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inertiaforce said:
According to this video, freefall isn't accelerated motion and is actually stationary. In other words, you aren't moving in freefall:
In other words, you aren't moving in freefall: ... is not necessarily always correct, but it could be in some instances. It would be more proper to say, "You (or an object) cannot ever
feel any motion whatsoever in free-fall:"
Otherwise the video is a pretty good rendition of gravity as Einstein saw it. The easiest way to understand this is to simply consider Einstein's thought experiment that he
himself used to form a slightly different perspective (conjecture) of gravity from that of Newton's now failed "attraction" theory. Now, in all fairness, Newton was pretty close, and Einstein certainly couldn't have completed
his gravity theory (GR) without Newton's help.
The trick to understanding (as employed by Einstein himself) is to use a pictoral imagination of geometry to see why the above video rings so close to true. Math is important to our overall
quantative understanding, and imperative to our conclusive geometric proofs, but there are those times,
in my opinion, when the tedious intricate symbolic language of math tends to clutter up clear understanding of the stark geometric
quality of natures basic principles.
To simplify his understanding, what Einstein did is imagine a chest (elevator) being drawn up in an earth-like accelerated manner (32 ft/sec/sec) in gravity-free space by a cable (A modern version might use a rocket ship under power with the scientists standing on the back wall, directly in front of the engine). Within the chest, he imagined two scientists that conduct simple experiments to see if they are in a gravitational field or not.
For example, one of the "thought" experiments might be to let a couple of balls fall off a table which is standing on what seems to be the floor. Let us do that. To make things interesting, we will have one ball heavier than the other. Next, both balls appear to roll off the table and fall to the floor, arriving simultaneously, just what the two scientists would expect in normal gravity, since that key point is exactly what is observed on earth.
In the previous above case, the balls, being accelerated by the chest and table top, initially stick to it as though they are attracted like Newton's erroneous "attraction-take" on gravity. In reality the balls are held there by the same inertial force one feels when a hotrod (or Space Shuttle) accelerates, pasting one to the seatback. We have always regarded this inertia as a form of artificial gravity and now Einstein has regarded the two to be "equivalent"... hence his Equivalence principle.
To continue, when these balls escape (roll past) the table edge, pure inertia causes them to merely continue to coast through space at the same last speed that previous contact with the accelerating table top gave them (threw them), while the floor speeds up even more (continues accelerating) to soon strike (meet) the balls. In this "chest" case, it is not so much that the different weight balls fall at the same velocity, as it is that the one-piece floor must logically rise evenly. Note that the floor will seem to strike the heavier ball with more force, the
only difference between the simultaneous impacts. In
effect, the side-by-side balls could be standing still, floating like you suggested, or moving along equally in any other form of inertial motion... when the rising floor simply strikes them both at the same time.
For Einstein, to furnish a theory of general relativity (GR) to include gravity, and yet accompany the special case of light (Special Relativity, SR), more thought becomes a nagging mandate. Inevitably, the curvature of space becomes evident in the same above "chest" scenario when Einstein considers what such a chest acceleration might do to the speed of light, which is regarded as merely constant. First, I imagine smiling in an understatement, Einstein remarks that the drawn chest, "would reach unheard of speeds", and leaves it at that. But he also realizes that if Equivalence is to be true, the acceleration of the chest will slightly outrun the ability of light to travel evenly across the room in a straight line. Consider the next paragraph.
In other words, a hole drilled in one side of an inertially moving chest might allow a perfectly perpendicular light beam to shoot across the chest and strike the other wall at exactly the same height as the hole in the first wall. But it cannot hit the same spot if the chest accelerates meanwhile. The acceleration of either the chest, or "equivalent" gravity on earth, means that the perfectly straight light beam will appear to bend in a minute curve and hit the adjacent wall slightly lower than it would in a non-accelerating chest (therefore an inertial chest; a chest either moving
consistantly in an inertial frame or standing still). If we are to continue to regard light as traveling in a straight line,
and we do, the conclusion is that both the acceleration of the chest and gravity itself, will bend space; our dear space which is always the path of light. Voila... light will be bent and it is!
And that is the essence of Einstein's General Relativity.
It gets more complicated for many of us when we apply advanced math, especially beyond our training level, but the basic principle is not so complicated and should never be forgotten. We must all dust it off on occasion. Even Einstein, the king of visualisation and thought experiment, once remarked in mock confusion:
“Since the mathematicians have invaded the theory of relativity, I do not understand it myself anymore.”
(source: In A. Sommerfelt “To Albert Einstein’s Seventieth Birthday” in Paul A. Schilpp (ed.)
Albert Einstein, Philosopher-Scientist, Evanston, 1949.)
Wes
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