Physics · Ch 1 — Electric Charges and Fields
Electric Flux
Electric Flux
Before Gauss's theorem can be stated, one more quantity must be defined precisely: electric flux, the measure of how much of an electric field passes through a given surface.
Flux through a flat surface in a uniform field. For a flat surface of area placed in a uniform field , with the unit vector normal (perpendicular) to the surface, the electric flux through it is defined as
where is the "area vector" (a vector of magnitude pointing along the surface's outward normal), and is the angle between and . Flux is a scalar quantity (the dot product of two vectors is a number, not a vector), with SI unit .
Three special cases illustrate the formula: if the field is parallel to the surface's normal (), , the maximum possible flux for that area and field strength; if the field runs exactly along the surface, i.e. perpendicular to the normal (), -- no field lines actually cross the surface, they merely graze it; and for a general angle in between, only the component of along the normal, , contributes to the flux.
Flux through a curved or non-uniform surface. When the surface is not flat, or the field is not uniform, the surface is divided into a very large number of infinitesimally small area elements , each small enough that can be treated as constant and the element as flat; the flux through each element is , and the total flux is the sum (integral) of all these contributions:
For a closed surface (one that completely encloses a volume, such as a sphere or a cube, with no gaps), this is written with a circle through the integral sign, , and the outward normal is always used at every point of the surface by convention -- so that flux due to field lines leaving the enclosed volume counts as positive, and flux due to field lines entering the enclosed volume counts as negative. …