\(v_{rms} = \sqrt {\frac 23}v_p\)
\(v_{rms} = \sqrt {\frac 32}v_p\)
\(v_{rms} = v_p\)
\(v_{rms} = \sqrt {\frac 13}v_p\)
The problem at hand requires us to express the relationship between the root mean square speed \((v_{rms})\) and the most probable speed \((v_p)\) of gas molecules, specifically oxygen in this case. These speeds are characteristic of the Maxwell-Boltzmann distribution describing the velocity of gas molecules at a given temperature. Let's analyze this relationship step by step.
1. **Understanding Root Mean Square Speed (\(v_{rms}\))**:
The root mean square speed is a measure of the average speed of particles in a gas, given by the formula:
v_{rms} = \sqrt{\frac{3kT}{m}}
where \(k\) is the Boltzmann constant, \(T\) is the temperature in Kelvin, and \(m\) is the mass of a single molecule of the gas.
2. **Understanding Most Probable Speed (\(v_p\))**:
The most probable speed is the speed at which the largest number of molecules is moving, given by the formula:
v_p = \sqrt{\frac{2kT}{m}}
3. **Finding the Relationship**:
Given the equations for \(v_{rms}\) and \(v_p\), we can express the ratio between these two speeds:
\frac{v_{rms}}{v_p} = \frac{\sqrt{\frac{3kT}{m}}}{\sqrt{\frac{2kT}{m}}}
Simplifying under the square root:
v_{rms} = \sqrt{\frac{3}{2}} \cdot v_p
4. **Conclusion**:
The correct relationship between the root mean square speed and the most probable speed for a gas molecule at a given temperature (in this case, Oxygen at 300 K, although temperature is not a factor influencing the ratio directly) is:
v_{rms} = \sqrt{\frac{3}{2}} \cdot v_p
This matches the given correct option: v_{rms} = \sqrt{\frac{3}{2}}v_p.