257 research outputs found
Crucial role of sidewalls in velocity distributions in quasi-2D granular gases
Our experiments and three-dimensional molecular dynamics simulations of
particles confined to a vertical monolayer by closely spaced frictional walls
(sidewalls) yield velocity distributions with non-Gaussian tails and a peak
near zero velocity. Simulations with frictionless sidewalls are not peaked.
Thus interactions between particles and their container are an important
determinant of the shape of the distribution and should be considered when
evaluating experiments on a tightly constrained monolayer of particles.Comment: 4 pages, 4 figures, Added reference, model explanation charified,
other minor change
Structure and soft magnetic properties of sputter deposited MnZn-ferrite films
In this paper we report the soft magnetic properties of thin films of sputtered MnZn ferrite deposited on thermally oxidized Si substrates. A high deposition temperature, 600¿°C, together with the addition of water vapor to the sputtering gas was found to improve the initial ac permeability, µ. The highest value obtained was approximately 30. For MnZn-ferrite films with much larger grain sizes, as obtained by deposition on a polycrystalline Zn-ferrite substrate, a µ of 100 was obtained. The results are discussed in terms of the so-called nonmagnetic grain boundary model
Grand canonical ensemble in generalized thermostatistics
We study the grand-canonical ensemble with a fluctuating number of degrees of
freedom in the context of generalized thermostatistics. Several choices of
grand-canonical entropy functional are considered. The ideal gas is taken as an
example.Comment: 14 pages, no figure
Multiple-Point and Multiple-Time Correlations Functions in a Hard-Sphere Fluid
A recent mode coupling theory of higher-order correlation functions is tested
on a simple hard-sphere fluid system at intermediate densities. Multi-point and
multi-time correlation functions of the densities of conserved variables are
calculated in the hydrodynamic limit and compared to results obtained from
event-based molecular dynamics simulations. It is demonstrated that the mode
coupling theory results are in excellent agreement with the simulation results
provided that dissipative couplings are included in the vertices appearing in
the theory. In contrast, simplified mode coupling theories in which the
densities obey Gaussian statistics neglect important contributions to both the
multi-point and multi-time correlation functions on all time scales.Comment: Second one in a sequence of two (in the first, the formalism was
developed). 12 pages REVTeX. 5 figures (eps). Submitted to Phys.Rev.
Onsager-Machlup theory for nonequilibrium steady states and fluctuation theorems
A generalization of the Onsager-Machlup theory from equilibrium to
nonequilibrium steady states and its connection with recent fluctuation
theorems are discussed for a dragged particle restricted by a harmonic
potential in a heat reservoir. Using a functional integral approach, the
probability functional for a path is expressed in terms of a Lagrangian
function from which an entropy production rate and dissipation functions are
introduced, and nonequilibrium thermodynamic relations like the energy
conservation law and the second law of thermodynamics are derived. Using this
Lagrangian function we establish two nonequilibrium detailed balance relations,
which not only lead to a fluctuation theorem for work but also to one related
to energy loss by friction. In addition, we carried out the functional
integrals for heat explicitly, leading to the extended fluctuation theorem for
heat. We also present a simple argument for this extended fluctuation theorem
in the long time limit.Comment: 20 pages, 2 figure
Theorem on the Distribution of Short-Time Particle Displacements with Physical Applications
The distribution of the initial short-time displacements of particles is
considered for a class of classical systems under rather general conditions on
the dynamics and with Gaussian initial velocity distributions, while the
positions could have an arbitrary distribution. This class of systems contains
canonical equilibrium of a Hamiltonian system as a special case. We prove that
for this class of systems the nth order cumulants of the initial short-time
displacements behave as the 2n-th power of time for all n>2, rather than
exhibiting an nth power scaling. This has direct applications to the initial
short-time behavior of the Van Hove self-correlation function, to its
non-equilibrium generalizations the Green's functions for mass transport, and
to the non-Gaussian parameters used in supercooled liquids and glasses.Comment: A less ambiguous mathematical notation for cumulants was adopted and
several passages were reformulated and clarified. 40 pages, 1 figure.
Accepted by J. Stat. Phy
Traveling Waves, Front Selection, and Exact Nontrivial Exponents in a Random Fragmentation Problem
We study a random bisection problem where an initial interval of length x is
cut into two random fragments at the first stage, then each of these two
fragments is cut further, etc. We compute the probability P_n(x) that at the
n-th stage, each of the 2^n fragments is shorter than 1. We show that P_n(x)
approaches a traveling wave form, and the front position x_n increases as
x_n\sim n^{\beta}{\rho}^n for large n. We compute exactly the exponents
\rho=1.261076... and \beta=0.453025.... as roots of transcendental equations.
We also solve the m-section problem where each interval is broken into m
fragments. In particular, the generalized exponents grow as \rho_m\approx
m/(\ln m) and \beta_m\approx 3/(2\ln m) in the large m limit. Our approach
establishes an intriguing connection between extreme value statistics and
traveling wave propagation in the context of the fragmentation problem.Comment: 4 pages Revte
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