Using \(v_{\text{rms}} = \sqrt{\frac{3RT}{m}}\)
At \(200 \, K\), the r.m.s. speed is \(v_0\):
\[
v_0 = \sqrt{\frac{3R \times 200}{m}} \quad \cdots (1)
\]
At \(800 \, K\), the r.m.s. speed is \(v'\):
\[
v' = \sqrt{\frac{3R \times 800}{m}} \quad \cdots (2)
\]
Dividing equation (2) by equation (1):
\[
\frac{v'}{v_0} = \sqrt{\frac{800}{200}} = \sqrt{4} = 2
\]
Therefore, \(v' = 2v_0\).