- #1
mich
- 40
- 0
The last thread I started consisted of the problems that I had with the implication of length contractions of a moving frame as measured by an observer on a different reference frame, although I had no problems with time dilations. With the help of all of you, I have now come to understand why a length contraction is needed as well as a dilation of time.
My original thought was that there could be an experiment which might prove whether or not a contraction could be observed, by simply doing the M&M experiment, having the observer (sensor) on a moving frame.My thought was that Relativity would predict that the observer on the moving frame would disagree with the observer stationary to the experiment concerning the simultaneity of the event when the two light signals arrives at the sensor. I was shown why this couldn't be done because both Relativity and Newtonian mechanics would predict the same outcome,that is, both would see the event as being simultaneous. therefore, proving nothing whatsoever.
My thought continues from here; so what would be the consequence, then, if the experiment was done and, to everyone's amazement (which was the reaction of Michelson), the event was observed as being non-simultaneous by the observer on the moving frame, relative to the experiment?
While it would disagree with Einstein's first postulate, it would not disagree with Relativity as such. For one thing, no form of classical
physics could predict such an outcome. But what about Relativity?
If we assume that the measuring rods within a moving frame, as measured from an observer on a different frame, is contracted not only in the direction of travel, but everywhere within the frame itself, then, it would explain the hypothetical outcome.The whole frame becomes contracted or smaller instead of just in the direction of motion only. The length of the vertical leg, being also contracted, would leave the hypotenuse also to be shorter, being the path of light observered by the observer on the moving frame.
The implication of this hypothetical outcome could be fairly important, since this would imply that certain events, such as a collision between two particles could exist on one frame while a nearmiss would be observed by another different moving frame. Observers on different frames would constitute an observation of, not only different time or length measurements, but also of different realities.
Andre
My original thought was that there could be an experiment which might prove whether or not a contraction could be observed, by simply doing the M&M experiment, having the observer (sensor) on a moving frame.My thought was that Relativity would predict that the observer on the moving frame would disagree with the observer stationary to the experiment concerning the simultaneity of the event when the two light signals arrives at the sensor. I was shown why this couldn't be done because both Relativity and Newtonian mechanics would predict the same outcome,that is, both would see the event as being simultaneous. therefore, proving nothing whatsoever.
My thought continues from here; so what would be the consequence, then, if the experiment was done and, to everyone's amazement (which was the reaction of Michelson), the event was observed as being non-simultaneous by the observer on the moving frame, relative to the experiment?
While it would disagree with Einstein's first postulate, it would not disagree with Relativity as such. For one thing, no form of classical
physics could predict such an outcome. But what about Relativity?
If we assume that the measuring rods within a moving frame, as measured from an observer on a different frame, is contracted not only in the direction of travel, but everywhere within the frame itself, then, it would explain the hypothetical outcome.The whole frame becomes contracted or smaller instead of just in the direction of motion only. The length of the vertical leg, being also contracted, would leave the hypotenuse also to be shorter, being the path of light observered by the observer on the moving frame.
The implication of this hypothetical outcome could be fairly important, since this would imply that certain events, such as a collision between two particles could exist on one frame while a nearmiss would be observed by another different moving frame. Observers on different frames would constitute an observation of, not only different time or length measurements, but also of different realities.
Andre