Difference between revisions of "Pedagogy: The Bubble Analogy and the Difference Between Gravitational Forces and Rocket Thrust in Spatial Flow Theories of Gravity"
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==Abstract== | ==Abstract== | ||
− | We present a physical analogy which can be used to understand the issues involved in the Principle of Equivalence in so-called spatial flow theories of gravity, and we discuss the essential kinematic properties of the flow which distinguish its gravitational, non-inertial, and inertial modes. We also point out that the acceleration experienced by a body moving in the flow does not always coincide with the co-moving derivative of the flow itself. | + | We present a physical analogy which can be used to understand the issues involved in the Principle of Equivalence in so-called spatial flow theories of gravity, and we discuss the essential kinematic properties of the flow which distinguish its gravitational, non-inertial, and inertial modes. We also point out that the acceleration experienced by a body moving in the flow does not always coincide with the co-moving derivative of the flow itself. |
− | [[Category:Gravity]] | + | [[Category:Scientific Paper|pedagogy bubble analogy difference gravitational forces rocket thrust spatial flow theories gravity]] |
+ | |||
+ | [[Category:Gravity|pedagogy bubble analogy difference gravitational forces rocket thrust spatial flow theories gravity]] |
Latest revision as of 19:49, 1 January 2017
Scientific Paper | |
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Title | Pedagogy: The Bubble Analogy and the Difference Between Gravitational Forces and Rocket Thrust in Spatial Flow Theories of Gravity |
Author(s) | Thomas D Martin |
Keywords | {{{keywords}}} |
Journal | None |
No. of pages | 7 |
Abstract
We present a physical analogy which can be used to understand the issues involved in the Principle of Equivalence in so-called spatial flow theories of gravity, and we discuss the essential kinematic properties of the flow which distinguish its gravitational, non-inertial, and inertial modes. We also point out that the acceleration experienced by a body moving in the flow does not always coincide with the co-moving derivative of the flow itself.