Daily Physicist


Home     Archive     Tags     About        RSS
January 28, 2026


Auguste Piccard image courtesy of Deutsches Bundesarchiv under the Creative Commons Attribution-ShareAlike 3.0 Germany License

Today is the birthday of

Today’s Problem

The probability distribution for molecular speeds in an ideal gas is given by the Maxwell-Boltzmann speed distribution function

\[f(v)=4\pi v^2\left(\frac{m}{2\pi kT}\right)^{3/2} e^{-mv^2/2kT}\]

Use this to calculate the average speed in an ideal gas.

Answer

The average speed will be given by the integral

\[\bar{v} = \int_{0}^{\infty}vf(v)dv = 4\pi\left(\frac{m}{2\pi kT}\right)^{3/2}\int_{0}^{\infty}v^{3}e^{-mv^2/2kT}dv\]

With the change of variables

\[x=v\sqrt{\frac{m}{2kT}}\]

the integral becomes

\[\bar{v} = 4\sqrt{\frac{2kT}{\pi m}}\int_{0}^{\infty}x^{3}e^{-x^2}dx\]

With the change in variables \(y=x^2\) the integral becomes

\[\frac{1}{2}\int_{0}^{\infty}ye^{-y}dy\]

Using integration by parts, this evaluates to \(1/2\). So the average speed is

\[\bar{v} = \sqrt{\frac{8kT}{\pi m}}\]


© 2026 Stefan Hollos and Richard Hollos