(I've resized the diagrams for compactness, and added gridlines)
If I use aether type equations, (ie a Galilean transform), then the speed of the light flashes (ie the gradient of the red and yellow lines) would change with reference frame; it would only be c in the aether rest frame.
At t=0, x=0, the clocks in both reference frames reads 0. The difference between clocks in the two frames increases the further (in both time and distance) you go from there.
Flash 1 starts as the back of the platform passes the front of the train, and it propagates at light speed.
Flash 2 starts as the front of the platform passes the back of the train, and it also propagates at light speed.
Both flashes take the same time to travel the length of the train.
Flash 1 takes from t'=-7.5 to t'=17.5
Flash 2 take from t'=7.5 to t'=32.5
So the train observer notices nothing unusual.
In the platform reference frame diagram, the flashes take different times to travel the length of the train, but that's what the platform observer expects, since in their rest frame, the train is moving.
No, the diagrams assume the Lorentz transform. Everything else follows.Yes, I think you put aether type equations into Minkowski Diagrams. The diagrams assume that an observer on the train will recieve the flashes of light from the opposite side of the train at different times.
If I use aether type equations, (ie a Galilean transform), then the speed of the light flashes (ie the gradient of the red and yellow lines) would change with reference frame; it would only be c in the aether rest frame.
Yes, the difference in clock readings between the two frame is a function of time and distance from the origin (look up the Lorentz Transformation)The arrival times of the front of the train change a lot more than the arrival times of the back of the train when it increases in velocity.
At t=0, x=0, the clocks in both reference frames reads 0. The difference between clocks in the two frames increases the further (in both time and distance) you go from there.
The train frame diagram tells the train observer's story.For the observer on the train, the arrival times from opposite ends of the train should remain the same. It is just like saying that your bedroom is in motion but you don't know about it. So then you wouldn't notice anything strange about flashing a light in one direction in the room or the other. In your room you would say that it takes just as long for the flashes to go in each direction.
Flash 1 starts as the back of the platform passes the front of the train, and it propagates at light speed.
Flash 2 starts as the front of the platform passes the back of the train, and it also propagates at light speed.
Both flashes take the same time to travel the length of the train.
Flash 1 takes from t'=-7.5 to t'=17.5
Flash 2 take from t'=7.5 to t'=32.5
So the train observer notices nothing unusual.
In the platform reference frame diagram, the flashes take different times to travel the length of the train, but that's what the platform observer expects, since in their rest frame, the train is moving.
I don't understand gauge theory; the maths is too advanced (Lie algebra?? Lagrangian??). But it's not relevant here since we're not considering interaction with any fields.Layman said:It would have gauge invariance.
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