say_physics04 said:
Hi to all! I’m just curious about something in time dilation. This is the case: IMAGINE you are a passenger in a trolley moving as fast as the speed of light.
There is a problem with this. One can't imagine a trolley moving at the speed of light from the standpoint of relativity theory because such a thing does not exist. Perhaps you would like to know what happens if you imagine you are in a passenger in a trolley moving NEARLY as fast as the speed of light?
Then there is a very huge clock capable of being seen wherever the viewer is. The velocity of the trolley is c and moving away from the huge clock. The current time in the huge clock is 12 noon, the same as the time in YOUR watch before you start moving. As the trolley moves, if I’m correct, you infinitely see the time in the huge clock as 12 noon, but you see the time in your watch running normally- 60 seconds per minute. I
For a trolley moving at nearly the speed of light, you'd see the clock ticking very slowly. This is described mathematically by a doppler shift factor k.
Suppose we make the doppler shift factor k equal to 12 - then you
see the clock ticking at 1/12 its normal rate. What you see includes relativistic time dilation and the fact that as you get further away from the clock, it takes longer from the light from the clock to arrive.
f your trolley keeps moving at this pace for 1 hour, based on an outside observer looking at the huge clock, then suddenly stops and you look immediately at the huge clock, will you see the huge clock having a time of 1 pm, meaning from 12 noon then 1 pm immediately? I know time dilation but I would appreciate if you’ll discuss how it happens in this case.
Thanks a lot!
If your trolley keeps moving at this pace for 1 hour, in the ammended problem 5 minutes pass on the clock. (1/12 of the 60 minutes you experience). If you suddenly stop, the time you visually see on the clockface will not change, but the clock will start to advance at its normal rate. So when you stop, an hour later, the clock reads 12:05, and as soon as you stop, it starts to appear to tick at the normal rate.
One of the best ways to see this is to draw a space-time diagram. To do this successfully, you need to know one fact - that the doppler shift factor k, the interval between transmission and reception, depends only on the relative velocity between the emitter and the receiver.
For more details, try googling for "bondi k calculus".