this is for holding javascript data
Flaviu Cipcigan edited resistance.tex
over 10 years ago
Commit id: 154a2bc2fe929076cf0d635e1d69b10080551999
deletions | additions
diff --git a/resistance.tex b/resistance.tex
index 43453b6..9a4ae90 100644
--- a/resistance.tex
+++ b/resistance.tex
...
The two key elements for conducting a current are mobile charged particles and an energy dissipation mechanism.\footnote{We're discussing here about non-superconducing metals. Superconductivity is a totally different beast.} Since a current is just the motion of charged particles, you need the former by definition. In order to prevent these particles accelerating indefinitely, you also need an energy dissipation mechanism -- without it, you have no steady state current for nonzero electric field.
We'll now derive Ohm's law starting only from these
assumptions\cite{Drude_1900}. assumptions, following the argument set by \citet{Drude_1900}. Assume that we have a uniform density $n$ of particles, carrying a charge $q$. These carriers are accelerated by an electric field $\mathbf{E}$ and scatter via a certain mechanism with a characteristic lifetime $\tau$. Assuming they have a well defined momentum $\mathbf{p}$, their equation of motion is:\footnote{As long as we only consider small changes in momentum, \mathbf{p} can also be crystal momentum}
\begin{equation}
\frac{d\mathbf{p}}{dt} = - \frac{1}{\tau} \mathbf{p} + q \mathbf{E}
\label{eq:eom}