Step 1: Concept:
This problem requires matching different statistical gas speeds derived from the Maxwell-Boltzmann distribution to their correct mathematical formulas.
Step 2: Key Formula or Approach:
For an ideal gas with molar mass $M$ at temperature $T$:
- Root mean square speed ($v_{rms}$) = $\sqrt{\frac{3RT}{M}}$
- Mean (average) speed ($v_{avg}$) = $\sqrt{\frac{8RT}{\pi M}}$
- Most probable speed ($v_{mp}$) = $\sqrt{\frac{2RT}{M}}$
- Mean relative speed ($v_{rel}$) of two colliding molecules = $\sqrt{2} \times v_{avg} = \sqrt{\frac{16RT}{\pi M}}$. Expressed using reduced mass ($\mu = m/2$) and the Boltzmann constant ($k$), this transforms to $\sqrt{\frac{8kT}{\pi\mu}}$.
Step 3: Step-by-step Explanation:
• A. Root mean square speed: By definition, $v_{rms} = (\frac{3RT}{M})^{1/2}$.
This matches III.
• B. Mean speed: The average speed of gas molecules is $v_{avg} = (\frac{8RT}{\pi M})^{1/2}$.
This matches II.
• C. Most probable speed: The speed at the peak of the Maxwell-Boltzmann curve is $v_{mp} = (\frac{2RT}{M})^{1/2}$.
This matches IV.
• D. Mean relative speed: The average relative speed between two colliding molecules is critical in collision theory. Using atomic mass $m$ and reduced mass $\mu = \frac{m_1 m_2}{m_1 + m_2} = \frac{m}{2}$ (for identical molecules), the formula is $(\frac{8kT}{\pi\mu})^{1/2}$.
This matches I.
The final matching sequence is A-III, B-II, C-IV, D-I.
Step 4: Final Answer:
The matching pairs correspond perfectly to option (A).