934:; This article ends with the announcement that in a forthcoming article the principles worked out so far shall be applied to the problems of reflection and refraction. The article contains on p. 235, last paragraph, and on p. 236, 2nd paragraph, a judgment on the Michelson experiment of 1886, which Voigt, after a correspondence with H. A. Lorentz in 1887 and 1888, has partly withdrawn in the article announced, namely in a footnote in Voigt (1888). According to Voigt's first judgment, the Michelson experiment must yield a null result, independently of whether the Earth transports the luminiferous aether with it (Fizeau's 1st aether hypothesis), or whether the Earth moves through an entirely independent, self-consistent universal
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702:(1909) is on record as saying that he could have taken these transformations into his theory of electrodynamics, if only he had known of them, rather than developing his own. It is interesting then to examine the consequences of these transformations from this point of view. Lorentz might then have seen that the transformation introduced
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No. 8, p. 235 and p. 236 (1887), and states indirectly that, after a correspondence with H. A. Lorentz, he can no longer maintain that in the case of the validity of Fizeau's 2nd aether hypothesis the
Michelson experiment must yield a null result
890:"Wir wollen uns deshalb nur darauf stĂŒtzen, dass ZustĂ€nde der geschilderten Art bei Spannungen und Dehnungen nicht starrer Körper auftreten, und sie deshalb tensorielle, die fĂŒr sie charakteristischen physikalischen Grössen aber Tensoren nennen."
789:
892:(We therefore want to be based only on conditions of the type described occur during stresses and strains of non-rigid bodies, and therefore call them "tensorial" but call the characteristic physical quantities for them "tensors".)
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are named after him. He was also an amateur musician and became known as a Bach expert (see
External links). He was the first to suggest, in 1886, that Bach's
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direction. However, as Voigt himself said, the transformation was aimed at a specific problem and did not carry with it the idea of a general
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can not distinguish between the two transformations. The crucial question is the issue of time dilation. The experimental measurement of
698:
said in 1908 that the transformations which play the main role in the principle of relativity were first examined by Voigt in 1887. Also
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Bucherer, A. H. (1908), "Messungen an
Becquerelstrahlen. Die experimentelle BestÀtigung der Lorentz-Einsteinschen Theorie",
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and eventually went on to head the
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784:{\displaystyle \Delta t_{\text{Voigt}}=\gamma ^{-2}\Delta t=\gamma ^{-1}\Delta t_{\text{Lorentz}}}
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Electromagnetic phenomena in a system moving with any velocity smaller than that of light
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Die fundamentalen physikalischen
Eigenschaften der Krystalle in elementarer Darstellung
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Physics as a
Calling: Discipline and Practice in the Königsberg Seminar for Physics
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Voigt, W. (1887), "Ueber das
Doppler'sche Princip (On the Principle of Doppler)",
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Since Voigt's transformation preserves the speed of light in all frames, the
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between a rest frame of reference and a frame moving with speed
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First
Proposal of the Universal Speed of Light by Voigt in 1887
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in its current meaning was introduced by him in 1898.
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339:Concerto for two harpsichords in C minor, BWV 1060
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663:{\displaystyle \gamma =1/{\sqrt {1-v^{2}/c^{2}}}}
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1052:Ernst, Andreas & Hsu Jong-Ping (June 2001);
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1145:Academic staff of the University of Königsberg
410:In modern notation Voigt's transformation was
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341:was originally scored for violin and oboe.
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19:For the German aerospace engineer, see
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1021:"A Note on Relativity Before Einstein"
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938:(Fizeau's 2nd aether hypothesis).
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1120:19th-century German physicists
594:{\displaystyle t'=t-vx/c^{2},}
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535:{\displaystyle z'=z/\gamma ,}
492:{\displaystyle y'=y/\gamma ,}
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16:German physicist (1850â1919)
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1060:Chinese Journal of Physics
871:, Cornell University Press
867:Olesko, Kahryn M. (1991),
704:relativity of simultaneity
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18:
1135:Leipzig University alumni
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954:(10): 370â396, 524â551,
807:{\displaystyle \Delta t}
449:{\displaystyle x'=x-vt,}
313:. His main work was the
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285:Franz Ernst Neumann
222:Franz Ernst Neumann
162:DyakonovâVoigt wave
1002:; See p. 198.
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1115:1919 deaths
1110:1850 births
706:, and also
293:Peter Debye
137:Voigt model
97:Nationality
1104:Categories
906:(7): 41â51
849:References
232:Paul Drude
56:1850-09-02
1033:CiteSeerX
799:Δ
769:Δ
761:−
757:γ
747:Δ
739:−
735:γ
718:Δ
678:γ
631:−
612:γ
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527:γ
484:γ
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281:Göttingen
271:Biography
265:physicist
200:Physicist
86:Göttingen
837:See also
821:and the
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512:′
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180:ForMemRS
1083:at the
1074:at the
956:Bibcode
777:Lorentz
368:in the
303:physics
300:crystal
277:Leipzig
248:German:
90:Germany
64:Leipzig
1058:, pdf
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604:where
327:tensor
196:Fields
183:(1913)
176:Awards
100:German
726:Voigt
976:too.
333:and
309:and
75:Died
50:Born
1043:doi
964:doi
913:XVI
829:by
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1045::
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615:=
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575:/
571:x
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552:t
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523:/
519:z
516:=
509:z
487:,
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476:y
473:=
466:y
444:,
441:t
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432:x
429:=
422:x
376:x
356:v
317:(
246:(
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54:(
23:.
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