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Thus an inductor resists changes in current. A pure inductor does not offer any resistance to direct current (an actual one does slightly), except when the current is switched on and off, then it makes the change more gradual.
When a sinusoidal alternating current flows through an inductor, a sinusoidal alternating voltage (or electromotive force, abbr. emf) is induced. The amplitude of the emf is related to the amplitude of the current and to the frequency of the sinusoid by the following equation.
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2 History 3 See also 4 Synonyms |
An inductor is usually constructed as a coil of conducting material, usually copper wire. A core of ferrous material is sometimes used. Inductors can also be built on integrated circuits using the same processes that are used to make computer chips. In these cases, aluminum is typically used as the conducting material. (However it is rare that actual inductors are built on ICs, it is far more common to use a circuit called a "gyrator" to make a capacitor appear to the IC as if it were an inductor.)
This effect can be understood as follows: the current produces a magnetic field; a change in current gives a change of this magnetic field; a changing magnetic field causes an electromotive force in the conductor. An induction coil is closely related to electromagnets in structure, but used for a different purpose—to store energy in a magnetic field.
Smaller inductors used for very high frequencies are sometimes made with a wire passing through a ferrite cylinder or bead.
In 1885, William Stanley, Jr built the first practical induction coil based on Lucien Gaulard and Josiah Willard Gibbs' idea. It was the precursor of the modern transformer.
Construction
History
See also
Electricity, Electronics, Capacitor, Transformer, Gyrator