# Clausius–Mossotti relation

(Redirected from Lorentz–Lorenz equation)

The Clausius–Mossotti relation expresses the dielectric constant (relative permittivity, εr) of a material in terms of the atomic polarizibility, α, of the material's constituent atoms and/or molecules, or a homogeneous mixture thereof. It is named after Ottaviano-Fabrizio Mossotti and Rudolf Clausius. It is equivalent to the Lorentz–Lorenz equation. It may be expressed as:[1][2]

${\displaystyle {\frac {\varepsilon _{\mathrm {r} }-1}{\varepsilon _{\mathrm {r} }+2}}={\frac {N\alpha }{3\varepsilon _{0}}}}$

where

• ${\displaystyle \varepsilon _{r}=\epsilon /\epsilon _{0}}$ is the dielectric constant of the material
• ${\displaystyle \varepsilon _{0}}$ is the permittivity of free space
• ${\displaystyle N}$ is the number density of the molecules (number per cubic meter), and
• ${\displaystyle \alpha }$ is the molecular polarizability in SI-units (C·m2/V).

In the case that the material consists of a mixture of two or more species, the right hand side of the above equation would consist of the sum of the molecular polarizability contribution from each species, indexed by i in the following form:[3]

${\displaystyle {\frac {\varepsilon _{\mathrm {r} }-1}{\varepsilon _{\mathrm {r} }+2}}=\sum _{i}{\frac {N_{i}\alpha _{i}}{3\varepsilon _{0}}}}$

In the CGS system of units the Clausius–Mossotti relation is typically rewritten to show the molecular polarizability volume ${\displaystyle \alpha '=\alpha /(4\pi \varepsilon _{0})}$ which has units of volume (m3).[2] Confusion may arise from the practice of using the shorter name "molecular polarizability" for both ${\displaystyle \alpha }$ and ${\displaystyle \alpha '}$ within literature intended for the respective unit system.

## Lorentz–Lorenz equation

The Lorentz–Lorenz equation is similar to the Clausius–Mossotti relation, except that it relates the refractive index (rather than the dielectric constant) of a substance to its polarizability. The Lorentz–Lorenz equation is named after the Danish mathematician and scientist Ludvig Lorenz, who published it in 1869, and the Dutch physicist Hendrik Lorentz, who discovered it independently in 1878.

The most general form of the Lorentz–Lorenz equation is (in CGS units)

${\displaystyle {\frac {n^{2}-1}{n^{2}+2}}={\frac {4\pi }{3}}N\alpha _{\mathrm {m} }}$

where ${\displaystyle n}$ is the refractive index, ${\displaystyle N}$ is the number of molecules per unit volume, and ${\displaystyle \alpha _{\mathrm {m} }}$ is the mean polarizability. This equation is approximately valid for homogeneous solids as well as liquids and gases.

When the square of the refractive index is ${\displaystyle n^{2}\approx 1}$, as it is for many gases, the equation reduces to:

${\displaystyle n^{2}-1\approx 4\pi N\alpha _{\mathrm {m} }}$

or simply

${\displaystyle n-1\approx 2\pi N\alpha _{\mathrm {m} }}$

This applies to gases at ordinary pressures. The refractive index ${\displaystyle n}$ of the gas can then be expressed in terms of the molar refractivity ${\displaystyle A}$ as:

${\displaystyle n\approx {\sqrt {1+{\frac {3Ap}{RT}}}}}$

where ${\displaystyle p}$ is the pressure of the gas, ${\displaystyle R}$ is the universal gas constant, and ${\displaystyle T}$ is the (absolute) temperature, which together determine the number density ${\displaystyle N}$.

## References

1. ^ Rysselberghe, P. V. (January 1932). "Remarks concerning the Clausius–Mossotti Law". J. Phys. Chem. 36 (4): 1152–1155. doi:10.1021/j150334a007.
2. ^ a b Atkins, Peter; de Paula, Julio (2010). "Chapter 17". Atkins' Physical Chemistry. Oxford University Press. pp. 622–629. ISBN 978-0-19-954337-3.
3. ^ Corson, Dale R; Lorrain, Paul (1962). Introduction to electromagnetic fields and waves. San Francisco: W.H. Freeman. p. 116. OCLC 398313.