Page:A history of the theories of aether and electricity. Whittacker E.T. (1910).pdf/131

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from Bradley to Fresnel.
111

substance; the spheroid being in the former case oblate and in the latter oblong." Young then proceeds to a formal proof that "an impulse is propagated through every perpendicular section of a lamellar elastic substance in the form of an elliptic undulation." This must be regarded as the beginning of the dynamical theory of light in crystals. It was confirmed in a striking way not long afterwards by Brewster,[1] who found that compression in one direction causes an isotropic transparent solid to become doubly-refracting.

Meanwhile, in January, 1808, the French Academy had proposed as the subject for the physical prize in 1810, "To furnish a mathematical theory of double refraction, and to confirm it by experiment." Among those who resolved to compete was Étienne Louis Malus (b. 1775, d. 1812), a colonel of engineers who had seen service with Napoleon's expedition to Egypt. While conducting experiments towards the end of 1808 in a house in the Rue des Enfers in Paris, Malus happened to analyse with a rhomb of Iceland spar the light of the setting sun reflected from the window of the Luxembourg, and was surprised to notice that the two images were of very different intensities. Following up this observation, he found that light which bad been reflected from glass acquires thereby a modification similar to that which Huygens had noticed in rays which have experienced double refraction, and which Newton had explained by supposing rays of light to have "sides." This discovery appeared so important that without waiting for the prize competition he communicated it to the Academy in December, 1808, and published it in the following month.[2]

"I have found," he said, "that this singular disposition, which has hitherto been regarded as one of the peculiar effects of double refraction, can be completely impressed on the luminous molecules by all transparent solids and liquids." "For example, light reflected by the surface of water at an

  1. Pbil. Trans., 1815, p. 60.
  2. Nouveau Bulletin des Sciences, par la Soc. Philomatique, i (1809), p. 266; Mémoires de la Soc. d'Arcueil, ii (1809).