Abstract
The most important characteristics of the Knudsen layer are the temperature jump ΔT between the liquid and vapor and the probability θK that a molecule, emitted by the liquid into the vapor, reaches infinity (as opposed to bouncing back due to collisions). In the present paper, the linearized Bhatnagar-Gross-Krook model is used to calculate ΔT and θK and show that, in the absence of macroscopic gradients of temperature and density, θK≈96.3%. It is then examined how ΔT and θK are affected by a combination of a temperature gradient (heat flux) and the matching density gradient, such that the resulting pressure field is uniform.
| Original language | English |
|---|---|
| Article number | 044116 |
| Journal | Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics |
| Volume | 111 |
| Issue number | 4 |
| DOIs | |
| Publication status | Published - Apr 2025 |
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