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Physics · Ch 1 — Electric Charges and Fields

Electric Flux

1.13

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 AA placed in a uniform field E⃗\vec{E}, with n^\hat{n} the unit vector normal (perpendicular) to the surface, the electric flux through it is defined as

Φ=E⃗⋅A⃗=EAcos⁡θ\Phi = \vec{E}\cdot\vec{A} = EA\cos\theta

where A⃗=An^\vec{A}=A\hat{n} is the "area vector" (a vector of magnitude AA pointing along the surface's outward normal), and θ\theta is the angle between E⃗\vec{E} and n^\hat{n}. Flux is a scalar quantity (the dot product of two vectors is a number, not a vector), with SI unit N m2/C\text{N}\,\text{m}^2/\text{C}.

Three special cases illustrate the formula: if the field is parallel to the surface's normal (θ=0∘\theta=0^\circ), Φ=EA\Phi=EA, the maximum possible flux for that area and field strength; if the field runs exactly along the surface, i.e. perpendicular to the normal (θ=90∘\theta=90^\circ), Φ=0\Phi=0 -- no field lines actually cross the surface, they merely graze it; and for a general angle in between, only the component of E⃗\vec{E} along the normal, Ecos⁡θE\cos\theta, 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 dA⃗d\vec{A}, each small enough that E⃗\vec{E} can be treated as constant and the element as flat; the flux through each element is dΦ=E⃗⋅dA⃗d\Phi=\vec{E}\cdot d\vec{A}, and the total flux is the sum (integral) of all these contributions:

Φ=∫E⃗⋅dA⃗\Phi = \int\vec{E}\cdot d\vec{A}

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, Φ=∮E⃗⋅dA⃗\Phi=\oint\vec{E}\cdot d\vec{A}, 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. …