elfmotat
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MihaiM said:Your t is the proper time (which someone in the rocket measures), while your to is the coordinate time (which someone on Earth measures, the observer, "us").
You have them reversed. t0 is proper time and t is coordinate time.
MihaiM said:The correct formula is this, as elfmotat wrote:
\Delta t_{o} = \Delta t \sqrt{1-v^2/c^2}, it's the same as \Delta t = \frac{\Delta t_{o}}{\sqrt{1-v^2/c^2}}, which you take from Wikipedia.
If you use my above definitions, then this is correct.
MihaiM said:So t is the time of the moving clock, to is the time of the static clock (ours).
to should be the moving clock's time.
MihaiM said:Now v is the speed of the moving clock, and we know it is lesser than c, both in respect to the observer. When v increases, then v^2/c^2 increases as well, which means 1-v^2/c^2 decreases towards zero (also \sqrt{1-v^2/c^2} decreases).
Correct so far.
MihaiM said:You can see now how, as the speed of the t clock (in the rocket) is increased, its period has to be lesser, in its frame of reference, to synchronize its ticks to the observer's clock (on Earth, "us").
This is incorrect. The way you had your equations the stationary clock would experience less time. Also, the two observers DO NOT synchronize their clocks - this is impossible.
MihaiM said:Imagine what happens if v is so great that \sqrt{1-v^2/c^2} = 0.8: when the clock on the observer from Earth (to) rings "one hour" [1], the guy in the rocket says "hey, wtf, based on my clock (t), only 48 minutes has passed!" - which is 60*0.8.
The guy in the rocket would not experience time dilation in his rest frame. From his perspective, the guy on Earth's clock is running slower.
MihaiM said:The two equations are equivalent, the former is for use by the observer in the rocket to figure out what time the clock on Earth shows when an hour has passed (to = 0.8 * t = 48 minutes - contracted time), the latter is for use by the static observer to figure out what time the clock in the rocket shows (t = to / 0.8 = 75 minutes - dilated time).
Neither of the clocks actually show these calculated times. The person in the rocket thinks the person on Earth's time is being dilated. The person in the rocket thinks the exact opposite.
Snip3r said:no you don't get me. Consider this a stationary observer S and a moving observer S' having identical light clocks. Now let S measure the time Δt between 2 consecutive ticks of the clock in S. Now how does he see the same clock to tick in S' (time difference between 2 ticks in S' as seen from S)it is Δt'=\frac{Δt}{\sqrt{1-V^{2}/C^{2}}}its also true for S'(as FoR and seeing S) i m just taking one of the case
You still don't have it right. It should be \Delta t' = \Delta t \sqrt{1-v^2/c^2}.