It is the average distance traveled by molecule between the successive collisions, which modify it's direction or energy or other particle property.
Let the duration between the collision is t and the distance covered by the molecule is "\\bar{v}t" and the diameter of the cylinder is 2d.
so, volume of the cylinder "=\\pi d^2 vt"
Average number of collisions z="n_v\\pi d^2 vt"
where "n_v" is the number of collisions.
So, mean free path(l) ="\\dfrac{vt}{n_v\\pi d^2 vt}=\\dfrac{1}{n_v\\pi d^2}"
we know that "n_v=\\dfrac{p}{K_bT}"
So, "l=" "\\dfrac{1}{n_v\\pi d^2}=\\dfrac{K_bT}{p\\pi d^2}"
we know that, "v\\rightarrow\\sqrt{2}v"
So, "z=n_v\\pi d^2 vt=n_v\\pi d^2 \\sqrt{2}vt"
Hence, mean free path (l)"=\\dfrac{vt}{n_v\\pi d^2 \\sqrt{2}vt}=\\dfrac{1}{\\sqrt{2}n_v\\pi d^2}"
"l=" "\\dfrac{K_b T}{\\sqrt{2}p\\pi d^2}"
As the number of molecules are getting increase, the molecules will become closer to each other, therefore they more likely to run each other so mean free path decreases.
Comments
Leave a comment