3,437 research outputs found
A Simplest Swimmer at Low Reynolds Number: Three Linked Spheres
We propose a very simple one-dimensional swimmer consisting of three spheres
that are linked by rigid rods whose lengths can change between two values. With
a periodic motion in a non-reciprocal fashion, which breaks the time-reversal
symmetry as well as the translational symmetry, we show that the model device
can swim at low Reynolds number. This model system could be used in
constructing molecular-size machines
On the third order structure function for rotating 3D homogeneous turbulent flow
A form for the two-point third order structure function has been calculated
for three dimensional homogeneous incompressible slowly rotating turbulent
fluid. It has been argued that it may possibly hint at the initiation of the
phenomenon of two-dimensionalisation of the 3D incompressible turbulence owing
to rotation.Comment: This revised version corrects some serious flaws in the discussions
after the equation (2) and the equation (13) of the earlier version. Some
typos are also correcte
Lattice Boltzmann simulations of a viscoelastic shear-thinning fluid
We present a hybrid lattice Boltzmann algorithm for the simulation of flow
glass-forming fluids, characterized by slow structural relaxation, at the level
of the Navier-Stokes equation. The fluid is described in terms of a nonlinear
integral constitutive equation, relating the stress tensor locally to the
history of flow. As an application, we present results for an integral
nonlinear Maxwell model that combines the effects of (linear) viscoelasticity
and (nonlinear) shear thinning. We discuss the transient dynamics of
velocities, shear stresses, and normal stress differences in planar
pressure-driven channel flow, after switching on (startup) and off (cessation)
of the driving pressure. This transient dynamics depends nontrivially on the
channel width due to an interplay between hydrodynamic momentum diffusion and
slow structural relaxation
Conformal Field Theory as Microscopic Dynamics of Incompressible Euler and Navier-Stokes Equations
We consider the hydrodynamics of relativistic conformal field theories at
finite temperature. We show that the limit of slow motions of the ideal
hydrodynamics leads to the non-relativistic incompressible Euler equation. For
viscous hydrodynamics we show that the limit of slow motions leads to the
non-relativistic incompressible Navier-Stokes equation. We explain the physical
reasons for the reduction and discuss the implications. We propose that
conformal field theories provide a fundamental microscopic viewpoint of the
equations and the dynamics governed by them.Comment: 4 page
Exact results for the thermal and magnetic properties of strong coupling ladder compounds
We investigate the thermal and magnetic properties of the integrable su(4)
ladder model by means of the quantum transfer matrix method. The magnetic
susceptibility, specific heat, magnetic entropy and high field magnetization
are evaluated from the free energy derived via the recently proposed method of
high temperature expansion for exactly solved models. We show that the
integrable model can be used to describe the physics of the strong coupling
ladder compounds. Excellent agreement is seen between the theoretical results
and the experimental data for the known ladder compounds
(5IAP)CuBr2HO, Cu(CHN)Cl etc.Comment: 10 pages, 5 figure
On the von Karman-Howarth equations for Hall MHD flows
The von Karman-Howarth equations are derived for three-dimensional (3D) Hall
magnetohydrodynamics (MHD) in the case of an homogeneous and isotropic
turbulence. From these equations, we derive exact scaling laws for the
third-order correlation tensors. We show how these relations are compatible
with previous heuristic and numerical results. These multi-scale laws provide a
relevant tool to investigate the non-linear nature of the high frequency
magnetic field fluctuations in the solar wind or, more generally, in any plasma
where the Hall effect is important.Comment: 11 page
Universality Class of the Reversible-Irreversible Transition in Sheared Suspensions
Collections of non-Brownian particles suspended in a viscous fluid and
subjected to oscillatory shear at very low Reynolds number have recently been
shown to exhibit a remarkable dynamical phase transition separating reversible
from irreversible behaviour as the strain amplitude or volume fraction are
increased. We present a simple model for this phenomenon, based on which we
argue that this transition lies in the universality class of the conserved DP
models or, equivalently, the Manna model. This leads to predictions for the
scaling behaviour of a large number of experimental observables. Non-Brownian
suspensions under oscillatory shear may thus constitute the first experimental
realization of an inactive-active phase transition which is not in the
universality class of conventional directed percolation.Comment: 4 pages, 2 figures, final versio
Drag Reduction by Bubble Oscillations
Drag reduction in stationary turbulent flows by bubbles is sensitive to the
dynamics of bubble oscillations. Without this dynamical effect the bubbles only
renormalize the fluid density and viscosity, an effect that by itself can only
lead to a small percentage of drag reduction. We show in this paper that the
dynamics of bubbles and their effect on the compressibility of the mixture can
lead to a much higher drag reduction.Comment: 7 pages, 1 figure, submitted to Phys. Rev.
Evolution to a singular measure and two sums of Lyapunov exponents
We consider dissipative dynamical systems represented by a smooth
compressible flow in a finite domain. The density evolves according to the
continuity (Liouville) equation. For a general, non-degenerate flow the result
of the infinite time evolution of an initially smooth density is a singular
measure. We give a condition for the non-degeneracy which allows to decide for
a given flow whether the infinite time limit is singular. The condition uses a
Green-Kubo type formula for the space-averaged sum of forward and
backward-in-time Lyapunov exponents. We discuss how the sums determine the
fluctuations of the entropy production rate in the SRB state and give examples
of computation of the sums for certain velocity fields.Comment: 4 pages, published versio
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