Lenz's law (pronounced (IPA) ) was formulated by German physicist Heinrich Lenz in 1833 and gives the direction of the induced emf resulting from electromagnetic induction, thus:
It is important to note that the induced current will always flow in a direction which opposes any change of magnetic flux, but it does not oppose the magnetic flux itself.
Lenz's law can be derived from Faraday's law of induction, simply by noting the minus sign on the right side of the equation.
Suppose instead that the current was produced in the opposite direction. Then the south pole of the induced magnetic field would be in the direction of the north pole of the magnet, to which the magnet would be accelerated by the field. As the magnet accelerates, the current in the loop would increase, causing an increasing force on the magnet and an increasing acceleration. Both the kinetic energy of the magnet and the rate of energy dissipation in the loop would increase. This means that for a very small push we would get a large energy dissipation which clearly violates the law of conservation of energy. Therefore the emf opposes the change that induces it, i.e. the change in magnetic flux.
See electromagnetic induction and Maxwell's equations for further mathematical treatment.
Electrodynamics | Eponymous laws
লেন্জের সূত্র | Lenzův zákon | Lenzsche Regel | Ley de Lenz | Loi de Lenz | 렌츠의 법칙 | Legge di Lenz | חוק לנץ | Lenz-törvény | Wet van Lenz | Prawo Lenza | Lenzovo pravilo | Ленцов закон | லென்சின் விதி | Định luật Lenz | 楞次定律
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