Difference between revisions of "A Formulation of Galilean Gravitation on a Maniford"
Jump to navigation
Jump to search
(Imported from text file) |
(Imported from text file) |
||
Line 12: | Line 12: | ||
==Abstract== | ==Abstract== | ||
− | This paper, which follows [1], presents the formal structure of a Galilean theory of gravitation which is "maximally simple," in the sense of it being impossible to formulate a Galilean invariant theory making<em> </em>fewer<em> a priori </em>statements about the world; specifically, the conservation of linear momentum is assumed, and gravitational trajectories are assumed to be those trajectories which are independent of measured mass properties. [[Category:Scientific Paper]] | + | This paper, which follows [1], presents the formal structure of a Galilean theory of gravitation which is "maximally simple," in the sense of it being impossible to formulate a Galilean invariant theory making<em> </em>fewer<em> a priori </em>statements about the world; specifically, the conservation of linear momentum is assumed, and gravitational trajectories are assumed to be those trajectories which are independent of measured mass properties. |
+ | |||
+ | [[Category:Scientific Paper|formulation galilean gravitation maniford]] | ||
[[Category:Gravity]] | [[Category:Gravity]] |
Revision as of 09:55, 1 January 2017
Scientific Paper | |
---|---|
Title | A Formulation of Galilean Gravitation on a Maniford |
Author(s) | David F Roscoe |
Keywords | Galilean theory, gravitation, linear momentum |
Published | 1993 |
Journal | Galilean Electrodynamics |
Volume | 4 |
Number | 2 |
Pages | 32-34 |
Abstract
This paper, which follows [1], presents the formal structure of a Galilean theory of gravitation which is "maximally simple," in the sense of it being impossible to formulate a Galilean invariant theory making fewer a priori statements about the world; specifically, the conservation of linear momentum is assumed, and gravitational trajectories are assumed to be those trajectories which are independent of measured mass properties.