To solve this problem, we need to use the concept of the root mean square (r.m.s.) speed of an ideal gas, which is given by the formula:
v_{\text{rms}} = \sqrt{\frac{3kT}{m}}
Where \(k\) is the Boltzmann constant, \(T\) is the temperature in Kelvin, and \(m\) is the mass of a gas molecule.
The r.m.s. speed of a gas is directly proportional to the square root of its absolute temperature. Thus, you can relate the r.m.s. speeds at two different temperatures as follows:
\frac{v_{\text{rms}_2}}{v_{\text{rms}_1}} = \sqrt{\frac{T_2}{T_1}}
Given in the problem:
\(v_{\text{rms}_1} = v_0\) at \(T_1 = 200 \, \text{K}\)
\(T_2 = 800 \, \text{K}\)
Substituting these into the formula, we get:
\frac{v_{\text{rms}_2}}{v_0} = \sqrt{\frac{800}{200}}
\frac{v_{\text{rms}_2}}{v_0} = \sqrt{4}
\frac{v_{\text{rms}_2}}{v_0} = 2
This implies that \(v_{\text{rms}_2} = 2v_0\).
Therefore, the r.m.s. speed of the gas at 800 K is twice that at 200 K, so the correct answer is:
2v_0.