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Commit 46379505 authored by Anton Akhmerov's avatar Anton Akhmerov
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Merge branch 'drude_better_calc' into 'master'

rework the drude derivation

See merge request !72
parents f7741401 de268634
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1 merge request!72rework the drude derivation
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......@@ -135,20 +135,22 @@ Our goal is then to compute the *average* velocity.
happens with each individual element.**
Let us compute how the average velocity changes with time.
The equation with the Lorentz force we just average right away:
Consider the effect that scattering has over a small time $dt$.
A fraction $dt/τ$ of the electrons scatters, and that their average velocity becomes zero.
The rest of the electrons $(1 - dt/τ)$ are accelerated by the Lorentz force, and after $dt$ their velocity becomes
$$
m\frac{d⟨\mathbf{v}⟩}{dt} = -e\left(\mathbf{E}+⟨\mathbf{v}⟩×\mathbf{B}\right).
m\mathbf{v}(t + dt) - m\mathbf{v}(t) = - e (\mathbf{E} + \mathbf{v} × \mathbf{B})⋅dt.
$$
Almost there, but we still need to do something with the change of the average velocity due to scattering.
Consider the effect that scattering has over a small time $dt$.
Most electrons continue with the same velocity, however a fraction $dt/τ$ will scatter, and that their average velocity becomes zero.
Therefore we get
Averaging the velocity of the two groups of particles, we get
$$
\mathbf{v}(t+dt)⟩ = ⟨\mathbf{v}(t)⟩(1 - dt/τ) + 0⋅(dt/τ) ⇒ \frac{d⟨\mathbf{v}⟩}{dt} = -\frac{⟨\mathbf{v}⟩}{τ}.
\begin{align}
m⟨\mathbf{v}(t+dt)⟩ &= [m⟨\mathbf{v}(t)⟩ - e (\mathbf{E} + \mathbf{v} × \mathbf{B})dt]\left(1 - \frac{dt}{\tau}\right) + 0⋅\frac{dt}{\tau}\\
&= m⟨\mathbf{v}(t)⟩ - dt [e (\mathbf{E} + \mathbf{v} × \mathbf{B}) - m⟨\mathbf{v}(t)⟩/τ] \\
&\quad\quad\quad\quad + e (\mathbf{E} + \mathbf{v} × \mathbf{B}) m⟨\mathbf{v}(t)⟩dt²/τ.
\end{align}
$$
That's it!
We now combine both contributions into a single equation and get
We now neglect the term proportional to $dt²$ (it vanishes when $dt → ∞$).
Finally, we recognize that $(⟨\mathbf{v}(t+dt)⟩ - (⟨\mathbf{v}(t)⟩)/dt = d⟨\mathbf{v}(t)⟩)/dt$, and arrive to
$$
m\frac{d⟨\mathbf{v}⟩}{dt} = -m\frac{⟨\mathbf{v}⟩}{τ} -e\left(\mathbf{E}+⟨\mathbf{v}⟩×\mathbf{B}\right).
$$
......
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