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In physics, the free electron model is a simple model for the behaviour of electrons in a crystal structure of a metallic solid. Developed principally by Drude and Sommerfeld, the free electron model neglects not only the Coulomb interaction (see Coulomb's law) between electrons, but also the interaction between the electrons and the atomic lattice through which they move. Once the effects of quantum mechanics are taken into account, many of the experimental predictions of the model are surprisingly accurate, given its simplicity.

The free electron model should be contrasted with the tight-binding model, which uses the opposite simplification of treating the electrons as tightly bound to the atomic cores. (Coulomb interactions between electrons are still neglected.) The predictions of these two complementary models are reassuringly similar.

Ideas and assumptions


The solid-state physics models valence electrons as completely detatched from their ions in an "electron gas". While this model is the simplest model, it reproduces the main electronic properties of metals. The two fundamental asumptions are:

Predictions of the model


This very simple model of metals more or less correctly predicts: h^2*k^2/((2pi)^2*2m

Problems


As not all the forces on the electrons are taken into account the electrons have a effective mass that is larger than the free electron model predicts.

See also


Free electron ''People ''Other

External articles and references


Condensed matter physics | Electron

 

This article is licensed under the GNU Free Documentation License. It uses material from the "Free electron model".

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