Electric flux

In electromagnetism, electric flux is the measure of the electric field through a given surface,^[1] although an electric field in itself cannot flow. It is a way of describing the electric field strength at any distance from the charge causing the field.

The electric field E can exert a force on an electric charge at any point in space. The electric field is the gradient of the potential.

Overview[]

An electric charge, such as a single electron in space, has an electric field surrounding it. In pictorial form, this electric field is shown as a dot, the charge, radiating "lines of flux". These are called Gauss lines.^[2] Note that field lines are a graphic illustration of field strength and direction and have no physical meaning. The density of these lines corresponds to the electric field strength, which could also be called the electric flux density: the number of "lines" per unit area. Electric flux is proportional to the total number of electric field lines going through a surface. For simplicity in calculations, it is often convenient to consider a surface perpendicular to the flux lines. If the electric field is uniform, the electric flux passing through a surface of vector area $S$ is

\Phi _{E}=\mathbf {E} \cdot \mathbf {S} =ES\cos \theta ,

where

E

is the electric field (having units of

V/m

),

E

is its magnitude,

S

is the area of the surface, and

θ

is the angle between the electric field lines and the normal (perpendicular) to

S

.

For a non-uniform electric field, the electric flux $dΦ E$ through a small surface area $d S$ is given by

{\textrm {d}}\Phi _{E}=\mathbf {E} \cdot {\textrm {d}}\mathbf {S}

(the electric field,

E

, multiplied by the component of area perpendicular to the field). The electric flux over a surface

S

is therefore given by the surface integral:

\Phi _{E}=\iint _{S}\mathbf {E} \cdot {\textrm {d}}\mathbf {S}

where

E

is the electric field and

d S

is a differential area on the closed surface

S

with an outward facing surface normal defining its direction.

For a closed Gaussian surface, electric flux is given by:

\Phi _{E}=\,\!

$\oiint$

\scriptstyle S

\mathbf {E} \cdot {\textrm {d}}\mathbf {S} ={\frac {Q}{\varepsilon _{0}}}\,\!

where

$E$ is the electric field,
$S$ is any closed surface,
$Q$ is the total electric charge inside the surface $S$ ,
$ε 0$ is the electric constant (a universal constant, also called the "permittivity of free space") ( $ε 0 \approx 8.854 187817 \times 10 -12 F / m$ )

This relation is known as Gauss' law for electric field in its integral form and it is one of Maxwell's equations.

While the electric flux is not affected by charges that are not within the closed surface, the net electric field, $E$ , in the Gauss' Law equation, can be affected by charges that lie outside the closed surface. While Gauss' Law holds for all situations, it is most useful for "by hand" calculations when high degrees of symmetry exist in the electric field. Examples include spherical and cylindrical symmetry.

Electric flux has SI units of volt meters ( $V m$ ), or, equivalently, newton meters squared per coulomb ( $N m 2 C -1$ ). Thus, the SI base units of electric flux are $kg\cdotm 3 \cdots -3 \cdotA -1$ . Its dimensional formula is ${\mathsf {L}}^{3}{\mathsf {MT}}^{-3}{\mathsf {I}}^{-1}$ .

Notes[]

Purcell, Edward, Morin, David; Electricity and Magnetism, 3rd Edition; Cambridge University Press, New York. 2013 ISBN 9781107014022.
Browne, Michael, PhD; Physics for Engineering and Science, 2nd Edition; McGraw Hill/Schaum, New York; 2010. ISBN 0071613994

References[]

^ Purcell, p22-26
^ Purcell, p5-6.

External links[]

Electric flux — HyperPhysics

[1] Purcell, p22-26

[2] Purcell, p5-6.

[1]

[2]

Electric flux

Contents

Overview[]

See also[]

Notes[]

References[]

External links[]