Banana Joe said:
Let’s consider this experiment: we have a straight rail with a rocket attached, on the rocket we have two arms (in the same orientation of the track) with a light source in the middle, each arm has at its extreme a light detector, plus we have one stationary detector at each end of the track. The rocket starts at one end of the track, reaches the maximum speed possible, and then the light source fires an impulse exactly in the middle of the track.
Here's a spacetime diagram depicting your scenario. The rocket starts out stationary at the left end of the track. The ends of the rocket are shown in blue and red. The ends of the track are shown in black and green. The middle of the rocket and the track are shown as separate grey lines. The dots mark off hundred nanosecond intervals of Proper Time for each end of each object and their middles. The speed of light is one foot per nanosecond.
The Proper Length of the rocket is 600 feet when at rest and it is accelerated to 60%c such that it's Proper Length is maintained at 600 feet. The Proper Length of the track is 1800 feet:
When the middle of the rocket reaches the middle of the track (the two grey lines intersect), the light source at the middle of the rocket emits a short burst of light which travels at c in both directions in the Inertial Reference Frame depicted in the diagram. As you can see, the light reaches the two detectors at each end of the track 900 nsecs later.
Banana Joe said:
If the speed of light was affected by the motion of the light source, I would expect the two sensors on the rocket to detect the light at the same time, and the stationary sensor at the end of the track in the rocket’s direction to detect it before the other one.
Or if the speed of light was affected by the Inertial Reference Frame (IRF) you choose to depict your scenario in, specifically, if it is defined to propagate at c in all directions, then you would expect the two sensors on the rocket to detect the light at the same time, just like when we transform to the IRF in which the rocket is at rest:
As you can see, the light reaches both rocket detectors in 300 nanoseconds. And note that the Proper Length of the rocket is still 600 feet when at rest in this IRF.
Banana Joe said:
If instead the light traveled at c from the point of emission regardless of the speed of the light source, I would expect the two stationary sensors to receive the light at the same time, and the sensor on the back of the rocket to receive it before the one in the front.
Or if the light travels at c no matter what IRF you depict the scenario in, then in the rest IRF of the track, the detectors at the ends of the track receive the light at the same time, as shown in the first diagram above.
Banana Joe said:
According to relativity, instead, not only the moving sensors detect it simultaneously, but also the stationary ones do, correct?
That is not the best way to say it. A better way to say it is in the rest IRF of the rocket, the rocket sensors detect it simultaneously and in the rest IRF of the track, the track sensors detect it simultaneously. So whichever sensors are at rest (stationary) in the IRF are the ones that detect the light simultaneously.
Banana Joe said:
Doesn’t that mean that light would be traveling at two speeds at the same time, at c relative to the track and the stationary sensors, and at c relative to the moving sensors (so at (c + the velocity of the rocket) relative to the track)?
No, you need to pick one IRF at a time, not two IRF's at the same time. Observers cannot measure the propagation of light. They cannot tell which IRF you are using to describe the scenario.
Banana Joe said:
If I’m in the rocket and everything is slower and I can’t notice, and I see the light traveling at c, shouldn’t that mean that it’s actually moving slower? If it was actually moving at c relative to me, shouldn't it appear to move faster than c?
You cannot see the light traveling at all. It's not a bullet that you can shine a light on to see where it is at any given moment and then plot its position as a function of time. How would you light up the light to see where it is? Instead, the best you can do is reflect the light off an object and then measure its "average" round trip time. When we apply Einstein's convention, we assume that the light takes the same amount of time to get to the target as its reflection takes to get back in any IRF and that allows us define the time it takes for the light to reach both stationary detectors in each IRF to be the same.
Pretty simple, isn't it? Does it make sense? Any questions?