Knudsen number
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The Knudsen number (Kn) is a dimensionless number defined as the ratio of the molecular mean free path length to a representative physical length scale. This length scale could be, for example, the radius of a body in a fluid. The number is named after Danish physicist Martin Knudsen (1871–1949).
Definition
The Knudsen number is defined as:
- [\mathit = \frac = \frac \pi\sigma^2 P L} ]
- [\lambda] = mean free path (m)*
- L = representative physical length scale (m)
- kB = Boltzmann's constant (1.38×10-23 J/K)
- T = temperature (K)
- [\sigma] = diameter (m)
- P = total pressure (Pa)
Application
The Knudsen number is useful for determining whether statistical mechanics or the continuum mechanics formulation of fluid dynamics should be used: If the Knudsen number is near or greater than one, the mean free path of a molecule is comparable to a length scale of the problem, and the continuum assumption of fluid mechanics is no longer a good approximation. In this case statistical methods must be used.
Problems with high Knudsen numbers include the calculation of the motion of a dust particle through the lower atmosphere, or the motion of a satellite through the exosphere. The solution of the flow around an aircraft has a low Knudsen number. Using the Knudsen number an adjustment for Stokes' Law can be used in the Cunningham correction factor, this is a drag force correction due to slip in small particles (i.e. dp <5 µm).
See also
- Cunningham correction factor
- Fluid dynamics
- Mach number
- Reynolds number
External links
- [Gas Dynamics Toolbox] – Using the VHS model for calculating Knudsen numbers of gas mixtures
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