Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 220
... transformation equations , where ( 4.29 ) v T = ( 1- v2 / w2 ) −ł . We shall now show that causality implies that ... transformation must be Galilean . อ If in ( 4.28 ) we set w = c , we obtain the ordinary Lorentz transformation ( 4.32 ) ...
... transformation equations , where ( 4.29 ) v T = ( 1- v2 / w2 ) −ł . We shall now show that causality implies that ... transformation must be Galilean . อ If in ( 4.28 ) we set w = c , we obtain the ordinary Lorentz transformation ( 4.32 ) ...
Page 226
... transformations only the Lorentz transformations leave the Maxwell equations covariant . A modern version of Frank's demonstration may be based on a paper by K. STIEGLER [ 50 ] , who derived the Lorentz transformation from the Maxwell ...
... transformations only the Lorentz transformations leave the Maxwell equations covariant . A modern version of Frank's demonstration may be based on a paper by K. STIEGLER [ 50 ] , who derived the Lorentz transformation from the Maxwell ...
Page 227
... transformation equations . Let us now discuss a problem connected with the consequences of these transformation equations . First of all , it is clear that these conclusions themselves must also be consistent among each other , for ...
... transformation equations . Let us now discuss a problem connected with the consequences of these transformation equations . First of all , it is clear that these conclusions themselves must also be consistent among each other , for ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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