{"title":"暗能量问题的解决方案","authors":"Donald Aucamp Sc.D","doi":"10.22259/2637-5826.0401001","DOIUrl":null,"url":null,"abstract":"REVIEW OF LAW L1 AND COROLLARY C1 Review of Law L1 and Corollary C1 In Aucamp [5] a gravitational law L1 is proposed which tweaks Newton’s Law of Gravity (NLG) in an insignificant way. The theory examines the force exerted by a gravity “ray” sent at t by a moving body of mass M and subsequently received by a moving body of mass m. In the analysis IFR(t) is defined as the inertial frame of reference of M at the ray emission time t. The term, “ray”, is used here to indicate the gravitational field emitted over an infinitesimal period of time. The following assumptions are made:","PeriodicalId":333499,"journal":{"name":"Open Access Journal of Physics","volume":"35 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Solution to the Dark Energy Problem\",\"authors\":\"Donald Aucamp Sc.D\",\"doi\":\"10.22259/2637-5826.0401001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"REVIEW OF LAW L1 AND COROLLARY C1 Review of Law L1 and Corollary C1 In Aucamp [5] a gravitational law L1 is proposed which tweaks Newton’s Law of Gravity (NLG) in an insignificant way. The theory examines the force exerted by a gravity “ray” sent at t by a moving body of mass M and subsequently received by a moving body of mass m. In the analysis IFR(t) is defined as the inertial frame of reference of M at the ray emission time t. The term, “ray”, is used here to indicate the gravitational field emitted over an infinitesimal period of time. The following assumptions are made:\",\"PeriodicalId\":333499,\"journal\":{\"name\":\"Open Access Journal of Physics\",\"volume\":\"35 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Open Access Journal of Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.22259/2637-5826.0401001\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Open Access Journal of Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22259/2637-5826.0401001","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
REVIEW OF LAW L1 AND COROLLARY C1 Review of Law L1 and Corollary C1 In Aucamp [5] a gravitational law L1 is proposed which tweaks Newton’s Law of Gravity (NLG) in an insignificant way. The theory examines the force exerted by a gravity “ray” sent at t by a moving body of mass M and subsequently received by a moving body of mass m. In the analysis IFR(t) is defined as the inertial frame of reference of M at the ray emission time t. The term, “ray”, is used here to indicate the gravitational field emitted over an infinitesimal period of time. The following assumptions are made:
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