggests a parallel approach for active fluids. Here, we start from a hydrodynamic description of chiral active fluids composed of spinning constituents and derive their low-frequency, long-wavelength response functions using the Kadanoff-Martin formalism. We find that the presence of odd (equivalently, Hall) viscosity leads to mixed density-vorticity response even at linear order. Such response, prohibited in time-reversal invariant fluids, is a large-scale manifestation of the microscopic breaking of time-reversal symmetry. Our work suggests possible experimental probes that can measure anomalous transport coefficients in active fluids through dynamic light scattering
Active viscoelasticity of odd materials
The mechanical response of active media ranging from biological gels to
living tissues is governed by a subtle interplay between viscosity and
elasticity. In this Letter, we generalize the canonical Kelvin-Voigt and
Maxwell models to active viscoelastic media that break both parity and
time-reversal symmetries. The resulting continuum theories exhibit viscous and
elastic tensors that are both antisymmetric, or odd, under exchange of pairs of
indices. We analyze how these parity violating viscoelastic coefficients
determine the relaxation mechanisms and wave-propagation properties of odd
materials.Comment: 6 pages, 3 figure