Ultrasonic waves in classical gases
arXiv:1710.03630 · doi:10.1103/PhysRevE.96.062142
Abstract
The velocity and absorption coefficient for the plane sound waves in a classical gas are obtained by solving the Boltzmann kinetic equation, which describes the reaction of the single-particle distribution function to a periodic external field. Within the linear response theory, the nonperturbative dispersion equation valid for all sound frequencies is derived and solved numerically. The results are in agreement with the approximate analytical solutions found for both the frequent- and rare-collision regimes.
arXiv comment8 pages, 2 figures
References in corpus (9)
- Viscous relaxation and collective oscillations in a trapped Fermi gas near the unitarity limit
- Viscosity in the excluded volume hadron gas model
- Quasiparticle Theory of Transport Coefficients for Hadronic Matter at Finite Temperature and Baryon Density
- Shear Viscosities from the Chapman-Enskog and the Relaxation Time Approaches
- A Continuum Description of Rarefied Gas Dynamics (II)--- The Propagation of Ultrasound
- Higher-order Continuum Approximation for Rarefied Gases
- Slope-dependent nuclear-symmetry energy within the effective surface approximation
- Viscosity of a classical gas: The rare-collision versus the frequent-collision regime
- Shear viscosity of nuclear matter