Einstein's simple argument
Sam Woole said:
Was Einstein too much ado about nothing?
You seem to be missing the point, which is a shame since Einstein's train argument for the relativity of simultaneity is delightfully simple. (You wouldn't be
lying to us, would you Sam?

) I'll give it one more shot.
For one thing, there are just
two events--the two lightning strikes--and these events are
viewed from two different frames of references (as JesseM tried to explain). One frame is the "stationary" platform; the other, the moving train. Events don't "belong" to a frame; they just exist. They can be observed from
any frame.
It may be useful to think of the lightning strikes as making burn marks on the train and the platform. Call the location of the burn marks on the platform A and B; the locations of the burn marks on the train, A' and B'. A diagram showing how things appear at the instant the lightning strikes--according to the platform observers--would look something like this:
Fig. 1.
v→
A' ____________________m' ___________________ B'
A ____________________M____________________ B
(1) ............(2)
To avoid confusion, I'm going to refer to the two lightning strikes as #1 and #2, as labeled on the diagram.
According to the platform observers, both lightning strikes #1 & #2 occur simultaneously. What can we deduce from this? Looking at things from the platform frame, we have no choice but to conclude that the light from lightning strike #2 must reach the moving observer at m'
before the light from lightning strike #1. This is a fact that everyone must agree occurs; even folks on the train will agree with this. (I'll refer to this as proposition #1.)
Another fact that both frames will agree with is that the lightning strikes occur at equal distances from the midpoint observers. By this I mean that observer M (on the platform) is at the midpoint of the two burn marks A & B; similarly, observer m' (on the train) is at the midpoint of the two burn marks at A' & B'. (I'll refer to this as proposition #2.)
Now let's view things from the train frame. Observer m' knows that the lightning strikes occurred equally distant from him (see proposition #2) and he also knows (after all, he was there!) that the light from strike #2 reaches him first (see proposition #1). From this simple fact, and the
relativistic premise that the speed of light is the same for all observers (whether on the train or on the platform), he
must deduce that lightning strike #2 must have occurred
before lightning strike #1. (I'll refer to this as the conclusion.)
This is Einstein's simple argument that events that are observed to occur simultaneously in one frame (the stationary platform frame, in this example) will be observed to occur at different times in another frame (the moving train frame). Simultaneity is not absolute; it depends on the frame doing the measuring.