Abstract

The kinetic flux vector splitting (KFVS) scheme, when used for quantum Euler equations, as was done by Yang et al [22], requires the integration of the quantum Maxwellian (Bose-Einstein or Fermi-Dirac distribution), giving a numerical flux much more complicated than the classical counterpart. As a result, a nonlinear 2 by 2 system that connects the macroscopic quantities temperature and fugacity with density and internal energy needs to be inverted by iterative methods at every spatial point and every time step. In this paper, we propose to use a simple classical KFVS scheme for the quantum hydrodynamics based on the key observation that the quantum and classical Euler equations share the same form if the (quantum) internal energy rather than temperature is used in the flux. This motivates us to use a classical Maxwellian - that depends on the internal energy rather than temperature - instead of the quantum one in the construction of the scheme, yielding a KFVS which is purely classical. This greatly simplifies the numerical algorithm and reduces the computational cost. The proposed schemes are tested on a 1-D shock tube problem for the Bose and Fermi gases in both classical and nearly degenerate regimes.

Highlights

  • The quantum Euler equations describe the hydrodynamics of a quantum gas

  • It can be derived via the Chapman-Enskog expansion [2] as the leading order approximation of the quantum Boltzmann equation

  • A Kinetic Flux Vector Splitting scheme was proposed for the quantum Euler equations

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Summary

Introduction

The quantum Euler equations describe the hydrodynamics of a quantum gas It can be derived via the Chapman-Enskog expansion [2] as the leading order approximation of the quantum Boltzmann equation. This work led to the development of kinetic flux vector splitting (KFVS) scheme by Deshpande [4]. A direct generalization of the KFVS scheme to the quantum Euler equations was done by Yang et al in [22, 23]. They adopted the KFVS of Deshpande with the classical Maxwellian replaced by the quantum ones (the Bose-Einstein or the Fermi-Dirac distribution).

Quantum Boltzmann Equation
Boltzmann’s H-Theorem and Quantum Maxwellians
The Quantum Euler Equations
Classical KFVS Schemes
Quantum KFVS Schemes
A New Quantum KFVS Scheme
High Resolution Schemes
Numerical Examples
Computing z and T
Bose Gas in Classical Regime
Bose Gas in Nearly Degenerate Regime
Fermi Gas in Classical Regime
Fermi Gas in Nearly Degenerate Regime
Another Example for Fermi Gas in Nearly Degenerate Regime
Conclusion
Full Text
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