In general if the surface is curved and the vector field isn't uniform, we must consider a small infinitesimal amount of flux through an element of area \( dA \),
$$ d\Phi_E = \vec{E} \circ \hat{n}dA \nonumber $$
Now let's add up all these infinitesimal fluxes to find the total flux through our curved surface in the non-uniform field,
$$ \Phi_E = \int _S \vec{E} \circ \hat{n}dA $$
The subscript \( S \) reminds us that this is a surface integral across the surface \( S \) in question.
If we integrate across an entire closed surface such as a sphere, or a cube, we denote this with a closed integral \( \oint \) instead of \( \int \). A closed surface is anything which divides space into an inside and an outside.
|