Mean free path
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In physics and kinetic theory, the mean free path of a particle, such as a molecule, is the average distance the particle travels between collisions with other particles.
The formula for calculating the magnitude of the mean free path depends on the characteristics of the system the particle is in. For a particle with a high velocity relative to the velocities of an ensemble of identical particles with random locations, the following relationship applies:
Where is the mean free path, n is the number of particles per unit volume, and σ is the effective cross sectional area for collision. If, on the other hand, the velocities of the identical particles have a Maxwell distribution of velocities, the following relationship applies:
Following table lists some typical values for different pressures.
Vacuum range | Pressure in hPa | Molecules / cm3 | mean free path |
---|---|---|---|
Ambient pressure | 1013 | 2.7*1019.. | 68 nm |
Low vacuum | 300..1 | 1019..1016 | 0.1..100 μm |
Medium vacuum | 1..10-3 | 1016..1013 | 0.1..100 mm |
High vacuum | 10-3..10-7 | 1013..109 | 10 cm..1 km |
Ultra high vacuum | 10-7..10-12 | 109..104 | 1 km..105 km |
Extremely high vacuum | <10-12 | <104 | >105 km |
Contents |
[edit] Derivation
Imagine a beam of particles being shot through a target, and consider an infinitesimally thin slab of the target (Figure 1). The atoms that might stop a beam particle are shown in red. The area of the slab is L2 and its volume is L2dx. The typical number of stopping atoms in the slab is the concentration n times the volume, i.e., nL2dx. The probability that a beam particle will be stopped in that slab is the net area of the stopping atoms divided by the total area of the slab.
where σ is the area (or, more formally, the "scattering cross-section") of one atom.
The drop in beam intensity equals the incoming beam intensity multiplied by the probability of being stopped within the slab
- dI = − Inσdx
This is an ordinary differential equation
whose solution is , where x is the distance traveled by the beam through the target and I0 is the beam intensity before it entered the target.
is called the mean free path because it equals the mean distance traveled by a beam particle before being stopped. To see this, note that the probability that the a particle is absorbed between x and x+dx is given by
Thus the expectation value (or average, or simply mean) of x is
[edit] Examples
A classic application of mean free path is to estimate the size of atoms or molecules. Another important application is in estimating the resistivity of a material from the mean free path of its electrons.
For example, for sound waves in an enclosure, the mean free path is the average distance the wave travels between reflections off the enclosure's walls.
[edit] See also
[edit] External links
- Gas Dynamics Toolbox Calculate mean free path for mixtures of gases using VHS model