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The importance of mean free path in determining gas flow behaviour

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Figure

FIGURE 1.slipSchematic of the momentum Knudsen layer (KL) closeto a planar wall, showing the microscopic slip u1(x,0); the macroscopic u(x,0) is required when using the classical Navier-Stokes equationswith a slip boundary condition.
FIGURE 2.The molecule under consideration is assumed to have just experiencedan intermolecular collision at its current positionHangleA molecule confined between two planar walls a distance apart
FIGURE 4.ized distance from a surface; (a) single-wall case and (b) parallel-wallcase
FIGURE 5.Normalized half-channel velocity profiles for variousKnudsen numbers. Comparison of power-law (PL) model results withthe solution of the Boltzmann equation [27], R26 moment equations [28]and conventional NS equations with first- and second-order slip.
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