{"title":"麦克斯韦场方程是伽利略协变的所有运动参照系","authors":"A. Potjekhin","doi":"10.1109/MMET.2008.4580959","DOIUrl":null,"url":null,"abstract":"The concepts of dynamical and kinematical reference systems by Newton are introduced. The Maxwell field equations in the kinematical non-accelerated (in relation to the inertial) reference systems are derived. It is shown, that Maxwell equations, written in the inertial reference system, are not covariant relative to the transformation of Galileo. But these equations are Galileo-covariant relative for all kinematical reference systems.","PeriodicalId":141554,"journal":{"name":"2008 12th International Conference on Mathematical Methods in Electromagnetic Theory","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Maxwell field equations are Galileo covariant for all kinematic refrence systems\",\"authors\":\"A. Potjekhin\",\"doi\":\"10.1109/MMET.2008.4580959\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The concepts of dynamical and kinematical reference systems by Newton are introduced. The Maxwell field equations in the kinematical non-accelerated (in relation to the inertial) reference systems are derived. It is shown, that Maxwell equations, written in the inertial reference system, are not covariant relative to the transformation of Galileo. But these equations are Galileo-covariant relative for all kinematical reference systems.\",\"PeriodicalId\":141554,\"journal\":{\"name\":\"2008 12th International Conference on Mathematical Methods in Electromagnetic Theory\",\"volume\":\"17 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-07-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 12th International Conference on Mathematical Methods in Electromagnetic Theory\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/MMET.2008.4580959\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 12th International Conference on Mathematical Methods in Electromagnetic Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/MMET.2008.4580959","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Maxwell field equations are Galileo covariant for all kinematic refrence systems
The concepts of dynamical and kinematical reference systems by Newton are introduced. The Maxwell field equations in the kinematical non-accelerated (in relation to the inertial) reference systems are derived. It is shown, that Maxwell equations, written in the inertial reference system, are not covariant relative to the transformation of Galileo. But these equations are Galileo-covariant relative for all kinematical reference systems.