the mean free path of collision of gas molecules varies with its diameter(d) of the molecules as?
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Explanation:
Mean free path of gas molecules
$ \, \, \, \, \, \, \, \, λ = \frac{λ_1 + λ_2 + ... + λ_n}{n}$
$ \, \, \, \, \, \, \, \, λ = \frac{1}{\sqrt{2} \pi nd^2}$
$ \, \, \, \, \, \, \, \, λ ∝ d^{-2}$
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what to prove write the full question I can't understand
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