Lorentz-Lorenz relation: Difference between revisions

From Citizendium
Jump to navigation Jump to search
imported>Paul Wormer
No edit summary
imported>Paul Wormer
Line 31: Line 31:
</math>
</math>
==References==
==References==
* H. A. Lorentz, ''Über die Beziehung zwischen der Fortpflanzungsgeschwindigkeit des Lichtes und der Körperdichte'' [ [On the relation between the propagation speed of light and density of a body], Ann. Phys. vol. '''9''', pp. 641-665 (1880). [http://gallica.bnf.fr/ark:/12148/bpt6k15253h/CadresFenetre?O=NUMM-15253&M=chemindefer Online]
* H. A. Lorentz, ''Über die Beziehung zwischen der Fortpflanzungsgeschwindigkeit des Lichtes und der Körperdichte'' [On the relation between the propagation speed of light and density of a body], Ann. Phys. vol. '''9''', pp. 641-665 (1880). [http://gallica.bnf.fr/ark:/12148/bpt6k15253h/CadresFenetre?O=NUMM-15253&M=chemindefer Online]
* L. Lorenz, ''Über die Refractionsconstante'' [About the constant of refraction], Ann. Phys. vol. '''11''', pp. 70-103 (1880). [http://gallica.bnf.fr/ark:/12148/bpt6k152556/CadresFenetre?O=NUMM-15255&M=chemindefer Online]
* L. Lorenz, ''Über die Refractionsconstante'' [About the constant of refraction], Ann. Phys. vol. '''11''', pp. 70-103 (1880). [http://gallica.bnf.fr/ark:/12148/bpt6k152556/CadresFenetre?O=NUMM-15255&M=chemindefer Online]
<!--
<!--

Revision as of 09:32, 24 November 2008

This article is a stub and thus not approved.
Main Article
Discussion
Related Articles  [?]
Bibliography  [?]
External Links  [?]
Citable Version  [?]
 
This editable Main Article is under development and subject to a disclaimer.

In physics, the Lorentz-Lorenz relation is an equation between the index of refraction n and the density ρ of a dielectricum (a non-conducting material),

where K is a constant depending on the molar polarizability of the dielectricum.

The relation is named after the Dutch physicist Hendrik Antoon Lorentz and the Danish physicist Ludvig Valentin Lorenz.

For molecular solids consisting of a single kind of non-polar molecules, the proportionality factor K (m3/kg) is to a good approximation,

where M (g/mol) is the the molar mass and PM is the molar polarizability (in SI units):

where NA is Avogadro's constant and α is the polarizability (with dimension volume) of one molecule. In this expression for PM it is assumed that the molecular polarizabilities are additive; if this is not the case, the expression can still be used when α is replaced by an effective polarizability. The factor 1/3 arises from the assumption that a single molecule inside the solid feels a nearly spherical field from the surrounding molecules.

In Gaussian units (a non-rationalized centimer-gram-second system):

and the factor 103 is absent from K.

For polar molecules a temperature dependent contribution due to the alignment of dipoles must be added to K.

The Lorentz-Lorenz law follows from the Clausius-Mossotti relation if we use that the index of refraction n is to a very good approximation (for non-conducting materials and long wavelengths) equal to the square root of the static relative permittivity (formerly known as relative dielectric constant) εr,

References

  • H. A. Lorentz, Über die Beziehung zwischen der Fortpflanzungsgeschwindigkeit des Lichtes und der Körperdichte [On the relation between the propagation speed of light and density of a body], Ann. Phys. vol. 9, pp. 641-665 (1880). Online
  • L. Lorenz, Über die Refractionsconstante [About the constant of refraction], Ann. Phys. vol. 11, pp. 70-103 (1880). Online