Mean free path equation λ = k T 2 π P d i 2 \lambda=\frac{kT}{\sqrt 2 \pi Pd^2_i} λ = 2 π P d i 2 k T
Where λ \lambda λ = Mean free path of gas species
KB=Boltzmann constant
P= pressure
d= gas species diameter
T= temperature
substituting the values in the equation,
diameter of gas species=1.8 × 2 = 3.6 A = 3.6 × 1 0 − 10 1.8\times2=3.6A=3.6\times10^{-10} 1.8 × 2 = 3.6 A = 3.6 × 1 0 − 10
6.0 × 1 0 − 8 = 1.38 × 1 0 − 23 × 300 2 π P × 3.6 × 1 0 − 10 6.0\times10^{-8}=\frac{1.38\times10^{-23}\times300}{\sqrt2 \pi P \times 3.6\times10^{-10}} 6.0 × 1 0 − 8 = 2 π P × 3.6 × 1 0 − 10 1.38 × 1 0 − 23 × 300
making P subject of the formula,
P = 1.38 × 1 0 − 23 × 300 3.6 × 1 0 − 10 × π × 2 × 6.0 × 1 0 − 8 P=\frac{1.38\times10^{-23}\times300}{3.6\times10^{-10}\times\pi\times\sqrt2\times6.0\times10^{-8}} P = 3.6 × 1 0 − 10 × π × 2 × 6.0 × 1 0 − 8 1.38 × 1 0 − 23 × 300
P = 4.14 × 1 0 − 21 9.5966 × 1 0 − 17 P=\frac{4.14\times10^{-21}}{9.5966\times10^{-17}} P = 9.5966 × 1 0 − 17 4.14 × 1 0 − 21
P = 4.314 × 1 0 − 5 P a P=4.314\times10^{-5}Pa P = 4.314 × 1 0 − 5 P a
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