Electrodynamics and relativity In 1892 and 1895, Lorentz worked on describing electromagnetic phenomena (the propagation of light) in reference frames that move relative to the postulated
luminiferous aether. He discovered that the transition from one to another reference frame could be simplified by using a new time variable that he called
local time and which depended on universal time and the location under consideration. Although he did not give a detailed interpretation of the physical significance of local time, with it, he could explain the
aberration of light and the result of the
Fizeau experiment. In 1900 and 1904,
Henri Poincaré called local time Lorentz's "most ingenious idea" and illustrated it by showing that clocks in moving frames are synchronized by exchanging light signals that are assumed to travel at the same speed against and with the motion of the frame In 1899 and again in 1904, Lorentz added
time dilation to his transformations and published what Poincaré in 1905 named
Lorentz transformations. It was apparently unknown to Lorentz that
Joseph Larmor had used identical transformations to describe orbiting electrons in 1897. Larmor's and Lorentz's equations look somewhat dissimilar, but they are algebraically equivalent to those presented by Poincaré and Einstein in 1905. known today as the
special theory of relativity. Einstein's unique perspective on the topic was not widely understood initially, causing some physicists to confusingly refer to the theory as the
Lorentz–Einstein theory. In 1910, Lorentz's 1906
lectures at
Columbia University, were published under the title
The Theory of Electrons. Lorentz covered his entire theory of the electron, including his work and that of Einstein on relativity. In this work he spoke affirmatively of Einstein's theory:
General relativity Lorentz was one of few scientists who supported Einstein's search for
general relativity from the beginning – he wrote several research papers and discussed with Einstein personally and by letter. For instance, he attempted to combine Einstein's formalism with
Hamilton's principle (1915), and to reformulate it in a
coordinate-free way (1916). Lorentz wrote in 1919:
Quantum mechanics Lorentz gave a series of lectures in the fall of 1926 at
Cornell University on the new
quantum mechanics; in these he presented
Erwin Schrödinger's
wave mechanics. == Civil work ==