Root-Mean-Square Speed \(u_\mathrm{rms}\)
In the kinetic–molecular theory, gas molecules move randomly and collide elastically.
The spread of their speeds in a sample at temperature \(T\) is described by the
Maxwell–Boltzmann distribution. Three characteristic speeds are commonly used:
\[
\boxed{
u_m=\sqrt{\dfrac{2RT}{M}},\quad
u_{\text{av}}=\sqrt{\dfrac{8RT}{\pi M}},\quad
u_{\mathrm{rms}}=\sqrt{\dfrac{3RT}{M}}
}
\]
Here \(R=8.314462618\ \mathrm{J\,mol^{-1}\,K^{-1}}\), \(M\) is the molar mass in
\(\mathrm{kg\,mol^{-1}}\), and speeds are in \(\mathrm{m\,s^{-1}}\).
At a fixed temperature, lighter gases (smaller \(M\)) have higher characteristic speeds.
Raising \(T\) increases all three speeds. The typical ordering is
\(u_m < u_{\text{av}} < u_{\mathrm{rms}}\).
Unit consistency
The formula for \(u_{\mathrm{rms}}\) produces speed units:
\[
\begin{aligned}
\left[u_{\mathrm{rms}}\right]
&= \sqrt{ \dfrac{ \mathrm{J\,mol^{-1}\,K^{-1}} \cdot \mathrm{K} }{ \mathrm{kg\,mol^{-1}} } } \\
&= \sqrt{ \dfrac{ \mathrm{kg\,m^{2}\,s^{-2}} }{ \mathrm{kg} } } \\
&= \mathrm{m\,s^{-1}}
\end{aligned}
\]
Interpretation
The rms speed equals the square root of the mean of \(u^2\) over all molecules, so it
slightly exceeds the average speed. Distributions become broader and shift to higher
values as \(T\) increases or \(M\) decreases.