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    In physics, Ampère's law, discovered by André-Marie Ampère, relates the circulating magnetic field in a closed loop to the electric current passing through the loop. It is the magnetic equivalent of Faraday's law of induction.


        Ampère's law
            Original Ampères law
            Corrected Ampères law: the Ampère-Maxwell equation
            See also

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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:

    oint_C rac cdot dmathbf = int!!!!int_S mathbf cdot d mathbf = I_

    where

    oint_C is the closed line integral around contour (closed curve) C.

    mathbf is the magnetic flux density in teslas,

    dmathbf is an infinitesimal element (differential) of the contour C,

    mathbf is the current density (in amperes per square meter) through the surface S enclosed by contour C

    d mathbf ! is a differential vector element of surface area A, with infinitesimally small magnitude and direction normal to surface S

    I_ ! is the current enclosed by the curve C, or strictly, the current that penetrates surface S,

    mu_0 = 4 pi imes 10^ 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'
    imes, is the cross product operator



    The magnetic field strength H in linear media, is related to the magnetic flux density B (in teslas) by

    mathbf = mu mathbf




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    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 S passes between the plates of the capacitor, and not through any wires, then mathbf = 0 even though oint_C mathbf cdot dmathbf
    e 0. 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:

    oint_C mathbf cdot dmathbf = iint_S mathbf cdot d mathbf +

    iint_S mathbf cdot d mathbf

    where in linear media

    mathbf = varepsilon mathbf


    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.

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    This article is licensed under the GNU Free Documentation License [copyleft]. It uses material from the Wikipedia article "Ampère's law". link