Thermal velocity

Thermal velocity

The thermal velocity or thermal speed is a typical velocity of the thermal motion of particles which make up a gas, liquid, etc. Thus, indirectly, thermal velocity is a measure of temperature. Technically speaking it is a measure of the width of the peak in the Maxwell-Boltzmann particle velocity distribution. Note that in the strictest sense "thermal velocity" is not a velocity, since "velocity" usually describes a vector rather than simply a scalar speed.

Since the thermal velocity is only a "typical" velocity, a number of different definitions can be and are used.

Taking k_B to be the Boltzmann constant, T is the temperature, and m is the mass of a particle, then we can write the different thermal velocities:

In one dimension

If v_{th} is defined as the root mean square of the velocity in any one dimension (i.e. any single direction), then

:v_{th}=sqrt{frac{k_BT}{m

If v_{th} is defined as the mean of the magnitude of the velocity in any one dimension (i.e. any single direction), then

:v_{th}=sqrt{frac{2 k_BT}{pi m

If v_{th} is defined as the 1/e half-width of the thermal distribution or

if v_{th} is defined such that a particle with this speed has an energy of k_B T, then

:v_{th}=sqrt{frac{2k_BT}{m.

In three dimensions

If v_{th} is defined as the root mean square of the total velocity (in three dimensions), then

:v_{th}=sqrt{frac{3k_BT}{m.

If v_{th} is defined as the mean of the magnitude of the velocity of the atoms or molecules is given by

:V_t=sqrt{frac{8k_B T}{mpi


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