name123 said:
So once returned the proper time that has passed for ship C is less than the proper time that has passed for Earth. Its clocks have objectively "ticked" less than those on Earth, regardless of how it appeared to ship C. Not quite clear on how from C's perspective the Earth's clocks suddenly seem to have been ticking faster after all, and not have done 0.8 the amount of "ticks" that had happened on C. If you can explain that, that would be great, if not, it doesn't matter.
It's not that The Earth's clock "seem to be ticking fast after all"., It's that by C's measurement, the Earth clocks ran really fast during the short time C was under acceleration And ran slow the rest of the time.
But if for ship C its clocks have objectively ticked less than those on Earth's. Then its clock was ticking slower as it had appeared to the observer on Earth.
As far as C is concerned, it's clock only ticked slow relative to the Earth clock during the period it was under acceleration, during the rest of the time it ran faster.
Given that C's journey consisted of an outward leg, during which it's clocks were in synch with those of A and an inward leg during which it's clocks were in synch with those of B, then can one not conclude that like C the clocks on A and B were objectively ticking slower than those on Earth?
No. As measured by the Earth, the clocks on A, B and C all run slow at the same rate while C is cruising. There will be a short period (for our purposes we will treat is as being infinitesimally short) where C when from cruising speed to zero speed and back up to cruising speed, during which time C's clock rate varied between running slow and running at the same rate as the Earth clock.)
As measured by clock A, the Earth clocks always ran slow by a fixed rate, and the clock on C ran at the same rate as theirs for part of the trip and ran really slow (even slower than Earth's clocks) for the rest of the trip
For B, Earth's clocks ran slow at the same rate for the whole time, and C's clock ran really slow for the first part of the trip then ran at the same rate as theirs for the rest of the trip.
For C the Earth clock ran slow during the outbound leg, ran extremely fast during turnaround, and then ran slow again during the return trip.
So while everyone agrees as to what the respective time it is on Earth and on C's clock when they meet up again, they don't agree as to exactly how this came about.
And there is no objective way to say what really happened. In other words, each of these views of what happened during the course of the trip is just as valid as any other. You can't ever say that one clock "actually" ran fast or slow compared to another at any given point of the trip.
Supposing A goes out along side C, and passes B at the point C turns around, and as B passes A it sets its clock to the time on A's and comes back along side C. If one were to assume almost instantaneous acceleration and deceleration for C, then presumably its clock would be roughly in synch with A's on the outward journey and in synch with B's on the inward journey, and the time on B's, like C's would be less than the clock it passes on Earth as C returns. Unlike C, A and B would be in inertial frames.
Now I have to bring the third "leg" of Special Relativity into play, The Relativity of Simultaneity. In a nutshell, it means that events that are simultaneous in one frame, are not going to be simultaneous for another frame in motion with respect to the first frame, if the events are separated along the line of relative motion.
As an example. Imagine that we put a clock at the turn around point, that has been synchronized with the Earth clock according Earth's and the turn around point's frame. For C and A, when the clock on Earth reads 0, the clock at the turnaround already reads 0.36 yrs. For ship B, when the clock at the turn around reads 0, the clock on Earth already reads 0.36 yr. Thus for ship's A and C, when A leaves Earth at time 0, the clock at turn around reads 0.36 yr, and in the time it takes (0.8 yr by A and C's clocks) this clock runs at a rate of 0.8 and accumulates 0.64 yr to read 1 yr, while their own clocks read 0.8 yr.
Ship B is just passing the turnaround at this moment, and takes the reading of 0.8 yr onto its own clock. For him, it will also be 1 yr at the turnaround clock, but it will be 1.36 yrs at the Earth clock. He will continue on towards Earth, adding another 0.8 yr to his clock, while the Earth clock runs slow and accumulates 0.64y. His clock will read 1.6 yr and the Earth clock will read 2 yrs upon his arrival.
Note that according to ships A and C, when they reach the turnaround point and the clock there reads 1 yr, the Earth clock at that moment only reads 0.64 years, while according to B, when it passes ship A at the turnaround point, the Earth clock already read 1.36 yr. Relativity of Simultaneity in action. For Ships A and C, the events of the Earth clock reading 0.64 and the turnaround clock reading 1 yrs are simultaneous. But for ship B, they are not, for him the simultaneous events are the turnaround clock reading 1yr and the Earth clock reading 1.36 yr.
Unfortunately, when people first start learning about SR, they usually start with time dilation. The problem is that SR only really makes sense if you also include length contraction and the relativity of simultaneity. And of the three, I really think that the relativity of simultaneity should be the one you start with. Once you grasp this idea, the other two fall into place very easily.