# Molar refractivity

Molar refractivity, $A$ , is a measure of the total polarizability of a mole of a substance and is dependent on the temperature, the index of refraction, and the pressure.

The molar refractivity is defined as

$A={\frac {4\pi }{3}}N_{A}\alpha ,$ where $N_{A}\approx 6.022\times 10^{23}$ is the Avogadro constant and $\alpha$ is the mean polarizability of a molecule.

Substituting the molar refractivity into the Lorentz-Lorenz formula gives, for gasses

$A={\frac {RT}{p}}{\frac {n^{2}-1}{n^{2}+2}}$ where $n$ is the refractive index, $p$ is the pressure of the gas, $R$ is the universal gas constant, and $T$ is the (absolute) temperature. For a gas, $n^{2}\approx 1$ , so the molar refractivity can be approximated by

$A={\frac {RT}{p}}{\frac {n^{2}-1}{3}}.$ In SI units, $R$ has units of J mol−1 K−1, $T$ has units K, $n$ has no units, and $p$ has units of Pa, so the units of $A$ are m3 mol−1.

In terms of density ρ, molecular weight M, it can be shown that:

$A={\frac {M}{\rho }}{\frac {n^{2}-1}{n^{2}+2}}\approx {\frac {M}{\rho }}{\frac {n^{2}-1}{3}}.$ This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.