9,213 research outputs found
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
Kinetic Density Functional Theory: A microscopic approach to fluid mechanics
In the present paper we give a brief summary of some recent theoretical
advances in the treatment of inhomogeneous fluids and methods which have
applications in the study of dynamical properties of liquids in situations of
extreme confinement, such as nanopores, nanodevices, etc. The approach obtained
by combining kinetic and density functional methods is microscopic, fully
self-consistent and allows to determine both configurational and flow
properties of dense fluids.
The theory predicts the correct hydrodynamic behavior and provides a
practical and numerical tool to determine how the transport properties are
modified when the length scales of the confining channels are comparable with
the size of the molecules. The applications range from the dynamics of simple
fluids under confinement, to that of neutral binary mixtures and electrolytes
where the theory in the limit of slow gradients reproduces the known
phenomenological equations such as the Planck-Nernst-Poisson and the
Smoluchowski equations. The approach here illustrated allows for fast numerical
solution of the evolution equations for the one-particle phase-space
distributions by means of the weighted density lattice Boltzmann method and is
particularly useful when one considers flows in complex geometries.Comment: 14 page
Multicomponent Diffusion in Nanosystems
We present the detailed analysis of the diffusive transport of spatially
inhomogeneous fluid mixtures and the interplay between structural and dynamical
properties varying on the atomic scale. The present treatment is based on
different areas of liquid state theory, namely kinetic and density functional
theory and their implementation as an effective numerical method via the
Lattice Boltzmann approach. By combining the first two methods it is possible
to obtain a closed set of kinetic equations for the singlet phase space
distribution functions of each species. The interactions among particles are
considered within a self-consistent approximation and the resulting effective
molecular fields are analyzed. We focus on multispecies diffusion in systems
with short-range hard-core repulsion between particles of unequal sizes and
weak attractive long-range interactions. As a result, the attractive part of
the potential does not contribute explicitly to viscosity but to diffusivity
and the thermodynamic properties. Finally, we obtain a practical scheme to
solve the kinetic equations by employing a discretization procedure derived
from the Lattice Boltzmann approach. Within this framework, we present
numerical data concerning the mutual diffusion properties both in the case of a
quiescent bulk fluid and shear flow inducing Taylor dispersion.Comment: 19 pages + 5 figure
A New Phenomenon: Sub-Tg, Solid-State, Plasticity-Induced Bonding in Polymers
Polymer self-adhesion due to the interdiffusion of macromolecules has been an
active area of research for several decades [70, 43, 62, 42, 72, 73, 41]. Here,
we report a new phenomenon of sub-Tg, solid-state, plasticity-induced bonding;
where amorphous polymeric films were bonded together in a period of time on the
order of a second in the solid-state at ambient temperatures nearly 60 K below
their glass transition temperature (Tg) by subjecting them to active plastic
deformation. Despite the glassy regime, the bulk plastic deformation triggered
the requisite molecular mobility of the polymer chains, causing
interpenetration across the interfaces held in contact. Quantitative levels of
adhesion and the morphologies of the fractured interfaces validated the sub-Tg,
plasticity-induced, molecular mobilization causing bonding. No-bonding outcomes
(i) during the compression of films in a near hydrostatic setting (which
inhibited plastic flow) and (ii) between an 'elastic' and a 'plastic' film
further established the explicit role of plastic deformation in this newly
reported sub-Tg solid-state bonding
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