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Woldemar Voigt

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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the Michelson experiment of 1886, which Voigt, after a correspondence with H. A. Lorentz in 1887 and 1888, has partly withdrawn in the article announced, namely in a footnote in Voigt (1888).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 257: 40: 1071: 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 975:
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".) 258: 668: 710:. However, the magnitude of the dilation was greater than the now accepted value in the Lorentz transformations. Moving clocks, obeying Voigt's time transformation, indicate an elapsed time 599: 540: 497: 454: 713: 812: 1144: 688: 1149: 386: 366: 337:
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
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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 Mathematical Physics Department there. He was succeeded in 1914 by
209: 389: 166: 20: 1037: 546: 503: 460: 251: 784:{\displaystyle \Delta t_{\text{Voigt}}=\gamma ^{-2}\Delta t=\gamma ^{-1}\Delta t_{\text{Lorentz}}} 161: 1032: 691: 345: 794: 416: 971:; In a footnote on p. 390 of this article, Voigt corrects his earlier judgment, made in 673: 1114: 1109: 955: 8: 1007:
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
707: 330: 146: 1080: 1046: 833:(1938) and others settled the issue in favor of the Lorentz transformation. 322: 295:, who took charge of the theoretical department of the Physical Institute. 131: 280: 85: 39: 292: 231: 264: 199: 943: 321:), first published in 1910. He discovered what is now called the 302: 299: 276: 63: 348:
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.
797: 716: 676: 610: 549: 506: 463: 419: 374: 354: 263:; 2 September 1850 – 13 December 1919) was a German 791:, while stationary clocks indicate an elapsed time 806: 783: 682: 662: 593: 534: 491: 448: 380: 360: 339:Concerto for two harpsichords in C minor, BWV 1060 908:; Reprinted with additional comments by Voigt in 885:(Leipzig, Germany: Veit & Co., 1898), p. 20. 866: 663:{\displaystyle \gamma =1/{\sqrt {1-v^{2}/c^{2}}}} 1101: 1052:Ernst, Andreas & Hsu Jong-Ping (June 2001); 1018: 979: 1145:Academic staff of the University of Königsberg 410:In modern notation Voigt's transformation was 1150:Academic staff of the University of Göttingen 993: 990:; For Minkowski's statement see p. 762. 341:was originally scored for violin and oboe. 38: 1036: 941: 923: 901: 944:"Theorie des Lichts fĂŒr bewegte Medien" 926:"Theorie des Lichts fĂŒr bewegte Medien" 875: 399: 344:In 1887 Voigt formulated a form of the 19:For the German aerospace engineer, see 1102: 1021:"A Note on Relativity Before Einstein" 895: 1130:Scientists from the Kingdom of Saxony 860: 250: 1155:Foreign members of the Royal Society 1000:, Leipzig & Berlin: B.G. Teubner 289:Georg August University of Göttingen 1090:The relativity of light (MathPages) 13: 798: 768: 746: 717: 406:History of Lorentz transformations 14: 1171: 1065: 938:(Fizeau's 2nd aether hypothesis). 1072:Works by or about Woldemar Voigt 843:German inventors and discoverers 1140:University of Königsberg alumni 1160:20th-century German physicists 1120:19th-century German physicists 594:{\displaystyle t'=t-vx/c^{2},} 1: 1085:Mathematics Genealogy Project 848: 535:{\displaystyle z'=z/\gamma ,} 492:{\displaystyle y'=y/\gamma ,} 823:Kennedy–Thorndike experiment 270: 16:German physicist (1850–1919) 7: 836: 819:Michelson–Morley experiment 319:Textbook on crystal physics 315:Lehrbuch der Kristallphysik 10: 1176: 1095:Bach expert Woldemar Voigt 1060:Chinese Journal of Physics 871:, Cornell University Press 867:Olesko, Kahryn M. (1991), 704:relativity of simultaneity 403: 18: 1135:Leipzig University alumni 1019:Macrossan, M. N. (1986), 982:Physikalische Zeitschrift 910:Physikalische Zeitschrift 690:, they become the modern 390:coordinate transformation 237: 227: 215: 205: 195: 188: 175: 114: 104: 96: 74: 49: 37: 30: 21:Woldemar Voigt (engineer) 968:10.1002/andp.18882711011 954:(10): 370–396, 524–551, 807:{\displaystyle \Delta t} 449:{\displaystyle x'=x-vt,} 313:. His main work was the 109:University of Königsberg 1125:Scientists from Leipzig 997:The theory of electrons 683:{\displaystyle \gamma } 210:University of Göttingen 44:Woldemar Voigt, c. 1908 808: 785: 692:Lorentz transformation 684: 664: 595: 536: 493: 450: 382: 362: 346:Lorentz transformation 287:. Voigt taught at the 283:. He was a student of 1047:10.1093/bjps/37.2.232 994:Lorentz, H.A (1916), 973:Göttinger Nachrichten 930:Göttinger Nachrichten 904:Göttinger Nachrichten 809: 786: 685: 665: 596: 537: 494: 451: 404:Further information: 383: 363: 167:Kelvin–Voigt material 795: 714: 674: 608: 547: 504: 461: 417: 400:Voigt transformation 392:, as is the case in 372: 352: 152:Voigt transformation 1025:Br. J. Philos. Sci. 960:1888AnP...271..370V 936:luminiferous aether 285:Franz Ernst Neumann 222:Franz Ernst Neumann 162:Dyakonov–Voigt wave 1002:; See p. 198. 948:Annalen der Physik 942:Voigt, W. (1888), 924:Voigt, W. (1887), 831:Ives and Stillwell 804: 781: 680: 660: 591: 532: 489: 446: 378: 358: 325:in 1898. The word 275:Voigt was born in 1013:Secondary sources 915:, 381–386 (1915). 778: 727: 696:Hermann Minkowski 658: 394:relativity theory 381:{\displaystyle x} 361:{\displaystyle v} 241: 240: 228:Doctoral students 190:Scientific career 157:Voigt–Thomson law 68:Kingdom of Saxony 1167: 1076:Internet Archive 1049: 1040: 1001: 989: 970: 933: 916: 907: 899: 893: 881:Woldemar Voigt, 879: 873: 872: 864: 813: 811: 810: 805: 790: 788: 787: 782: 780: 779: 776: 767: 766: 745: 744: 729: 728: 725: 689: 687: 686: 681: 669: 667: 666: 661: 659: 657: 656: 647: 642: 641: 626: 624: 600: 598: 597: 592: 587: 586: 577: 557: 541: 539: 538: 533: 525: 514: 498: 496: 495: 490: 482: 471: 455: 453: 452: 447: 427: 387: 385: 384: 379: 367: 365: 364: 359: 298:Voigt worked on 262: 261: 260: 254: 249: 217:Doctoral advisor 184: 122:Piezoelectricity 81: 78:13 December 1919 60:2 September 1850 59: 57: 42: 28: 27: 1175: 1174: 1170: 1169: 1168: 1166: 1165: 1164: 1100: 1099: 1068: 1038:10.1.1.679.5898 920: 919: 900: 896: 880: 876: 865: 861: 854:Primary Sources 851: 839: 796: 793: 792: 775: 771: 759: 755: 737: 733: 724: 720: 715: 712: 711: 700:Hendrik Lorentz 675: 672: 671: 652: 648: 643: 637: 633: 625: 620: 609: 606: 605: 582: 578: 573: 550: 548: 545: 544: 521: 507: 505: 502: 501: 478: 464: 462: 459: 458: 420: 418: 415: 414: 408: 402: 373: 370: 369: 353: 350: 349: 273: 256: 255: 252:[foːkt] 247: 182: 171: 127:Pyroelectricity 105:Alma mater 92: 83: 79: 70: 61: 55: 53: 45: 33: 24: 17: 12: 11: 5: 1173: 1163: 1162: 1157: 1152: 1147: 1142: 1137: 1132: 1127: 1122: 1117: 1112: 1098: 1097: 1092: 1087: 1081:Woldemar Voigt 1078: 1067: 1066:External links 1064: 1063: 1062: 1050: 1031:(2): 232–234, 1015: 1014: 1010: 1009: 1005:Lorentz 1904, 1003: 991: 977: 939: 918: 917: 894: 874: 858: 857: 856: 855: 850: 847: 846: 845: 838: 835: 803: 800: 774: 770: 765: 762: 758: 754: 751: 748: 743: 740: 736: 732: 723: 719: 679: 655: 651: 646: 640: 636: 632: 629: 623: 619: 616: 613: 602: 601: 590: 585: 581: 576: 572: 569: 566: 563: 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949: 945: 940: 937: 931: 927: 922: 921: 914: 911: 905: 898: 891: 888: 887:From page 20: 884: 878: 870: 863: 859: 853: 852: 844: 841: 840: 834: 832: 828: 827:time dilation 824: 820: 815: 801: 772: 763: 760: 756: 752: 749: 741: 738: 734: 730: 721: 709: 708:time dilation 705: 701: 697: 693: 677: 653: 649: 644: 638: 634: 630: 627: 621: 617: 614: 611: 588: 583: 579: 574: 570: 567: 564: 561: 558: 554: 551: 543: 529: 526: 522: 518: 515: 511: 508: 500: 486: 483: 479: 475: 472: 468: 465: 457: 443: 440: 437: 434: 431: 428: 424: 421: 413: 412: 411: 407: 397: 395: 391: 375: 355: 347: 342: 340: 336: 332: 331:Voigt profile 328: 324: 320: 316: 312: 308: 304: 301: 296: 294: 290: 286: 282: 278: 268: 266: 259: 253: 245: 236: 233: 230: 226: 223: 220: 218: 214: 211: 208: 204: 201: 198: 194: 191: 187: 181: 178: 174: 168: 165: 163: 160: 158: 155: 153: 150: 148: 147:Voigt profile 145: 143: 140: 138: 135: 133: 130: 128: 125: 123: 120: 119: 117: 113: 110: 107: 103: 99: 95: 91: 87: 77: 73: 69: 65: 52: 48: 41: 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962:, 952:35 950:, 946:, 928:, 814:. 694:. 396:. 305:, 267:. 88:, 66:, 1045:: 986:9 966:: 958:: 802:t 773:t 764:1 753:= 750:t 742:2 731:= 722:t 654:2 650:c 645:/ 639:2 635:v 628:1 622:/ 618:1 615:= 589:, 584:2 580:c 575:/ 571:x 568:v 562:t 559:= 552:t 530:, 523:/ 519:z 516:= 509:z 487:, 480:/ 476:y 473:= 466:y 444:, 441:t 438:v 432:x 429:= 422:x 376:x 356:v 317:( 246:( 58:) 54:( 23:.

Index

Woldemar Voigt (engineer)

Leipzig
Kingdom of Saxony
Göttingen
Germany
University of Königsberg
Piezoelectricity
Pyroelectricity
Voigt effect
Voigt model
Voigt notation
Voigt profile
Voigt transformation
Voigt–Thomson law
Dyakonov–Voigt wave
Kelvin–Voigt material
ForMemRS
Physicist
University of Göttingen
Doctoral advisor
Franz Ernst Neumann
Paul Drude
[foːkt]

physicist
Leipzig
Göttingen
Franz Ernst Neumann
Georg August University of Göttingen

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