Maxwell's equations

Maxwell's equations for electromagnetism

Maxwell's equations are a set of partial differential equations that, together with the Lorentz force law, form the foundation of classical electromagnetism, classical optics, and electric circuits. The equations are named after the physicist and mathematician James Clerk Maxwell, who, in 1861 and 1862, published an early form of the equations that included the Lorentz force law. Maxwell proposed that light (including radiant heat, and other radiations if any) is an electromagnetic phenomenon, based upon deriving of the speed of light from his equations.

Quotes

• ... applications in gauge field theories and the physics of condensed matter. The starting point here is now quite well known: expressing the Maxwell equations for an electromagnetic field over Lorentz space as the Euler-Lagrange equations for a Lagrangian defined on the connections on a $U(1)$ bundle, where the electromagnetic potential becomes the connection and the field tensor its curvature. The freedom of choice of "gauge" for the potential is a fundamental fact which stems, in the geometrical picture, from the lack of a preferred trivialisation of the bundle.
  • Simon Donaldson: (1995). "Book Review: Topology of gauge fields and condensed matter by Michael Monastyrsky (translated from Russian by Oleg Efimov)". Bulletin of the American Mathematical Society 32 (2): 248–251. ISSN 0273-0979. DOI:10.1090/S0273-0979-1995-00574-4. (quote from p. 249)

• But the mathematicians of the nineteenth century failed miserably to grasp the equally great opportunity offered to them in 1865 by Maxwell. If they had taken Maxwell's equations to heart as Euler took Newton's, they would have discovered, among other things, Einstein's theory of special relativity, the theory of topological groups and their linear representations, and probably large pieces of the theory of hyperbolic differential equations and functional analysis. A great part of twentieth century physics and mathematics could have been created in the nineteenth century, simply by exploring to the end the mathematical concepts to which Maxwell's equations naturally lead.
  • Dyson, Freeman J. Missed opportunities. Bull. Amer. Math. Soc. 78 (1972), no. 5, 635--652. http://projecteuclid.org/euclid.bams/1183533964.

• We have a wave which leaves the material source and goes outward at the velocity c, which is the speed of light. ... From a historical point of view, it wasn’t known that the coefficient c in Maxwell’s equations was also the speed of light propagation. There was just a constant in the equations. We have called it c from the beginning, because we knew what it would turn out to be. We didn’t think it would be sensible to make you learn the formulas with a different constant and then go back to substitute c wherever it belonged. ... just by experiments with charges and currents we find a number c² which turns out to be the square of the velocity of propagation of electromagnetic influences. From static measurements—by measuring the forces between two unit charges and between two unit currents—we find that c = 3.00 × 10⁸ meters/sec. When Maxwell first made this calculation with his equations, he said that bundles of electric and magnetic fields should be propagated at this speed. He also remarked on the mysterious coincidence that this was the same as the speed of light. “We can scarcely avoid the inference,” said Maxwell, “that light consists in the transverse undulations of the same medium which is the cause of electric and magnetic phenomena.” Maxwell had made one of the great unifications of physics. Before his time, there was light, and there was electricity and magnetism. The latter two had been unified by the experimental work of Faraday, Oersted, and Ampère. Then, all of a sudden, light was no longer “something else,” but was only electricity and magnetism in this new form—little pieces of electric and magnetic fields which propagate through space on their own.
  • Richard Feynman: (1964). 18–5. The speed of light in Chapter 18. The Maxwell Equations, The Feynman Lectures on Physics, Volume II, Mainly Electromagnetism and Matter

• ... the fullest statement Maxwell gave of his theory, his 1873 Treatise on Electricity and Magnetism, does not contain the four famous "Maxwell's equations," nor does it even hint at how electromagnetic waves might be produced or detected. These and many other aspects of the theory were quite thoroughly hidden in the version of it given by Maxwell himself; in the words of Oliver Heaviside, they were "latent" but hardly "patent." ... Maxwell was only forty-eight when he died of cancer in November 1879. ... the task of digging out the "latent" aspects of his theory and of exploring its wider implications was thus left to a group of younger physicists, most of them British.
  • Bruce J. Hunt: The Maxwellians. Cornell University Press. 2005. pp. 1–2. ISBN 0-8014-8234-8. 

• ... the orginal field equations explicitly contain the magnetic vector potential, ${\overrightarrow {A}}$ ... In Maxwell's original formulaton, Faraday's ${\overrightarrow {A}}$ field was central and had physical meaning. The magnetic vector potential was not arbitrary, as defined by boundary conditions and choice of gauge as we will discuss; they were said to be gauge invariant. The original equations are thus often called the Faraday-Maxwell theory.
  • Paul G. Huray (16 November 2009). Maxwell's Equations. John Wiley & Sons. pp. 21–22. ISBN 978-0-470-54276-7. 

• The general equations are next applied to the case of a magnetic disturbance propagated through a non-conductive field, and it is shown that the only disturbances which can be so propagated are those which are transverse to the direction of propagation, and that the velocity of propagation is the velocity v, found from experiments such as those of Weber, which expresses the number of electrostatic units of electricity which are contained in one electromagnetic unit. 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.
  • James Clerk Maxwell, A Dynamical Theory of the Electromagnetic Field (1864), Introduction, p. 466, §20.

• Whenever I teach a course on electromagnetism, one of the first ... exam questions I will ask students is, "Why is the magnetic field called $H$ in the textbook?" ... The reason it is called $H$ is, of course, Maxwell did not use the vector notation. He writes out all the components. So the electric field he starts with $E$ ... And so, the electric field is $E,F,G,$ and the magnetic field is, obviously, $H,I,J.$ ... So all six components are written out. And so, it's very misleading for a textbook nowadays to say there are four Maxwell's equations. There were actually, if you look at Maxwell's papers, something like twenty-four equations. And the whole thing looks incredibly complicated.
  • Anthony Zee: (December 7, 2013)"Quantum Field Theory, Anthony Zee | Lecture 1 of 4 (lectures in 2004)". aoflex, YouTube. (quote at 11:42 of 1:36:31)

See also

• Electrical engineering
• Electricity
• Electromagnetism
• Magnetism
• Michael Faraday
• History of science
• James Clerk Maxwell
• Physics