teodorakis said:
i got an answer for my question above now another one:)
in mm experiment the null result is verified by the fact that the distance in the direction of motion of light is shrunk by lorentz factor. But they still accept that the velocity of light towards the observer is c+u(u:speed of observer), so until einstein the constantness of the speed of light wasn't known yet or was it?And even after einstein if we use the lorentz factor and add the velocities as i metioned we still get the correct result(time dilation for example) but with mistaken assumption?
I hope i could explain what i mean.
The speed of light is considered always to be c in the frame of an observer in the M-M experiment also. The thing is, though, that while the light is traveling at c, the apparatus is traveling at v as well, so it may look like the speed of light is figured at c+v and c-v but it is really just the combination of c only for the light and v for the apparatus. For example, let's say that according to some reference frame, the apparatus is traveling away from the observer at v while light travels in the same direction along an arm of the apparatus from one end to the other with a length of d as measured in the reference frame. So the light pulse starts at one end of the arm and travels to the other end of the arm at c, but while this is happening, the arm itself is moving away from the observer at v, so the end point is moving away at v.
The distance the observer sees the light pulse travel is just x = c t. The other end of the apparatus was originally at a distance of d from the end that the light pulse started, but during the time that the light pulse was traveling from one end to the other along the arm, the end it was traveling to was also moving away at v, so in a time of t, that end has traveled a distance of v t, making the distance the light has to travel a total of x = d + v t, therefore x = c t = d + v t. The time the light takes to travel this distance according to that reference frame, then, is c t = d + v t, (c - v) t = d, t = d / (c - v). Similarly, for a light pulse traveling from the furthest end to the closest end, the closest end will be moving toward the light pulse at v while the light pulse also moves toward the closest end at c, so less time elapses to travel the arm, with a time traveling back of t = d / (c + v). So the c - v and c + v there have nothing to do with the speed of light itself, being just c always in any direction, but have to do with the time it takes to travel along an arm while the arm is also moving to the frame of reference.