DewaldS said:
The relative motion and the relative time of any inertial system to another one is in literature available (to me) subject to multiplication by a factor lambda = (1-v^2/c^2)^-1/2. It is found in the Lorentz transformation as well as STR. Is it possible to arrive at the same result and formulae without the 2nd postulate of STR? I note that some physicists do not go with the 2nd postulate of STR, (Lorentz contraction for Michelson Morley device arm)
That last comment is a little confusing, the 2nd postulate doesn't say anything about Lorentz contraction, rather it says that the speed of light is the same in all inertial frames. From the two postulates of SR you can derive the Lorentz transformation for relating the coordinates of one frame to another, and from that you can derive Lorentz contraction and time dilation.
DewaldS said:
but use the Lorentz transformation (with speed of light as a max inside these formulae) in their arguments - how can this make sense?
"Use the Lorentz transformation" to do what, exactly? To derive the length contraction and time dilation equations? Like I said, the usual sequence is to start from the two postulates of SR (that the laws of physics are the same in all inertial frames, and that the speed of light is c in all inertial frames), use them to derive the Lorentz transformation, and use the Lorentz transformation to derive the length contraction and time dilation equations.
DewaldS said:
Where can I find a derivation of the Lorentz transformation with the arguments that are put forward?
What do you mean "the arguments that are put forward"? Do you want a derivation of the Lorentz transformation from the two postulates?
DewaldS said:
Is the progression of physics not hampered by the 'maximum possible speed of information transmission' being the speed of light? I mean - if I do not see an object traveling at c via it's light reflection -it does not mean that it is not there.
The coordinates of events in a given inertial frame don't depend on when you
see them, if that's what you mean. Normally inertial frames are defined in terms of a hypothetical lattice of rulers and synchronized clocks at rest in that frame, with the coordinates of each event depending on
local readings on this lattice so there is no problem with light delays. For example, if I see an explosion through my telescope when my clock reads t=15 seconds, and I see it happened right next to the 10 light-second marking on my ruler, and the clock sitting at that marking read t=5 seconds at the moment it happened, then I assign the event a time-coordinate of t=5 seconds, not t=15 seconds when I actually saw it.
The one tricky part about using local readings on rulers and synchronized clocks is defining what it means for two clocks at different locations to be "synchronized"--Einstein suggested the convention that each observer defines the meaning of "synchronization" using the
assumption that light travels at the same speed in all directions in their own frame, so that if I set off a flash at the midpoint of two clocks, I define them to be synchronized if they both read exactly the same time at the moment the light from the flash hits them. It is true that this is just a synchronization
convention--one could define what it means for clocks to be "synchronized" in other ways--but what Einstein postulated was that the laws of physics would have the interesting property that they would obey exactly the same equations in the coordinate systems of different inertial observers who each synchronize their own clocks in this way, a property of the laws of physics known as "Lorentz-invariance" (because the coordinate systems of different observers are related to one another by the Lorentz transformation). So far, all investigation into the fundamental laws of physics has backed up the hypothesis that the laws of nature are always Lorentz-invariant.
DewaldS said:
Or if I go faster than the speed of light - even directly into the light - why am I going 'back into time'? (Even in relation to the light wave or 'light particle's' clock)? I do not get this - please help!
Different inertial frames define simultaneity differently, so that if you could send a message that was faster than light in one frame, there would be some other frames where the message would actually be received at an earlier time than it was sent! And since the first postulate of relativity is that the laws of physics work the same in all inertial frames, if it were possible to have messages arrive before they're sent in one frame, then this would have to be possible in
all frames.
The reason different frames disagree about simultaneity has to do with the synchronization convention I mentioned earlier. Suppose I am in a ship with clocks at the front and back, so I synchronize them in the ship's rest frame by setting off a flash at the midpoint of the ship, and setting the clocks to read the same time at the moment the light from the flash reaches each one. But if in your frame you observe the ship to be moving forward, then if you assume the light moves at the same speed in both directions in
your frame, naturally that means that in your frame the light must reach the back clock before the front clock, since the back clock was moving towards the point where the flash was set off while the front clock was moving away from that point, so the light will take longer to catch up to the front clock.
Here is a little youtube movie which illustrates this point. And if you want to know more about the relation between FTL and time travel, see this recent thread:
https://www.physicsforums.com/showthread.php?t=252523