Section 13.1 Flux of the Electric Field
The most natural direction associated with a surface is the direction perpendicular to it. Therefore, the natural integral to compute over a surface adds up the normal component of \(\EE\text{.}\) This is called the flux of \(\EE\) through the given surface (in the given direction):
\begin{gather*}
\hbox{flux} = \int \EE \cdot \nn \, dA = \int \EE \cdot d\AA .
\end{gather*}
Be warned that some authors use two integral signs rather than one, and other letters, such as \(S\) or \(\sigma\text{,}\) are often used in place of \(A\text{.}\)