On unified preserving properties of kinetic schemes

The kinetic theory provides a good basis for developing numerical methods for multiscale gas flows covering a wide range of flow regimes. A particular challenge for kinetic schemes is whether they can capture the correct hydrodynamic behaviors of the system in the continuum regime (i.e., as the Knudsen number $\epsilon\ll 1$ ) without enforcing kinetic scale resolution. At the current stage, the main approach to analyze such property is the asymptotic preserving (AP) concept, which aims to show whether the kinetic scheme reduces to a solver for the hydrodynamic equations as $\epsilon \to 0$. However, the detailed asymptotic properties of the kinetic scheme are indistinguishable as $\epsilon$ is small but finite under the AP framework. In order to distinguish different characteristics of kinetic schemes, in this paper we introduce the concept of unified preserving (UP) aiming at assessing asmyptotic orders (in terms of $\epsilon$) of a kinetic scheme by employing the modified equation approach and Chapman-Enskon analysis. It is shown that the UP properties of a kinetic scheme generally depend on the spatial/temporal accuracy and closely on the inter-connections among the three scales (kinetic scale, numerical scale, and hydrodynamic scale). Specifically, the numerical resolution and specific discretization determine the numerical flow behaviors of the scheme in different regimes, especially in the near continuum limit. As two examples, the UP analysis is applied to the discrete unified gas-kinetic scheme (DUGKS) and a second-order implicit-explicit Runge-Kutta (IMEX-RK) scheme to evaluate their asymptotic behaviors in the continuum limit.