Step 1: Concept
The mean free path (\(\lambda\)) of a gas molecule is defined as the average distance traveled by a molecule between two successive collisions. It depends on the size of the molecules and the density of the gas.
Step 2: Meaning
Inversely proportional means that if one quantity increases, the other decreases in such a way that their product remains constant.
Step 3: Analysis
The mean free path \(\lambda\) is given by:
\[\lambda = \frac{1}{\sqrt{2} \pi d^2 n}\]
where \(d\) is the molecular diameter and \(n\) is the number density of molecules. Notice that \(\lambda\) is inversely proportional to \(d^2\). This relationship can be understood as follows:
As the molecular diameter \(d\) increases, the area over which a molecule can collide with another decreases, leading to a longer mean free path.
Conversely, if \(d\) decreases (molecules become smaller), the area for collisions increases, reducing the mean free path.
Let's examine each option:
A) Square of the molecular diameter: \(\lambda \propto \frac{1}{d^2}\). This is correct because an increase in \(d^2\) leads to a decrease in \(\lambda\).
B) Molecular diameter: \(\lambda \propto \frac{1}{d}\). This would imply that doubling the molecular diameter halves the mean free path, which does not match the given relationship.
C) Temperature: The mean free path is independent of temperature. While higher temperatures increase the speed of molecules, they also increase the number density \(n\), balancing out to keep \(\lambda\) constant at a fixed pressure and volume.
D) Square root of temperature: This would imply that \(\lambda \propto \frac{1}{\sqrt{T}}\). However, since the mean free path is independent of temperature under ideal gas assumptions, this option is incorrect.
Step 4: Conclusion
The correct relationship between the mean free path and the molecular diameter is that they are inversely proportional to the square of the molecular diameter.
Final Answer: (A)