Maxwell's equations


 

Maxwell's equations are the set of four equations, attributed to James Clerk Maxwell (written by Oliver Heaviside), that describe the behavior of both the electric and magnetic fields, as well as their interactions with matter.

Related Topics:
James Clerk Maxwell - Oliver Heaviside - Electric and magnetic fields

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Maxwell's four equations express, respectively, how electric charges produce electric fields (Gauss' law), the experimental absence of magnetic charges, how currents produce magnetic fields (Ampere's law), and how changing magnetic fields produce electric fields (Faraday's law of induction). Maxwell, in 1864, was the first to put all four equations together and to notice that a correction was required to Ampere's law: changing electric fields act like currents, likewise producing magnetic fields. (This additional term is called the displacement current.)

Related Topics:
Electric charge - Electric field - Gauss' law - Magnetic charge - Current - Magnetic field - Ampere's law - Faraday's law of induction - 1864 - Displacement current

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Furthermore, Maxwell showed that waves of oscillating electric and magnetic fields travel through empty space at a speed that could be predicted from simple electrical experiments—using the data available at the time, Maxwell obtained a velocity of 310,740,000 m/s. Maxwell (1865) wrote:

Related Topics:
Wave - M/s - 1865

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:This velocity is so nearly that of light, that it seems we have strong reason to conclude that light itself (including radiant heat, and other radiations if any) is an electromagnetic disturbance in the form of waves propagated through the electromagnetic field according to electromagnetic laws.

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Maxwell was correct in this conjecture, though he did not live to see its vindication by Heinrich Hertz in 1888. Maxwell's quantitative explanation of light as an electromagnetic wave is considered one of the great triumphs of 19th-century physics. (Actually, Michael Faraday had postulated a similar picture of light in 1846, but had not been able to give a quantitative description or predict the velocity.) Moreover, it laid the foundation for many future developments in physics, such as special relativity and its unification of electric and magnetic fields as a single tensor quantity, and Kaluza and Klein's unification of electromagnetism with gravity and general relativity.

Related Topics:
Heinrich Hertz - 1888 - Light - Michael Faraday - 1846 - Special relativity - Tensor - Kaluza and Klein - Gravity - General relativity

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~ Table of Content ~

Introduction
Historical developments of Maxwell's equations and relativity
Summary of the equations
Detail
Maxwell's equations in CGS units
Formulation of Maxwell's equations in special relativity
Maxwell's equations in terms of differential forms
Classical electrodynamics as a line bundle
See also
References
External links

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