Gauss' law (magnetism)

In physics, more specifically in electromagnetism, Gauss' law is a theorem concerning a surface integral of magnetic induction B. Mathematically, Gauss' law for magnetism has the form:

$\iint _{\mathrm {closed} \atop \mathrm {surface} }\mathbf {B} \cdot d\mathbf {S} =0$

Here dS is an vector with length dS, the area of an infinitesimal surface element on the closed surface, and direction perpendicular to the surface element dS, pointing outward. The vector B is the magnetic induction (in vacuum proportional to the magnetic field H) at the position dS, the dot indicates a dot product between the vectors B and dS. The double integral is over a closed surface that may envelop one or more permanent magnets and electric current carrying wires. The law is called after the German mathematician Carl Friedrich Gauss.

By application of the divergence theorem Gauss' law becomes one of Maxwell's equations, namely, the divergence of the field B is zero everywhere,

${\boldsymbol {\nabla }}\cdot \mathbf {B} =0.$

Magnetic monopole

A surface integral of B is often called magnetic flux denoted by Φ,

$\Phi \equiv \iint _{S}\mathbf {B} \cdot d\mathbf {S} .$

In electrostatics one defines an electric flux Ψ,

$\Psi \equiv \iint _{S}\mathbf {D} \cdot d\mathbf {S}$

where the displacement D is equal to the electric constant ε₀ times the electric field E (in SI units and vacuum). Gauss' law for electrostatics states that electric charge is the source of flux through a closed surface

$\Psi =\iint _{\mathrm {closed} \atop \mathrm {surface} }\mathbf {D} \cdot d\mathbf {S} =Q_{\mathrm {tot} }.$

Since the corresponding integral of B over a closed surface is always zero, one concludes that a magnetic charge (magnetic monopole) cannot exist, neither as permanent monopole, nor as monopole induced by an electric current.