Peter Martin said:
I agree. Here's my thought on the subject of inertial frames of reference and the principles describing the propagation of light.
Does Einstein’s train-lightening thought experiment violate SR?
Let’s propose a scenario which doesn’t differ significantly from Einsetin’s.
A high-speed bullet train runs on a straight portion of track. A woman sits in an isle seat at the train’s midpoint. The doors between the cars are open, allowing the woman to see all the way to the front and rear of the train, where at each location a strobe light is mounted. The two lights are wired to a switch at the woman’s seat.
As the train plummets ahead, she throws the switch. Let’s assume Einstein’s conclusion that she sees the forward flash first.
Now, the train is an inertial reference frame. SR states that all the laws of physics — including those pertaining to light — are the same for all inertial reference frames — that there exist no “preferred” reference frames. Any inertial reference frame has an equal claim to being “at rest” relative to other frames.
But the train is a preferred reference frame. (Or more accurately, a “non-preferred” reference frame.) By analyzing data entirely from within the train, she can conclude that the train is moving. Were the train at rest on the tracks, there is no doubt she would see the strobe flashes as simultaneous. Knowing the train’s length and having an atomic clock, she could even calculate the train’s speed based on the interval between the arrival of the two flashes.
I’d appreciate a clear explanation of what’s wrong with this picture.
In the scenario you give, Einstein conclusion would not be that she would see the forward flash first, but that she would see both flashes at the same time She would also conclude that both strobes were triggered simultaneously. An observer on the embankment would agree that the light from the flashes reach her at the same time, but would not agree that the strobes were triggered simultaneously. If she timed the throwing of her switch such that, according to her the signals traveling along the wires reached the strobes at the same moment as she was passing the embankment observer, you have basically the same thing as Einstein's train experiment where you have just changed the frame in which the flashes are deemed to occur simultaneously. (even in the original set up, our train observer would agree that the light flashes hit the embankment observer at the same moment.)
The only thing you have added is that she initiates the strobes by throwing a switch connected by wires to the strobes. But there will be a propagation delay between the throwing of the switch and the strobes firing. For her this delay will be equal for both strobes. For the embankment observer, it will not be. For him, you would have to apply the relativistic addition of velocities to the signals.
Electric signals travel a bit slower than c. Lets' use 0.95c as an example, and assume that the train is moving at 0.99 c relative to the tracks.
Then for the embankment observer, the signal traveling in the direction of the train's motion would be moving at
(0.99c+0.95c)/(1+0.99c(0.95c)) = 0.9997c, relative to himself and 0.0497c with respect to the train.
The signal traveling in the other direction would be moving at
(0.99c-0.95c)/(1-0.99c(0.95c)) = 0.6723c relative to him and 0.2777c with respect to the train.
Since switch is at the midpoint between the strobes on the train, this signal will reach its strobe first triggering its flash before the other according to the embankment frame.
Introducing the switch and signals traveling along them the wires just adds another complicating factor to the scenario. One which includes more than just the relativity of simultaneity which the scenario is meant to illustrate.