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**Definition/Summary**Flux sometimes means total flow through a surface (a scalar), and sometimes means flow per unit area (a vector).

In electromagnetism, flux always means total flow through a surface (a scalar), and is measured in webers (magnetic flux) or volt-metres (electric flux).

Scalar flux is the amount of a vector field going through a surface: it is the integral (over the surface) of the normal component of the field: [itex]\Phi\ =\ \oint_S\mathbf{E}\cdot d\mathbf{A}[/itex]

For a closed surface, this equals (Gauss' theorem, or the divergence theorem) the integral (over the interior) of the divergence of the field: [itex]\Phi\ =\ \int\int\int_V \mathbf{\nabla}\cdot\mathbf{E}\,dxdydz[/itex].

Therefore the scalar flux, through a closed surface, of an electric field is proportional to the enclosed charge (Gauss' law: [itex]\Phi_{E}\ =\ Q_{total}/\varepsilon_0,\ \ \Phi_{D}\ =\ Q_{free}/\varepsilon_0,\ \ \Phi_{P}\ =\ -Q_{bound}/\varepsilon_0[/itex]), and of a magnetic field is zero (Gauss' law for magnetism: [itex]\Phi_{B}\ =\ \Phi_{H}\ =\ \Phi_{M}\ =\ 0[/itex]).

**Equations**FLUX THROUGH A CLOSED SURFACE, S:

Gauss' Law:

[tex]\Phi_\mathbf{E}(S)\ =\ \oint_S\mathbf{E}\cdot d\mathbf{A}\ =\ Q/\varepsilon_0[/tex]

Gauss' Law for Magnetism:

[tex]\Phi_\mathbf{B}(S)\ =\ \oint_S\mathbf{B}\cdot d\mathbf{A}\ =\ 0[/tex]

RATE OF CHANGE OF FLUX THROUGH A CLOSED CURVE, C:

Ampère-Maxwell Law:

[tex]\mu_0\varepsilon_0\frac{\partial\Phi_\mathbf{E}(S)}{\partial t}\ =\ \mu_0\varepsilon_0\frac{\partial}{\partial t}\int_S\mathbf{E}\cdot d\mathbf{A}\ =\ \oint_C\mathbf{B}\cdot d\mathbf{\ell}\ -\ \mu_0I[/tex]

Faraday's law:

[tex]\frac{\partial\Phi_\mathbf{B}(S)}{\partial t}\ =\ \frac{\partial}{\partial t}\int_S \mathbf{B}\cdot d\mathbf{A}\ =\ -\oint_C\mathbf{E}\cdot d\mathbf{\ell}[/tex]

E and B are the electric and magnetic fields; a closed surface is the boundary of a volume, and Q is the charge within that volume; in the last two laws, S is any surface whose boundary is the closed curve C; I is the current passing through C or S; the symbol [itex]\oint[/itex] indicates that the integral is over a closed surface or curve

those are the flux (or integral) versions of the total-charge versions of Maxwell's equations; there are also free-charge versions of Gauss' law and the Ampère-Maxwell law which use D H free charge and free current:

Gauss' Law:

[tex]\Phi_\mathbf{D}(S)\ =\ \oint_S\mathbf{D}\cdot d\mathbf{A}\ =\ Q_{free}[/tex]

Ampère-Maxwell Law:

[tex]\frac{\partial\Phi_\mathbf{D}(S)}{\partial t}\ =\ \frac{\partial}{\partial t}\int_S\mathbf{D}\cdot d\mathbf{A}\ =\ \oint_C\mathbf{H}\cdot d\mathbf{\ell}\ -\ I_{free}[/tex]

**Extended explanation****Scalar flux vs vector flux:**

The

**vector**form of flux is the density (

*per area*, not the usual density

*per volume*) of the scalar form of flux.

In electromagnetism, it is called the flux density …

ie, in electromagnetism, flux is flow across a surface, and flux density is the density (per area) of that flow;

flux in other topics, is the same as flux density in electromagnetism.

flux in other topics, is the same as flux density in electromagnetism.

**Flux density in electromagnetism:**

Magnetic flux, [itex]\Phi_m[/itex], is a scalar, measured in webers (or volt-seconds), and is a total amount measured across a surface (ie, you don't have flux at a point).

Magnetic flux density, [itex]\mathbf{B}[/itex], is a vector, measured in webers per square metre (or teslas), and exists at each point.

The flux across a surface S is the integral of the magnetic flux density over that surface:

[itex]\Phi_m\ =\ \int\int_S\ \mathbf{B}\cdot d\mathbf{S}[/itex]

(and is zero across a *closed*surface)

Magnetic flux density is what physicists more commonly call the

**magnetic field**.

It is a density

*per area*, rather than the usual density per volume.

Similarly,

*electric*flux, [itex]\Phi_e[/itex], is a scalar, measured in volt-metres, and*electric*flux density (also a density*per area*), [itex]\mathbf{E}[/itex], is a vector, measured in volts per metre (and is more commonly called the**electric field**).* This entry is from our old Library feature. If you know who wrote it, please let us know so we can attribute a writer. Thanks!