11
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: found
      • Article: found
      Is Open Access

      Thermal conductivity of the chain with an asymmetric pair interaction

      Preprint
      ,

      Read this article at

      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          We provide molecular dynamics simulation of heat transport in one-dimensional molecular chains with different interparticle pair potentials. We show that the thermal conductivity is finite in the thermodynamic limit in the chains with the potential, which allows for bond dissociation. The Lennard-Jones, Morse and Coulomb potentials belong to such type of potentials. The convergence of the thermal conductivity is provided by phonon scattering on the locally stretched loose interatomic bonds at low temperature and by the many-particle scattering at high temperature. On the other hand, the chains with the confining pair potential, which does not allow for the bond dissociation, posses anomalous (diverging with the chain length) thermal conductivity. We emphasize that the chains with the symmetric or asymmetric Fermi-Pasta-Ulam potential or with the combined potentials containing parabolic confining potential all exhibit anomalous heat transport.

          Related collections

          Most cited references15

          • Record: found
          • Abstract: found
          • Article: not found

          Finite Thermal Conductivity in 1D Lattices

          We discuss the thermal conductivity of a chain of coupled rotators, showing that it is the first example of a 1D nonlinear lattice exhibiting normal transport properties in the absence of an on-site potential. Numerical estimates obtained by simulating a chain in contact with two thermal baths at different temperatures are found to be consistent with those based on linear response theory. The dynamics of the Fourier modes provides direct evidence of energy diffusion. The finiteness of the conductivity is traced back to the occurrence of phase jumps. Our conclusions are confirmed by the analysis of two variants of this model.
            Bookmark
            • Record: found
            • Abstract: found
            • Article: not found

            Normal Heat Conductivity of the One-Dimensional Lattice with Periodic Potential of Nearest-Neighbor Interaction

            The process of heat conduction in a chain with a periodic potential of nearest-neighbor interaction is investigated by means of molecular dynamics simulation. It is demonstrated that the periodic potential of nearest-neighbor interaction allows one to obtain normal heat conductivity in an isolated one-dimensional chain with conserved momentum. The system exhibits a transition from infinite to normal heat conductivity with the growth of its temperature. The physical reason for normal heat conductivity is the excitation of high-frequency stationary localized rotational modes. These modes absorb the momentum and facilitate locking of the heat flux.
              Bookmark
              • Record: found
              • Abstract: found
              • Article: found
              Is Open Access

              Heat Conduction and Entropy Production in a One-Dimensional Hard-Particle Gas

              , , (2002)
              We present large scale simulations for a one-dimensional chain of hard-point particles with alternating masses. We correct several claims in the recent literature based on much smaller simulations. Both for boundary conditions with two heat baths at different temperatures at both ends and from heat current autocorrelations in equilibrium we find heat conductivities kappa to diverge with the number N of particles. These depended very strongly on the mass ratios, and extrapolation to N -> infty resp. t -> infty is difficult due to very large finite-size and finite-time corrections. Nevertheless, our data seem compatible with a universal power law kappa ~ N^alpha with alpha approx 0.33. This suggests a relation to the Kardar-Parisi-Zhang model. We finally show that the hard-point gas with periodic boundary conditions is not chaotic in the usual sense and discuss why the system, when kept out of equilibrium, leads nevertheless to energy dissipation and entropy production.
                Bookmark

                Author and article information

                Journal
                17 July 2013
                Article
                1307.4725
                10b40d36-ae3c-4ed1-9a9c-b7a604bab53d

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                12 pages, 18 figures
                cond-mat.stat-mech

                Condensed matter
                Condensed matter

                Comments

                Comment on this article