- A$0.2\,\mu m$
- ✓$0.2\,mm$
- C$0.2\,cm$
- D$0.2\,nm$
$Y=\frac{K T}{\sqrt{2} \pi \sigma^{2} p}$
-wherein
$\sigma=$ Diameter of the molecule
$p=$ pressure of the gas
$T=$ temperature
$K=$ Boltzmann's Constant
Let intermolecular distance be $D$ then in a volume $\frac{4 \pi}{3} D^{3}$ there is only one
$\frac{4 \pi}{3} D^{3} P=\frac{1}{N_{A}}=R_{T} \quad$ or $\quad D=\left(\frac{3 R T}{4 \pi N_{A} P}\right)^{1 / 3}$
$\begin{aligned} \text { Put } P=& 4 \times 10^{-10} P a, R=83, N_{A}=6 \times 10^{23} \\ T=& 300 \mathrm{K} \end{aligned}$
$D=0.2 \mathrm{mm}$
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$(iv)$ The observer may be moving towards the source with a velocity of $33\,ms^{-1}$