inversely proportional to number of molecules per unit volume
inversely proportional to diameter of the molecule
directly proportional to the square root of the absolute temperature
directly proportional to the molecular mass
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Solution and Explanation
Mean free path, $\lambda = \frac{1}{\sqrt{2}\pi d^{2} n}$
where, n = Number of molecules per unit volume
d = Diameter of the molecule
As $PV = k_{B}NT$
$n = \frac{N}{V} = \frac{P}{k_{B}T} \quad\therefore \quad\lambda = \frac{1}{\sqrt{2}\pi d^{2} P}$
where,
$k_{B} =$ Boltzmann constant
$P =$ Pressure of gas
$T =$ Absolute temperature of the gas