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HERTZ, HEINRICH RUDOLF (1857-1894)

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Originally appearing in Volume V13, Page 401 of the 1911 Encyclopedia Britannica.
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HERTZ, HEINRICH See also:RUDOLF (1857-1894) , See also:German physicist, was See also:born at See also:Hamburg on the 22nd of See also:February 1857. On leaving school he determined to adopt the profession of See also:engineering, and in the pursuance of this decision went to study in See also:Munich in 1877. But soon coming to the conclusion that engineering was not his vocation he abandoned it in favour of See also:physical See also:science, and in See also:October 1878 began to attend the lectures of G. R. See also:Kirchhoff and H. von See also:Helmholtz at See also:Berlin. In preparation for these he spent the See also:winter of 1877–1878 in See also:reading up See also:original See also:treatises like those of See also:Laplace and See also:Lagrange on See also:mathematics and See also:mechanics, and in attending courses on See also:practical physics under P. G. von See also:Jolly and J. F. W. von Bezold; the consequence was that within a few days of his arrival in Berlin in October 1878 he was able to plunge into original See also:research on a problem of electric inertia. For the best See also:solution a See also:prize was offered by the philosophical See also:faculty of the University, and this he succeeded in winning with the See also:paper which was published in 188o on the " Kinetic See also:Energy of See also:Electricity in See also:Motion." His next investigation, on " See also:Induction in Rotating See also:Spheres," he offered in 188o as his dissertation for his See also:doctor's degree, which he obtained with the rare distinction of summa cum laude. Later in the same See also:year he became assistant to Helmholtz in the physical laboratory of the Berlin See also:Institute. During the three years he held this position he carried out researches on the contact of elastic solids, hardness, evaporation and the electric See also:discharge in gases, the last earning him the See also:special See also:commendation of Helmholtz.

In 1883 he went to See also:

Kiel, becoming PrivatdozQnt, and there he began the studies in See also:Maxwell's electro-magnetic theory which a few years later resulted in the discoveries that rendered his name famous. These were actually made between 1885 and 1889, when he was See also:professor of physics in the Carlsruhe See also:Polytechnic. He himself recorded that their origin is to be sought in a prize problem proposed by the Berlin See also:Academy of Sciences in 1879, having reference to the experimental See also:establishment of some relation between electromagnetic forces and the See also:dielectric polarization of insulators. Imagining that this would See also:interest Hertz and be successfully attacked by him, Helmholtz specially See also:drew his See also:attention to it, and promised him the assistance of the Institute if he decided to See also:work on the subject; but Hertz did not take it up seriously at that See also:time, because he could not think of any See also:procedure likely to prove effective. It was of course well known, as a See also:necessity of Maxwell's mathematical theory, that the polarization and depolarization of an insulator must give rise to the same electromagnetic effects in the neighbourhood as a voltaic current in a conductor. The ex perimental See also:proof, however, was still lacking, and though several experimenters had come very near its See also:discovery, Hertz was the first who actually succeeded in supplying it, in 1887. Continuing his inquiries for the next year or two, he was able to discover the progressive See also:propagation of electromagnetic See also:action through space, to measure the length and velocity of electromagnetic waves, and to show that in the transverse nature of their vibration and their susceptibility to reflection, See also:refraction and polarization they are in See also:complete See also:correspondence with the waves of See also:light and See also:heat. The result, was in Helmholtz's words, to establish beyond doubt that See also:ordinary light consists of See also:electrical vibrations in an all-pervading See also:ether which possesses the properties of an insulator and of a magnetic See also:medium. Hertz himself gave an admirable See also:account of the significance of his discoveries in a lecture on the relations between light and electricity, delivered before the German Society for the See also:Advancement of Natural Science and See also:Medicine at See also:Heidelberg in See also:September 1889. Since the time of these See also:early experiments, various other modes of detecting the existence of electric waves have been found out in addition to the spark-See also:gap which he first employed, and the results of his observations, the earliest interest of which was simply that they afforded a See also:confirmation of an abstruse mathematical theory, have been applied to the practical purposes of signalling over considerable distances (see TELEGRAPHY, WIRELESS). In 1889 Hertz was appointed to succeed R. J.

E. See also:

Clausius as ordinary professor of physics in the university of See also:Bonn. There he continued his researches on the discharge of electricity in rarefied gases,. only just missing the discovery of the X-rays described by W. C. See also:Rontgen a few years later, and produced his See also:treatise on the Principles of Mechanics. This was his last work, for after a See also:long illness he died at Bonn on the 1st of See also:January 1894. By his premature See also:death science lost one of her most promising disciples. Helmholtz thought him the one of all his pupils who had penetrated farthest into his own circle of scientific thought, and looked to him with the greatest confidence for the further See also:extension and development of his work. Hertz's scientific papers were translated into See also:English by Professor D. E. See also:Jones, and published in three volumes: Electric Waves (1893), . See also:Miscellaneous Papers (1896), and Principles of Mechanics (1899).

The See also:

preface contributed to the first of these by See also:Lord See also:Kelvin, and the introductions to the second and third by Professors P. E. A. Lenard and Helmholtz, contain many See also:biographical details, together with statements of the See also:scope and significance of his investigations.

End of Article: HERTZ, HEINRICH RUDOLF (1857-1894)

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