{"title":"G的新测定","authors":"J. Faller, J. Schwarz, T. Niebauer, D. Robertson","doi":"10.1109/CPEM.1998.699825","DOIUrl":null,"url":null,"abstract":"A determination of G, the Newtonian constant of gravitation, has been made utilizing a new free-fall method. Traditionally this determination has been made using a torsion fiber which (functionally) eliminates g (the acceleration due to gravity) from the measurement process. In this determination, we explicitly use g to measure G. We do this by measuring the effect a large, yet moveable, mass has on the measured value of g. In this determination we use a FG-5 absolute gravimeter to measure g. This commercial instrument uses time-resolved interferometry of a freely falling \"mirror\" to determine g with a measurement accuracy approaching 1 part in 10/sup 9/. Together with the FG-5, we use a large and finely moveable mass which surrounds the dropping region. On twenty-minute intervals this mass is moved between positions just above and just below this region. As a result, the measured value of g is square-wave modulated with a peak-to-peak amplitude of approximately 80 parts in 10/sup 9/. This precisely measured difference together with a straightforward, though numerically involved, analysis of the effects of the mass in the two positions on the measured value of g determine G.","PeriodicalId":239228,"journal":{"name":"1998 Conference on Precision Electromagnetic Measurements Digest (Cat. No.98CH36254)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-07-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"A new determination of G\",\"authors\":\"J. Faller, J. Schwarz, T. Niebauer, D. Robertson\",\"doi\":\"10.1109/CPEM.1998.699825\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A determination of G, the Newtonian constant of gravitation, has been made utilizing a new free-fall method. Traditionally this determination has been made using a torsion fiber which (functionally) eliminates g (the acceleration due to gravity) from the measurement process. In this determination, we explicitly use g to measure G. We do this by measuring the effect a large, yet moveable, mass has on the measured value of g. In this determination we use a FG-5 absolute gravimeter to measure g. This commercial instrument uses time-resolved interferometry of a freely falling \\\"mirror\\\" to determine g with a measurement accuracy approaching 1 part in 10/sup 9/. Together with the FG-5, we use a large and finely moveable mass which surrounds the dropping region. On twenty-minute intervals this mass is moved between positions just above and just below this region. As a result, the measured value of g is square-wave modulated with a peak-to-peak amplitude of approximately 80 parts in 10/sup 9/. This precisely measured difference together with a straightforward, though numerically involved, analysis of the effects of the mass in the two positions on the measured value of g determine G.\",\"PeriodicalId\":239228,\"journal\":{\"name\":\"1998 Conference on Precision Electromagnetic Measurements Digest (Cat. No.98CH36254)\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-07-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1998 Conference on Precision Electromagnetic Measurements Digest (Cat. No.98CH36254)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CPEM.1998.699825\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 Conference on Precision Electromagnetic Measurements Digest (Cat. No.98CH36254)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CPEM.1998.699825","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A determination of G, the Newtonian constant of gravitation, has been made utilizing a new free-fall method. Traditionally this determination has been made using a torsion fiber which (functionally) eliminates g (the acceleration due to gravity) from the measurement process. In this determination, we explicitly use g to measure G. We do this by measuring the effect a large, yet moveable, mass has on the measured value of g. In this determination we use a FG-5 absolute gravimeter to measure g. This commercial instrument uses time-resolved interferometry of a freely falling "mirror" to determine g with a measurement accuracy approaching 1 part in 10/sup 9/. Together with the FG-5, we use a large and finely moveable mass which surrounds the dropping region. On twenty-minute intervals this mass is moved between positions just above and just below this region. As a result, the measured value of g is square-wave modulated with a peak-to-peak amplitude of approximately 80 parts in 10/sup 9/. This precisely measured difference together with a straightforward, though numerically involved, analysis of the effects of the mass in the two positions on the measured value of g determine G.