teachmemore said:
Also I need to correct something in this thought experiment that arises from my post #30 there. The stationary counter could not possibly send out its first pulse when the device is triggered.
Instead of having a scheme with a "switching device" sending a signal to get both counters started, you could just have both counters programmed to calculate the current time in the stationary frame, and then have them both start sending signals at a pre-decided time-coordinate in the stationary frame.
teachmemore said:
The question then becomes this:
If the two counters are equally relative to one another, how did one counter send more pulses than the other? Both the number of pulses and the number of counts should be equal.
I don't believe that this defies special relativity. I think there is a difference between what can be perceived by data transmission and what special relativity says about relative motion and time.
Each counter sees the same ratio between (rate other counter's signals are arriving)/(rate I am sending signals). In this case, since the counters are moving towards each other each sees the other's signals coming in
faster than they themselves are sending signals. However, if they each start sending signals simultaneously
in the stationary frame (as would be true under my assumption above), then their view of one another is not completely symmetrical, because the delay that each counter sees between the time it started sending signals and the time it sees the first signal from the other counter will not be equal due to the relativity of simultaneity, so the stationary counter sees a greater delay and thus receives less signals in total from the moving counter than the moving counter receives from the stationary counter.
For example, suppose in the stationary frame the stationary counter is at x=0 light-years, and the moving counter is moving towards it at 0.6c, and at t=0 years the moving counter is at x=30 light-years, and both counters start sending signals at t=0, each sending signals at a rate of 1 per year according to their own clock. Then the two counters will meet after a time of 30/0.6 = 50 years in this frame. Since the moving counter sends the first signal at t=0 from 30 light-years away, the stationary counter receives the first signal at t=30, a delay of 30 years. Meanwhile, at t=18.75 years, the moving counter will be at position x=30 - 0.6*18.75 = 18.75 light-years, and naturally the first signal from the stationary counter will also be at x=18.75 light-years at time t=18.75 years, so that's when the moving counter receives the first signal. And in fact the delay is even smaller according to the moving counter's clock, since in the stationary frame it's running slow by \sqrt{1 - 0.6^2} = 0.8, so the moving counter only experiences a delay of 0.8*18.75 = 15 years between sending its own first signal and receiving the first signal from the stationary counter.
After each starts receiving signals from the other, they will each receive them at a rate of 2 per year according to their own clock, since the
relativistic Doppler effect equation says f_{received} = f_{sent} \sqrt{\frac{1 + v/c}{1 - v/c}}, so with v/c = 0.6 the received frequency is greater than the sent frequency by a factor of \sqrt{\frac{1.6}{0.4}} = \sqrt{4} = 2. So if the stationary counter receives the first signal when its own clock reads 30 years, and meets the moving counter when its own clock reads 50 years, it must have received 40 signals from the moving counter in this time. Meanwhile if the moving counter receives its first signal at t=18.75 years and meets the stationary counter at t=50 years, a time-interval of 31.25 years in the stationary frame, according to its own clock the time between receiving the first signal and meeting the stationary counter must be 0.8*31.25 = 25 years, so it has received a total of 50 signals from the stationary counter.