6533b828fe1ef96bd128861e

RESEARCH PRODUCT

Transition to ballistic regime for heat transport in helium II

Michele SciaccaMichele SciaccaDavid JouDavid JouAntonio Sellitto

subject

Quantum turbulenceGeneral Physics and Astronomychemistry.chemical_elementFOS: Physical sciencesQuantum turbulencelaw.inventionSuperfluidityPhysics::Fluid DynamicsSuperconductivity (cond-mat.supr-con)Ballistic phononsThermal conductivityThermal conductivity; Liquid helium; Quantum turbulence; Micropores; Quantized vortices; Ballistic phononslawMesoscale and Nanoscale Physics (cond-mat.mes-hall)Settore MAT/07 - Fisica MatematicaHeliumLiquid heliumPhysicsMicroporesCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsLiquid heliumTurbulenceCondensed Matter - SuperconductivityMicroporeQuantized vorticeschemistryHeat fluxThermal conductivityQuantized vorticeSuperfluid helium-4

description

The size-dependent and flux-dependent effective thermal conductivity of narrow capillaries filled with superfluid helium is analyzed from a thermodynamic continuum perspective. The classical Landau evaluation of the effective thermal conductivity of quiescent superfluid, or the Gorter-Mellinck regime of turbulent superfluids, are extended to describe the transition to ballistic regime in narrow channels wherein the radius $R$ is comparable to (or smaller than) the phonon mean-free path $\ell$ in superfluid helium. To do so we start from an extended equation for the heat flux incorporating non-local terms, and take into consideration a heat slip flow along the walls of the tube. This leads from an effective thermal conductivity proportional to $R^2$ (Landau regime) to another one proportional to $R\ell$ (ballistic regime). We consider two kinds of flows: along cylindrical pipes and along two infinite parallel plates.

https://dx.doi.org/10.48550/arxiv.1405.3596