External magnetic field produced by a magnetic dipole moment
In classical physics, the magnetic field of a dipole is calculated as the limit of either a current loop or a pair of charges as the source shrinks to a point while keeping the magnetic moment constant. For the current loop, this limit is most easily derived for the vector potential. Outside of the source region, this potential is with being the surface of a sphere of radius ; and the magnetic flux density in teslas is Equivalently, if is the unit vector in the direction of In spherical coordinates with the magnetic moment aligned with the z-axis, if we use, then this relation can be expressed as Alternatively one can obtain the scalar potential first from the magnetic pole limit, and hence the magnetic field strength in ampere-turns per meter is The magnetic field is symmetric under rotations about the axis of the magnetic moment.
Internal magnetic field of a dipole
The two models for a dipole, give the same predictions for the magnetic field far from the source. However, inside the source region they give different predictions. The magnetic field between poles is in the opposite direction to the magnetic moment, while inside a current loop it is in the same direction. Clearly, the limits of these fields must also be different as the sources shrink to zero size. This distinction only matters if the dipole limit is used to calculate fields inside a magnetic material. If a magnetic dipole is formed by making a current loop smaller and smaller, but keeping the product of current and area constant, the limiting field is where is the Dirac delta function in three dimensions. Unlike the expressions in the previous section, this limit is correct for the internal field of the dipole. If a magnetic dipole is formed by taking a "north pole" and a "south pole", bringing them closer and closer together but keeping the product of magnetic pole-charge and distance constant, the limiting field is These fields are related by, where is the magnetization.
Forces between two magnetic dipoles
The force exerted by one dipole moment on another separated in space by a vector can be calculated using: or where is the distance between dipoles. The force acting on is in the opposite direction. The torque can be obtained from the formula
Dipolar fields from finite sources
The magnetic scalar potential produced by a finite source, but external to it, can be represented by a multipole expansion. Each term in the expansion is associated with a characteristic moment and a potential having a characteristic rate of decrease with distance from the source. Monopole moments have a rate of decrease, dipole moments have a rate, quadrupole moments have a rate, and so on. The higher the order, the faster the potential drops off. Since the lowest-order term observed in magnetic sources is the dipolar term, it dominates at large distances. Therefore, at large distances any magnetic source looks like a dipole of the same magnetic moment.