If temperature measures the average kinetic energy, how fast are the molecules really moving? The quantity that answers this is the root mean square speed vrmsv_\text{rms}: the square root of the average of the squares of the molecular speeds. It is the “typical” speed of thermal agitation.

Principle — Agitation speed

vrms=3kBTmpart=3RTmmol\ev{v_{\text{rms}} = \sqrt{\frac{3\,k_B\,T}{m_{\text{part}}}} = \sqrt{\frac{3\,R\,T}{m_{\text{mol}}}}}

Here too the two forms are equivalent: one uses the mass of the single particle mpartm_\text{part} with kBk_B, the other the molar mass mmolm_\text{mol} with RR. Two immediate readings: at the same temperature, lighter molecules are faster (vrms1/mv_\text{rms}\propto 1/\sqrt{m}); and at the same mass, heating the gas increases the speed (vrmsTv_\text{rms}\propto\sqrt{T}).

Note the factor 33: it is always 33, regardless of whether the gas is mono- or diatomic. This is because only the three translational degrees of freedom contribute to the speed of translation through space, and these are always three. Any rotations (which take ff from 3 to 5 in the internal energy) do not move the centre of the molecule and so do not enter vrmsv_\text{rms}.

Common mistake

Do not confuse the factor f2\frac{f}{2} of the internal energy with the factor 33 of vrmsv_\text{rms}. The first counts all the degrees of freedom; the second counts only the three translational ones, always three.

Topics: Teoria cinetica dei gas Concepts: Velocità quadratica media · Temperatura Skills: Interpretazione micro-macro

Related exercises: Problema — Temperatura di fuga dell’idrogeno · Problema — Temperatura da v_rms · Problema — Velocità quadratica media dell’azoto