The Loschmidt constant or Loschmidt's number (symbol: n0) is the number of particles (atoms or molecules) of an ideal gas per volume (the number density), and usually quoted at standard temperature and pressure. The 2018 CODATA recommended value[1] is at 0 °C and 1 atm. It is named after the Austrian physicist Johann Josef Loschmidt, who was the first to estimate the physical size of molecules in 1865.[2] The term Loschmidt constant is also sometimes used to refer to the Avogadro constant, particularly in German texts.
By ideal gas law,
p0V=NkBT0
N=n0V
n0=
p0 | |
kBT0 |
,
Since the Avogadro constant NA satisfies
R=NAk
n0=
p0NA | |
RT0 |
,
Being a measure of number density, the Loschmidt constant is used to define the amagat, a practical unit of number density for gases and other substances:
1 rm{amagat}=n0=2.686 780 111... x 1025 rm{m}-3
In the CODATA set of recommended values for physical constants, the Loschmidt constant is calculated from the Avogardo constant and the molar volume of an ideal gas, or equivalently the Boltzmann constant:[3]
n0:=
NA | = | |
Vm |
p0 | |
kBT0 |
,
Loschmidt did not actually calculate a value for the constant which now bears his name, but it is a simple and logical manipulation of his published results. James Clerk Maxwell described the paper in these terms in a public lecture eight years later:[4]
Loschmidt has deduced from the dynamical theory the following remarkable proportion:—As the volume of a gas is to the combined volume of all the molecules contained in it, so is the mean path of a molecule to one-eighth of the diameter of a molecule.To derive this "remarkable proportion", Loschmidt started from Maxwell's own definition of the mean free path (there is an inconsistency between the result on this page and the page cross-referenced to the mean free path; here appears an additional factor 3/4):
\ell=
3 | |
4n0\pid2 |
,
1 | |
n0 |
=
16 | |
3 |
\pi\elld2 | |
4 |
,
d=8
Vl | |
Vg |
\ell
The number density, the constant which now bears Loschmidt's name, can be found by simply substituting the diameter of the molecule into the definition of the mean free path and rearranging:
n0=\left(
Vg | |
Vl |
\right)2
3 | |
256\pi\ell3 |
.
Loschmidt's estimated data for air give a value of n = . Eight years later, Maxwell was citing a figure of "about 19 million million million" per cm, or .