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・ Induction sealing
・ Induction shrink fitting
・ Induction training
・ Induction variable
・ Induction welding
・ Induction-recursion (type theory)
・ Inductionism
・ Inductive amplifier
・ Inductive Automation
・ Inductive bias
・ Inductive charging
・ Inductive cleavage
・ Inductive coupling
・ Inductive data type
・ Inductive dimension
Inductive discharge ignition
・ Inductive effect
・ Inductive functional programming
・ Inductive logic programming
・ Inductive output tube
・ Inductive probability
・ Inductive programming
・ Inductive pump
・ Inductive reasoning
・ Inductive reasoning aptitude
・ Inductive sensor
・ Inductive set
・ Inductive transfer
・ Inductive type
・ Inductively coupled plasma


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Inductive discharge ignition : ウィキペディア英語版
Inductive discharge ignition

Inductive discharge ignition systems were developed in the 19th century as a means to ignite the air-fuel mixture in the combustion chamber of internal combustion engines. The first versions were low tension coils, then low-tension and in turn high-tension magnetos, which were offered as a more effective alternative to the older-design hot-tube ignitors that had been utilized earlier on hot tube engines. With the advent of small stationary engines; and with the development of the automobile, engine-driven tractors, and engine-driven trucks; first the magneto and later the distributor-type systems were utilized as part of an efficient and reliable engine ignition system on commercially available motorized equipment. These systems were in widespread use on all cars and trucks through the 1960s. Manufacturers such as Ford, General Motors, Chrysler, Citroen, Mercedes, John Deere, International Harvester, and many others incorporated them into their products. The inductive discharge system is still extensively used today. Most people today are familiar with it as a "points-type" ignition system.
==Faraday's Law==
The inductive-discharge ignition system operates according to the rules of electromagnetism described by Faraday's Law of Induction which states that the induction of electromotive force (emf) in any closed circuit is equal to the time rate of change of the magnetic flux through the circuit. In other words, the emf generated is proportional to the rate of change of the magnetic flux. More simply stated, an electric field is induced in any system in which a magnetic field is changing with time. The change could be changes in direction of force or strength. The effects described by this law are those by which generators, motors, alternators, and transformers function. There are two main concepts to be taken from Faraday's Law that apply to the design of inductive discharge ignitions. One is that moving a wire through a magnetic field will induce an electric voltage and current in the wire, aka electromagnetic induction. The second is that current moving in a wire will induce a magnetic field around the wire.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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