The most important characteristics of the Knudsen layer are the temperature jump ^T 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 ^T and θK and show that, in the absence of macroscopic gradients of temperature and density, θK ≈ 96.3%. It is then examined how ^T 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