The root mean square (rms) velocity \( v_{{rms}} \) of gas molecules is given by the formula:
\[
v_{{rms}} = \sqrt{\frac{3kT}{m}}
\]
where:
- \( k \) is the Boltzmann constant,
- \( T \) is the absolute temperature in Kelvin,
- \( m \) is the mass of the gas molecule.
The ratio of the rms velocities at two different temperatures \( T_1 \) and \( T_2 \) can be written as:
\[
\frac{v_{{rms1}}}{v_{{rms2}}} = \sqrt{\frac{T_1}{T_2}}
\]
Given:
- \( T_1 = 327^\circ C = 327 + 273 = 600 \, {K} \),
- \( T_2 = 627^\circ C = 627 + 273 = 900 \, {K} \).
Substitute these values into the formula for the ratio of rms velocities:
\[
\frac{v_{{rms1}}}{v_{{rms2}}} = \sqrt{\frac{600}{900}} = \sqrt{\frac{2}{3}} = \frac{\sqrt{2}}{\sqrt{3}}
\]
Thus, the ratio of the rms velocities is:
\[
\boxed{\sqrt{2} : \sqrt{3}}
\]