The present study numerically investigates nonlinear thermal stress in a rarefied gas flow between two coaxial elliptic cylinders with a hot outer wall. Monatomic argon is considered and isothermal boundary conditions are implemented on the walls. Three different numerical methods are used to solve this problem, i.e., first, direct simulation Monte Carlo (DSMC) method is used and validated against the numerical solution of the Boltzmann equation available in the literature. The results of the DSMC algorithm are compared with the results of the Discrete Unified Gas Kinetic Scheme (DUGKS), and the continuum set of equations of slow non-isothermal (SNIT) flow, which includes nonlinear thermal stress terms compared to the Navier-Stokes equations. For the first time, flow is examined in a wide range of Knudsen numbers in the slip regime from the Knudsen number (Kn) of Kn=0.005 to Kn=0.1. At minimal Knudsen number, there is just one vortex due to nonlinear thermal stress flow; however, as Kn increases, the velocity peak near the inner cylinder is replaced with another vortex, which is created due to the second-order thermal creep effects on the inner wall of the cylinder. We show that as Kn increases, the inner vortex increases in size while the outer vortex shrinks. The mechanisms of the formation of both vortices are described in detail. Other flow characteristics, including walls velocity slip, shear stress, vorticity, and heat flux, are discussed.

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