Step 1: Use the formula for the root mean square (RMS) speed of an ideal gas:
\( v_{\text{rms}} = \sqrt{\frac{3kT}{m}} \), where:
- \( v_{\text{rms}} \) is the RMS speed
- \( k \) is Boltzmann’s constant
- \( T \) is the absolute temperature
- \( m \) is the mass of a single gas molecule
Step 2: Since \( k \) and \( m \) are constants for a given gas, the RMS speed depends on the square root of the temperature:
\( v_{\text{rms}} \propto \sqrt{T} \)
Step 3: Let the initial RMS speed at \( T_1 = 200\,K \) be \( v_0 \).
Now, the temperature is increased to \( T_2 = 800\,K \).
Using the proportionality:
\( \frac{v_{\text{rms, new}}}{v_0} = \sqrt{\frac{T_2}{T_1}} = \sqrt{\frac{800}{200}} = \sqrt{4} = 2 \)
Step 4: Therefore, the new RMS speed is:
\( v_{\text{rms, new}} = 2v_0 \)
Final Answer: \( 2v_0 \)