APS March Meeting 2012
Volume 57, Number 1
Monday–Friday, February 27–March 2 2012;
Boston, Massachusetts
Session B19: Invited Session: One Hundred Fifty Years of Maxwell's Equations (1862-2012)
11:15 AM–2:15 PM,
Monday, February 27, 2012
Room: 253AB
Sponsoring
Unit:
FHP
Chair: Edward Gerjuoy, University of Pittsburgh
Abstract ID: BAPS.2012.MAR.B19.1
Abstract: B19.00001 : The discovery of Maxwell's equations
11:15 AM–11:51 AM
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Abstract
Author:
Francis Everitt
(Stanford University)
In January 1865, Maxwell at age 34 wrote a letter to his cousin Charles Cay
describing various doings, including his work on the viscosity of gases and
a visit from two of the world's leading oculists to inspect the eyes of his
dog ``Spice''. He added, ``I have also a paper afloat, with an
electromagnetic theory of light, which, till I am convinced to the contrary,
I hold to be great guns.''
That paper ``A Dynamical Theory of the Electromagnetic Field'' was his
fourth on the subject. It was followed in 1868 by another, and then in 1873
by his massive two volume \underline {Treatise on Electricity and
Magnetism}. Even so, by the time of his death in 1879 as he was beginning a
radically revised edition of the \underline {Treatise}, much remained to be
done. We celebrate here the 150$^{th}$ anniversary of Maxwell's first
astonished realization in 1862 of the link between electromagnetism and
light. So revolutionary was this that 15 or more years went by before
Lorentz, Poynting, FitzGerald, and others came to address it, sometimes with
improvements, sometimes not. Not until 1888 did Hertz make the essential
experimental discovery of radio waves.
What is so remarkable about Maxwell's five papers is that each presents a
complete view of the subject radically different from the one before. I
shall say something about each, emphasizing in particular Maxwell's most
unexpected idea, the displacement current, so vastly more interesting than
the accounts of it found in textbooks today. Beyond lie other surprises. The
concept of gauge invariance, and the role the vector potential would play in
defining the canonical momentum of the electron, both go back to Maxwell. In
1872 came a paper ``On the Mathematical Classification of Physical
Quantities'', which stands as an education in itself. Amid much else, there
for the first time appears the distinction between axial and polar vectors
and those new operational concepts related to quaternion theory: \textit{curl, divergence, }and\textit{ gradient}.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.MAR.B19.1