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PHILIPP LENARD
Philipp_Lenard

Philipp Lenard in 1905 |
| Born |
June 7, 1862
Pressburg, Hungary |
| Died |
May 20, 1947
Messelhausen, Germany |
| Residence |
Germany |
| Nationality |
Hungarian before 1907, then German |
| Field |
Physicist |
| Institution |
University of Breslau, University of Aachen, University of Heidelberg, University of Kiel |
| Alma Mater |
University of Heidelberg |
| Doctoral Advisor |
Robert Bunsen |
| Doctoral Students |
<please insert> |
| Known for |
Cathode rays (electron beams) |
| Prizes |
Matteucci Medal (1896), Nobel Prize for Physics (1905), Rumford Medal (1896) |
Philipp Eduard Anton von Lenard, (Hungarian: Lénárd Fülöp) (June 7, 1862–May 20, 1947) was a physicist and the winner of the Nobel Prize for Physics in 1905 for his research on cathode rays and the discovery of many of their properties.
Biography
Philipp Lenard was born in Bratislava (then as Pressburg part of the Austro-Hungarian Empire) on July 7, 1862, and he attended a Hungarian-language secondary school. He studied under the illustrious Bunsen and Helmholtz, and obtained his doctoral degree in 1886 at the University of Heidelberg. He was certainly a Hungarian citizen as of 1897 (when the Hungarian Academy of Sciences elected him to be a corresponding member) but he resigned his nationality probably before 1907. ([1]) After posts at Aachen, Bonn, Breslau, Heidelberg (1896-1898), and Kiel (1898-1907), he returned finally to the University of Heidelberg in 1907 as the head of the Philipp Lenard Institute.
As a physicist, Lenard's major contributions were in the study of cathode rays. Prior to his work, cathode rays were produced in primitive tubes which are partially evacuated glass tubes that have metallic electrodes in them, across which a high voltage can be placed.
Photoelectric investigation
The cathode rays were difficult to study because they were inside sealed glass tubes, difficult to access, and because the rays were in the presence of air molecules (fully evacuated tubes didn't produce rays). Lenard overcame these problems by devising a method of making small metallic windows in the glass that were thick enough to be able to withstand the pressure differences, but thin enough to allow passage of the rays. Having made a window for the rays, he could pass them out into the laboratory, or, alternatively, into another chamber that was completely evacuated. He was able to conveniently detect the rays and measure their intensity by means of paper sheets coated with phosphorescent materials.
As a result of his Crookes tube investigations, he showed that the rays produced by radiating metals in a vacuum with ultraviolet light were similar in many respects to cathode rays. His most important observations were that the energy of the rays was independent of the light intensity, but was greater for shorter wavelengths of light.
Another observation that Lenard made was that the absorption of the rays was, to first order, proportional to the density of the material they were made to pass through. This appeared to contradict the idea that they were some sort of electromagnetic radiation. He also showed that the rays could pass through some inches of air of a normal density, and appeared to be scattered by it, implying that they must be particles that were even smaller than the molecules in air. He confirmed some of J.J. Thomson's work, which ultimately arrived at the understanding that cathode rays were streams of energetic electrons.
These observations were explained by Albert Einstein as a quantum effect. This theory predicted that the plot of the cathode ray energy versus the frequency would be a straight line with a slope equal to Planck's constant, h. This was shown to be the case some years later. The photo-electric quantum theory was the work cited when Einstein was awarded the Nobel Prize in Physics. This much embittered Lenard, who became a prominent skeptic of relativity and of Einstein's theories generally. Ironically, Einstein never really accepted quantum mechanics, and was its most prominent critic.
Later Years and Legacy
Lenard is most remembered today as a strong German nationalist who despised English physics, which he considered as having stolen their ideas from Germany. He joined the National Socialist Party before it became politically necessary or popular to do so. During the Nazi regime, he was the outspoken proponent of the idea that Germany should rely on "Deutsche Physik" ("German physics") and ignore the (in his opinion) fallacious and perhaps deliberately misleading ideas of "Jewish physics", by which he meant chiefly the theories of Albert Einstein, including "the Jewish fraud" of relativity. An advisor to Adolf Hitler, Lenard became Chief of Aryan Physics under the Nazis.
Lenard retired from Heidelberg Univerisity as professor of theoretical physics in 1931. He achieved emeritus status there, but he was expelled from his post by Allied occupation forces in 1945. He died two years later in Messelhausen.
Honors
External links
Books by Philipp Lenard
- Ueber Aether und Materie (second edition 1911)
- Quantitatives über Kathodenstrahlen (1918)
- Ueber das Relativitätsprinzip (1918)
- Grosse Naturforscher (second edition 1930)
- Deutsche Physik (1936-37, physics, 4 vols.)
- Lenard, Philipp, Great Men of Science. Translated from the second German edition, G. Bell and sons, London (1950) ISBN 083691614X
References
- Beyerchen, Alan, Scientists under Hitler: Politics and the physics community in the Third Reich (New Haven, CT: Yale University Press, 1977).
- Hentschel, Klaus, ed. Physics and National Socialism: An anthology of primary sources (Basel: Birkhaeuser, 1996).
- Walker, Mark, Nazi science: Myth, truth, and the German atomic bomb (New York: Harper Collins, 1995).
- Wolff, Stephan L., "Physicists in the 'Krieg der Geister': Wilhelm Wien's 'Proclamation'", Historical Studies in the Physical and Biological Sciences Vol. 33, No. 2 (2003): 337-368.
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1901: Röntgen 02: Lorentz, Zeeman 03: Becquerel, P.Curie, M.Curie 04: Rayleigh 05: Lenard 06: Thomson 07: Michelson 08: Lippmann 09: Marconi, Braun 10: van der Waals 11: Wien 12: Dalén 13: Kamerlingh Onnes 14: von Laue 15: Bragg 17: Barkla 18: Planck 19: Stark 20: Guillaume 21: Einstein 22: N.Bohr 23: Millikan 24: Siegbahn 25: Franck, Hertz 26: Perrin 27: Compton, Wilson 28: Richardson 29: de Broglie 30: Raman 32: Heisenberg 33: Schrödinger, Dirac 35: Chadwick 36: Hess, Anderson 37: Davisson, Thomson 38: Fermi 39: Lawrence 43: Stern 44: Rabi 45: Pauli 46: Bridgman 47: Appleton 48: Blackett 49: Yukawa 50: Powell 51: Cockcroft, Walton 52: Bloch, Purcell 53: Zernike 54: Born, Bothe 55: Lamb, Kusch 56: Shockley, Bardeen, Brattain 57: Yang, T.D.Lee 58: Cherenkov, Frank, Tamm 59: Segrè, Chamberlain 60: Glaser 61: Hofstadter, Mössbauer 62: Landau 63: Wigner, Goeppert‑Mayer, Jensen 64: Townes, Basov, Prokhorov 65: Tomonaga, Schwinger, Feynman 66: Kastler 67: Bethe 68: Alvarez 69: Gell‑Mann 70: Alfvén, Néel 71: Gabor 72: Bardeen, Cooper, Schrieffer 73: Esaki, Giaever, Josephson 74: Ryle, Hewish 75: A.Bohr, Mottelson, Rainwater 76: Richter, Ting 77: Anderson, Mott, van Vleck 78: Kapitsa, Penzias, Wilson 79: Glashow, Salam, Weinberg 80: Cronin, Fitch 81: Bloembergen, Schawlow, Siegbahn 82: Wilson 83: Chandrasekhar, Fowler 84: Carlo Rubbia, van der Meer 85: von Klitzing 86: Ruska, Binnig, Rohrer 87: Bednorz, Müller 88: Lederman, Schwartz, Steinberger 89: Ramsey, Dehmelt, Paul 90: Friedman, Kendall, Taylor 91: de Gennes 92: Charpak 93: Hulse, Taylor 94: Brockhouse, Shull 95: Perl, Reines 96: D.Lee, Osheroff, Richardson 97: Chu, Cohen‑Tannoudji, Phillips 98: Laughlin, Störmer, Tsui 99: 't Hooft, Veltman 2000: Alferov, Kroemer, Kilby 01: Cornell, Ketterle, Wieman 02: Davis, Koshiba, Giacconi 03: Abrikosov, Ginzburg, Leggett 04: Gross, Politzer, Wilczek 05: Glauber, Hall, Hänsch
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