Electromagnetic induction is nothing but a process in which a conductor is held in a fixed position, and the magnetic field changes or remains constant as the conductor moves. This results in a voltage or EMF (electromotive force) being created across the electrical conductor.<\/p>\n\n\n\n
Electromagnetic induction was invented by Michael Faraday in 1831 and independently and almost simultaneously by Joseph Henry in 1832. Faraday discovered electromagnetic induction and demonstrated it with a copper coil around a toroidal piece of iron and a galvanometer (an instrument used to show electrical current) as a magnet. As the magnet moves toward the coil, an EMF is created, moving the gauge on the galvanometer.<\/p>\n\n\n\n
The discovery of electromagnetic induction is a fundamental principle in understanding and using electricity. James Clerk formulated Maxwell Faraday’s mathematical description of induction, later known as the Maxwell-Faraday equation.<\/p>\n\n\n\n
Facts connecting electricity and magnetism:<\/strong><\/p>\n\n\n\n Faraday’s laws of <\/strong>Electromagnetic Induction<\/strong>:<\/strong><\/p>\n\n\n\n In 1831 Michael Faraday developed two fundamental laws of electromagnetic induction. These laws are known as Faraday’s first law and Faraday’s second law of electromagnetic induction. These two laws describe how a changing magnetic field produces an EMF in a moving conductor.<\/p>\n\n\n\n The first law of Faraday states that:<\/p>\n\n\n\n When a conductor is placed in a periodically varying magnetic field, an e.m.f. (electromotive force) is induced across the conductor. An induced current is produced if a conductor is closed to form a circuit.<\/p>\n\n\n\n An equation that mathematically describes electromagnetic induction is Faraday’s law, which states that any change in the magnetic environment of a coiled wire induces a voltage (EMF). Faraday discovered several ways to change the magnetic field strength: moving a magnet through a coil of wire and a coil through a magnetic field. The following equation describes the voltage (EMF) produced in a coil of wire:<\/p>\n\n\n\n EMF = \u2212<\/strong>N(\u0394(<\/strong>BA)\/<\/strong>\u0394t)<\/strong><\/p>\n\n\n\n where<\/p>\n\n\n\n N is the number of wire turns<\/p>\n\n\n\n \u0394(BA) is the change in magnetic flux<\/p>\n\n\n\n \u0394t is the change in time<\/p>\n\n\n\n This law is EMF. It is produced by varying magnetic fields in the following manner:<\/p>\n\n\n\n EMF. The induced in a conductor equals the rate of change of flux associated with the conductor.<\/p>\n\n\n\n In practice, this law can be written as: \u03b5 = d\u03a6dt<\/p>\n\n\n\n Here, \u03b5 is the measure of e.m.f. Induced, \u03a6 is the value of the magnetic flux passing through the surface, and t is the time it takes for the flux to change. Since we usually have magnetic flux passing through several loops simultaneously, the general equation becomes: \u03b5 = Nd\u03a6dt, where N is the number or thickness of the loops.<\/p>\n\n\n\n Applications of Faraday\u2019s Laws of Electromagnetic Induction:<\/strong><\/p>\n\n\n\n Faraday’s laws are widely used in many fields of electrical engineering, such as electrical machines, measuring instruments, medicine for disease diagnosis, etc. Some typical applications of Faraday’s laws are:<\/p>\n\n\n\n Lenz’s Law of <\/u><\/strong>Electromagnetic Induction<\/u><\/strong>:<\/u><\/strong><\/p>\n\n\n\n Lenz’s Law states, “The polarity of the induced emf gives a current that opposes the change in magnetic flux that produced it.”<\/p>\n\n\n\n Lenz’s law is based on Newton’s third law and the principle of energy conservation. This is the simplest way to determine the direction of the induced current. Lenz’s law is named after Emil Lenz. There are also many Lenz Law applications. The principle of Lenz’s law is used in metal detectors, eddy current balances, card readers, AC generators, and more.<\/p>\n\n\n\n Lenz’s Law Formula;<\/p>\n\n\n\nTypes of Electromagnetic Induction<\/h3>\n\n\n\n
Electromagnetic Induction Applications<\/h2>\n\n\n\n