Pedagogy: The Bubble Analogy and the Difference Between Gravitational Forces and Rocket Thrust in Spatial Flow Theories of Gravity: Difference between revisions
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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.[[Category:Scientific Paper]] | 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:Scientific Paper|pedagogy bubble analogy difference gravitational forces rocket thrust spatial flow theories gravity]] | |||
[[Category:Gravity]] | [[Category:Gravity]] | ||
Revision as of 13:52, 1 January 2017
| Scientific Paper | |
|---|---|
| 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.