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Gravity as a Force and the Newtonian Limit

Abstract

The thesis of this paper is based upon the observation that the Lorentz Transformation probably is not exact to an arbitrary degree of precision-nothing manmade ever is-and therefore the concept of a "space-time manifold" in which time is inseparably bound with space disintegrates and must be replaced by what I call "space with time" or "temporal geometry" which is contrasted with the static geometries of Euclid, Bolyai and Riemann as well as the absolute time of Newton by including in spatial geometry a time parameter which dynamically interacts with spatial variables but is not identical with them as in the Minkowskian conception (which can degenerate into a completely absurd "block space time" in which everything is written out in advance for all time-nature, by contrast, is dynamic and chaotic, not static. In the words of a song by Natasha Bedingfield, "Your book is still unwritten.") The four-metric, , is merely a convenient mathematical auxiliary variable with no direct physical meaning. We define a force as any deviation from a spatial geodesic (thus returning to Newton's original conception), because, among other things, a space-time geodesic cannot be meaningfully defined if there is no space-time manifold, and in that case, gravity is a force. The much ballyhooed "curvature of space-time" (which is said to be the cause of gravity) will be found to be caused entirely by a vector-like potential, , and not the full tensor potential,. We close in our conclusion with some remarks on empiricism and the flaw in trying to develop theories intellectually rather than being guided exclusively by trying to explain empirical results, an activity that has become popular since the-in my opinion, unfortunateunique example of the development of the General Theory of relativity.