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Original Ampères law In its original form, Ampère's law relates the magnetic field B to its source, the current density J: where is the closed line integral around contour (closed curve) . is the magnetic flux density in teslas, is an infinitesimal element (differential) of the contour , is the current density (in amperes per square meter) through the surface S enclosed by contour C is a differential vector element of surface area A, with infinitesimally small magnitude and direction normal to surface S is the current enclosed by the curve , or strictly, the current that penetrates surface , is the permeability of free space (in henries per meter), Equivalently, the original equation in differential form is abla imes mathbf = mathbf where abla is the vector differential 'Del' is the cross product operator The magnetic field strength H in linear media, is related to the magnetic flux density B (in teslas) by Corrected Ampères law: the Ampère-Maxwell equation James Clerk Maxwell noticed a logical inconsistency when applying Ampère's law to a charging or discharging capacitor. If surface passes between the plates of the capacitor, and not through any wires, then even though . He concluded that this law had to be incomplete. To resolve the problem, he came up with the concept of displacement current and made a generalized version of Ampère's law which was incorporated into Maxwell's equations. The generalized law, as corrected by Maxwell, takes the following integral form: iint_S mathbf cdot d mathbf where in linear media is the displacement current density (in amperes per square meter). This Ampère-Maxwell law can also be stated in differential form: abla imes mathbf = mathbf + rac where the second term arises from the displacement current. With the addition of the displacement current, Maxwell was able to postulate (correctly) that light was a form of electromagnetic wave. See Electromagnetic wave equation for a discussion on this important discovery. See also | ||||||||||
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