Examples of 1/R potentials include the electric potential, the magnetic potential and the gravitational potential of point sources.

The magnetic vector potential can then be written as

The magnetic potential difference between any two points.

Due to the pre-magnetization, the magnetic potential difference between neighboring magnetic circuits is reduced.

where A is a magnetic potential (non-unique vector).

A magnetic potential of the outer pole piece is generated by applying a current to the primary coil winding.

Examples of 1/R potentials include the electric potential, the magnetic potential and the gravitational potential of point sources.

The electric force, which arises either due to a gradient in the electric potential or due to a time-varying magnetic vector potential.

The magnetic potential A is therefore determined at within the gradient of a scalar field Ψ.

It can also mean the difference in magnetic potential between a positive charge and a neutral mass or a null electromagnetic potential.

A separate magnetic potential of each sector is generated by applying current to each sector of the outer pole piece.

A is the magnetic potential relative to O (in m-1.s.V or kg.m.s-2.A-1).

The Electric potential V and the Magnetic potential A are defined from relations (R2) and (R3) by the following relations (see proof below) :

The principle of the device function consists in generating a pulse vector magnetic potential, which has a destroying and irreversible effect on live material.