Free electron gas model or classical theory

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SUMMARY

The discussion centers on the Drude-Lorentz Free Electron Gas Model, specifically addressing the uniform electrostatic field experienced by conduction electrons and the concept of effective mass. It is established that conduction electrons are treated as free due to their delocalization, which renders the potential from ion cores effectively constant. This approximation holds true for low-energy electrons, but may fail under high temperatures or strong currents, where the influence of ion cores becomes significant.

PREREQUISITES
  • Understanding of the Drude-Lorentz model
  • Knowledge of effective mass in solid-state physics
  • Familiarity with electrostatic potential and fields
  • Basic principles of conduction in solids
NEXT STEPS
  • Study the implications of effective mass in semiconductor physics
  • Explore the breakdown of the free electron model at high temperatures
  • Learn about the role of ion cores in solid-state physics
  • Investigate the mathematical formulation of electrostatic potential in solids
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Physics students, solid-state physicists, and researchers interested in the behavior of conduction electrons in materials will benefit from this discussion.

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Homework Statement



In Drude - Lorentz' FREE ELECTRON GAS MODEL , it has been said " since the conduction electrons move in a uniform electrostatic field of ion cores, their potential energy remains constant and is normally taken as zero, i.e., the existence of ion cores is ignored." I don't understand this point i.e
1) how we say uniform electrostatic field
2) why movement in uniform electrostatic field makes potential energy as constant
Thanks in advance.

Homework Equations





The Attempt at a Solution

 
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In reality, the existence of the ion cores is not completely ignored. What we do is use an effective mass for the electron in all of the equations instead of the real mass of the electron to account for the fact that the electrons are really bound to a potential created by the ion cores. The beauty is that once we use the effective mass, we can effectively ignore the ions because we have already accounted for them and treat the electrons as free.

1) a conduction electron in a solid is so delocalized that the electrostatic potential of the ions looks essentially uniform and constant for low energy electrons. If you heat up the solid enough are drive a current strong enough, this approximation will break down.

2) Let's be careful with words here. In the effective mass approximation, the potential due to the ions looks constant to a conduction electron, so their field is zero. (The field is the negative gradient of the potential and the derivative of a constant is zero.)
 

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