Eddy currents (also called
Foucault's currents) are loops of
electrical current induced within
conductors by a changing
magnetic field in the conductor according to
Faraday's law of induction. Eddy currents flow in closed loops within conductors, in planes perpendicular to the magnetic field. They can be induced within nearby stationary conductors by a time-varying magnetic field created by an AC
electromagnet or
transformer, for example, or by relative motion between a
magnet and a nearby conductor. The magnitude of the current in a given loop is proportional to the strength of the magnetic field, the area of the loop, and the rate of change of flux, and inversely proportional to the
resistivity of the material. When graphed, these circular currents within a piece of metal look vaguely like eddies or whirlpools in a liquid.
By
Lenz's law, an eddy current creates a magnetic field that opposes the change in the magnetic field that created it, and thus eddy currents react back on the source of the magnetic field. For example, a nearby conductive surface will exert a drag force on a moving magnet that opposes its motion, due to eddy currents induced in the surface by the moving magnetic field. This effect is employed in
eddy current brakes which are used to stop rotating power tools quickly when they are turned off. The current flowing through the resistance of the conductor also dissipates energy as
heat in the material. Thus eddy currents are a cause of energy loss in alternating current (AC)
inductors,
transformers,
electric motors and
generators, and other AC machinery, requiring special construction such as
laminated magnetic cores or
ferrite cores to minimize them. Eddy currents are also used to heat objects in
induction heating furnaces and equipment, and to detect cracks and flaws in metal parts using
eddy-current testing instruments.