The mean free path for gas, with molecular diameter \(d\) and number density can be expressed as:
1. \(\dfrac{1}{\sqrt{2} n πd^{2}}\)
2. \(\dfrac{1}{\sqrt{2} n^{2} πd^{2}}\)
3. \(\dfrac{1}{\sqrt{2} n^{2} \pi^{2} d^{2}}\)
4. \(\dfrac{1}{\sqrt{2} n πd}\)
The mean free path of gas molecules depends on:
(\(d=\) molecular diameter)
| 1. | \(d\) | 2. | \(d^2\) |
| 3. | \(d^{-2}\) | 4. | \(d^{-1}\) |

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The mean free path of molecules of a gas, (radius \(r\)) is inversely proportional to:
1. \(r^3\)
2. \(r^2\)
3. \(r\)
4. \(\sqrt{r}\)

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| 1. | decreases | 2. | increases |
| 3. | remains the same | 4. | becomes double |