The root mean square (rms) speed of gas molecules is related to temperature by the following equation:
\[
v_{\text{rms}} \propto \sqrt{T}
\]
where \(v_{\text{rms}}\) is the root mean square speed and \(T\) is the temperature in Kelvin.
Given:
- Initial speed \(v_{\text{rms1}} = 120 \, \text{m/s}\) at \(T_1 = 88^\circ \text{C} = 88 + 273 = 361 \, \text{K}\).
- Final temperature \(T_2 = 127^\circ \text{C} = 127 + 273 = 400 \, \text{K}\).
- The pressure change does not affect the rms speed directly in this case since we are comparing the same gas under ideal conditions.
Now, using the relation \( \frac{v_2}{v_1} = \sqrt{\frac{T_2}{T_1}} \), we can solve for \(v_2\):
\[
\frac{v_2}{120} = \sqrt{\frac{400}{361}}
\]
\[
v_2 = 120 \times \sqrt{\frac{400}{361}} = 120 \times \sqrt{1.107} \approx 120 \times 1.053 \approx 126.3 \, \text{m/s}
\]
Thus, the root mean square speed at 127°C and 2 atmospheric pressure is approximately 126.3 m/s.