Derivation
Imagine a beam of particles being shot through a target, and consider an infinitesimally thin slab of the target (Figure 1). The atoms (or particles) that might stop a beam particle are shown in red. The magnitude of the mean free path depends on the characteristics of the system the particle is in:
Where is the mean free path, n is the number of target particles per unit volume, and is the effective cross sectional area for collision.
The area of the slab is and its volume is . The typical number of stopping atoms in the slab is the concentration n times the volume, i.e., . 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 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 the particle being stopped within the slab
This is an ordinary differential equation
whose solution is known as Beer-Lambert law and has the form, where x is the distance travelled by the beam through the target and I0 is the beam intensity before it entered the target; ℓ 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 a particle is absorbed between x and x + dx is given by
Thus the expectation value (or average, or simply mean) of x is
The fraction of particles that are not stopped (attenuated) by the slab is called transmission where x is equal to the thickness of the slab x = dx.
Read more about this topic: Mean Free Path