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.[[Category:Scientific Paper]]
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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]]
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[[Category:Scientific Paper|pedagogy bubble analogy difference gravitational forces rocket thrust spatial flow theories gravity]]
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[[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
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.