Free electron gas model or classical theory

In summary, the Drude-Lorentz model for a free electron gas ignores the existence of ion cores and uses an effective mass for the electrons instead. This is based on the assumption that the electrostatic potential of the ions is uniform and constant for low energy electrons, but may break down at higher temperatures or current strengths. The effective mass approximation allows for the electrons to be treated as free, even though the ions are still present.
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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.)
 

1. What is the free electron gas model or classical theory?

The free electron gas model, also known as the classical theory, is a simplified model used to describe the behavior of electrons in a solid material. It assumes that the electrons in the material are not affected by the presence of other electrons and are free to move throughout the material.

2. How does the free electron gas model explain conductivity in metals?

The free electron gas model explains conductivity in metals by proposing that the electrons in a metal are not bound to specific atoms, but rather, are free to move throughout the material. This allows them to easily flow in response to an applied electric field, resulting in high conductivity.

3. What are the limitations of the free electron gas model?

The free electron gas model has several limitations. It does not take into account the interactions between electrons and other particles, such as atoms or impurities, which can affect the behavior of electrons in a material. It also does not account for the effects of temperature and does not accurately describe the behavior of electrons in non-metallic materials.

4. How does the free electron gas model relate to the band theory of solids?

The free electron gas model is a simplified version of the band theory of solids, which takes into account the interactions between electrons and other particles. The band theory explains how the energy levels of electrons in a material form bands, and how the movement of electrons between these bands determines the material's properties, such as conductivity.

5. Can the free electron gas model be used to accurately describe the behavior of real materials?

No, the free electron gas model is a simplified model and cannot accurately describe the behavior of all materials. It is most applicable to metals, where the electrons are relatively free to move, but it does not take into account the complexities of other materials such as semiconductors and insulators.

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