I Drude model with and without an electric field

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In the Drude model, without an electric field, electrons do not transfer energy to ions because they reach equilibrium after collisions, balancing energy gained and lost. When an electric field is applied, electrons gain kinetic energy between collisions, allowing them to transfer energy to lattice ions. This energy transfer corresponds to the work done by the electric field on the electrons. The average velocity of electrons, known as drift velocity, results from these interactions, described by a linear friction term in their motion equations. Thus, the presence of an electric field is crucial for energy transfer in the Drude model.
aaronll
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Why in the Drude model without e-field no energy is transfer by electrons to ions, but when there is an e-field electrons transfer energy to ions ?
 
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aaronll said:
Why in the Drude model without e-field no energy is transfer by electrons to ions
What, precisely, gives you that impression ?
One of the assumptions says
The electron is considered to be immediately at equilibrium with the local temperature after a collision.
i.e. the electrons pick up just as much energy as they lose.

##\ ##
 
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BvU said:
What, precisely, gives you that impression ?
One of the assumptions says i.e. the electrons pick up just as much energy as they lose.

##\
that is clear, right, so with an electric field electron gain energy between collision and they transfer energy (kinetic energy) to lattice ion, and that energy is equal to the work done by the e-field on the electron?
So in "reality" electron gains velocity between collision but they lose that energy in collision and on average the velocity is the drift velocity?
 
It's an effective description of an electron in the medium. The interaction with the medium is described by a linear friction term and thus the equation of motion for the electron reads
$$m \dot{\vec{v}}=-\frac{m}{\tau} \vec{v}-e \vec{E}.$$
If ##\tau## is small enough the velocity "relaxes" quickly to the equilibrium limit, where the force vanishes, i.e.,
$$\vec{v}=-\frac{e \tau}{m} \vec{E}.$$
Now for DC you assume the electrons within the conductor are all independent and then the relation to the elctric current is
$$\vec{j}=-e n \vec{v}=\frac{e^2 n \tau}{m} \vec{E} \; \Rightarrow \; \sigma=\frac{e^2 n \tau}{m}.$$
 
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