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In physics, specifically electromagnetism, the magnetic flux through a surface is the surface integral of the normal component of the magnetic field B over that surface. It is usually denoted Φ or Φ_B. The SI unit of magnetic flux is the weber (Wb; in derived units, volt–seconds or V⋅s), and the CGS unit is the maxwell.^[1] Magnetic flux is usually measured with a fluxmeter, which contains measuring coils, and it calculates the magnetic flux from the change of voltage on the coils.

The magnetic flux through a surface—when the magnetic field is variable—relies on splitting the surface into small surface elements, over which the magnetic field can be considered to be locally constant. The total flux is then a formal summation of these surface elements (see surface integration).

Each point on a surface is associated with a direction, called the surface normal; the magnetic flux through a point is then the component of the magnetic field along this direction.

The magnetic interaction is described in terms of a vector field, where each point in space is associated with a vector that determines what force a moving charge would experience at that point (see Lorentz force).^[1] Since a vector field is quite difficult to visualize, introductory physics instruction often uses field lines to visualize this field. The magnetic flux through some surface, in this simplified picture, is proportional to the number of field lines passing through that surface (in some contexts, the flux may be defined to be precisely the number of field lines passing through that surface; although technically misleading, this distinction is not important). The magnetic flux is the net number of field lines passing through that surface; that is, the number passing through in one direction minus the number passing through in the other direction (see below for deciding in which direction the field lines carry a positive sign and in which they carry a negative sign).^[2] More sophisticated physical models drop the field line analogy and define magnetic flux as the surface integral of the normal component of the magnetic field passing through a surface. If the magnetic field is constant, the magnetic flux passing through a surface of vector area S is $${\displaystyle \Phi _{B}=\mathbf {B} \cdot \mathbf {S} =BS\cos \theta ,}$$ where B is the magnitude of the magnetic field (the magnetic flux density) having the unit of Wb/m² (tesla), S is the area of the surface, and θ is the angle between the magnetic field lines and the normal (perpendicular) to S. For a varying magnetic field, we first consider the magnetic flux through an infinitesimal area element dS, where we may consider the field to be constant: $${\displaystyle d\Phi _{B}=\mathbf {B} \cdot d\mathbf {S} .}$$ A generic surface, S, can then be broken into infinitesimal elements and the total magnetic flux through the surface is then the surface integral $${\displaystyle \Phi _{B}=\iint _{S}\mathbf {B} \cdot d\mathbf {S} .}$$ From the definition of the magnetic vector potential A and the fundamental theorem of the curl the magnetic flux may also be defined as: $${\displaystyle \Phi _{B}=\oint _{\partial S}\mathbf {A} \cdot d{\boldsymbol {\ell }},}$$ where the line integral is taken over the boundary of the surface S, which is denoted ∂S.

Gauss's law for magnetism, which is one of the four Maxwell's equations, states that the total magnetic flux through a closed surface is equal to zero. (A "closed surface" is a surface that completely encloses a volume(s) with no holes.) This law is a consequence of the empirical observation that magnetic monopoles have never been found.

In other words, Gauss's law for magnetism is the statement:

${\displaystyle \Phi _{B}=\,\!}$ ${\displaystyle \scriptstyle S}$ ${\displaystyle \mathbf {B} \cdot d\mathbf {S} =0}$

for any closed surface S.

While the magnetic flux through a closed surface is always zero, the magnetic flux through an open surface need not be zero and is an important quantity in electromagnetism.

When determining the total magnetic flux through a surface only the boundary of the surface needs to be defined, the actual shape of the surface is irrelevant and the integral over any surface sharing the same boundary will be equal. This is a direct consequence of the closed surface flux being zero.

For example, a change in the magnetic flux passing through a loop of conductive wire will cause an electromotive force (emf), and therefore an electric current, in the loop. The relationship is given by Faraday's law: $${\displaystyle {\mathcal {E}}=\oint _{\partial \Sigma }\left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)\cdot d{\boldsymbol {\ell }}=-{\frac {d\Phi _{B}}{dt}},}$$ where:

• ${\displaystyle {\mathcal {E}}}$ is the electromotive force (EMF),
• The minus sign represents Lenz's Law,
• Φ_B is the magnetic flux through the open surface Σ,
• ∂Σ is the boundary of the open surface Σ; the surface, in general, may be in motion and deforming, and so is generally a function of time. The electromotive force is induced along this boundary.
• dℓ is an infinitesimal vector element of the contour ∂Σ,
• v is the velocity of the boundary ∂Σ,
• E is the electric field, and
• B is the magnetic field.

The two equations for the EMF are, firstly, the work per unit charge done against the Lorentz force in moving a test charge around the (possibly moving) surface boundary ∂Σ and, secondly, as the change of magnetic flux through the open surface Σ. This equation is the principle behind an electrical generator.

By way of contrast, Gauss's law for electric fields, another of Maxwell's equations, is

${\displaystyle \Phi _{E}=\,\!}$ ${\displaystyle \scriptstyle S}$ ${\displaystyle \mathbf {E} \cdot d\mathbf {S} ={\frac {Q}{\varepsilon _{0}}}\,\!}$

where

• E is the electric field,
• S is any closed surface,
• Q is the total electric charge inside the surface S,
• ε₀ is the electric constant (a universal constant, also called the "permittivity of free space").

The flux of E through a closed surface is not always zero; this indicates the presence of "electric monopoles", that is, free positive or negative charges.

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Electrostatics Electric charge Coulomb's law Conductor Charge density Permittivity Electric dipole moment Electric field Electric potential Electric flux / potential energy Electrostatic discharge Gauss's law Induction Insulator Polarization density Static electricity Triboelectricity
Magnetostatics Ampère's law Biot–Savart law Gauss's law for magnetism Magnetic field Magnetic flux Magnetic dipole moment Magnetic permeability Magnetic scalar potential Magnetization Magnetomotive force Magnetic vector potential Right-hand rule
Electrodynamics Lorentz force law Electromagnetic induction Faraday's law Lenz's law Displacement current Maxwell's equations Electromagnetic field Electromagnetic pulse Electromagnetic radiation Larmor formula Bremsstrahlung Cyclotron radiation Synchrotron radiation Maxwell tensor Poynting vector Liénard–Wiechert potential Jefimenko's equations Eddy current London equations Mathematical descriptions of the electromagnetic field
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Covariant formulation Electromagnetic tensor (stress–energy tensor) Four-current Electromagnetic four-potential
Scientists Ampère Biot Coulomb Davy Einstein Faraday Fizeau Gauss Heaviside Henry Hertz Hopkinson Jefimenko Joule Kelvin Lenz Liénard Lorentz Maxwell Neumann Ørsted Ohm Poynting Ritchie Savart Singer Steinmetz Tesla Volta Weber Wiechert Poisson
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• Dannatt plates, thick sheets made of electrical conductors
• Flux linkage, an extension of the concept of magnetic flux
• Magnetic circuit is a closed path in which magnetic flux flows
• Magnetic flux quantum is the quantum of magnetic flux passing through a superconductor

• Media related to Magnetic flux at Wikimedia Commons
• US 6720855, Vicci, "Magnetic-flux conduits", issued 2003 
• Magnetic Flux through a Loop of Wire by Ernest Lee, Wolfram Demonstrations Project.
• Conversion Magnetic flux Φ in nWb per meter track width to flux level in dB – Tape Operating Levels and Tape Alignment Levels
• wikt:magnetic flux