cos said:
On the basis that the equatorial clock does, on average over an entire orbit, 'go more slowly' than the polar clock I am of the impression that during this orbit the equatorial clock also 'goes more slowly' (i.e. ticks over at a slower rate) than the polar clock.
Only on average over the whole orbit, not necessarily at every moment, depending what frame you choose. In certain frames there will be periods of time where the equatorial clock has a smaller speed than the polar clock, so during these periods of time the polar clock must be ticking slower in such a frame.
cos said:
I agree that "...in this example A is "physically", "really", or "actually" ticking slower than B between the time it's accelerated and the time it reaches B."
You "agree"? I did not say that was what
I thought.
cos said:
however I do not accept that "...there are perfectly valid inertial frames where it is B that's ticking slower during this period of time."
So do you disagree with the math in the second paragraph in my example from post #64 below?
Suppose for example A and B are a distance of 60 light-seconds apart in the "stationary" frame K, and both are synchronized in this frame. Then if A is moved at 0.6c towards B at the moment when both clocks read a time of t=0, it will take 100 seconds in this frame for A to reach B, during which time A will only tick 80 seconds due to time dilation (the Lorentz factor being 1.25), so when A meets B, B will read t=100 seconds while A reads t=80 seconds.
Now consider things from the perspective of the inertial frame where A and B were initially moving at 0.6c and then A was accelerated to come to rest in this frame while B continued to move towards it at 0.6c. In this frame the clocks were not synchronized initially, so when A read t=0, B already read t=36 seconds according to this frame's definition of simultaneity. Then it takes 80 seconds in this frame for B to reach A (because the initial distance between them was 48 light-seconds in this frame due to length contraction, and 48 light-seconds/0.6c = 80 seconds), during which time B only ticks forward by 80/1.25 = 64 seconds due to time dilation, meaning B reads t=36 + 64 = 100 seconds when they meet, while A reads t=80 seconds when they meet. So you see that both frames make the same prediction about their respective times, even though in the first frame A was ticking slower while in the second frame B was ticking slower.
Unless you think the math is wrong in the second paragraph, the second paragraph is saying that in the frame where A and B were initially moving at 0.6c, it must be true that at the moment A accelerates (and we can assume the acceleration is instantaneously brief), A reads t=0 seconds and B reads t=36 seconds, and at the moment B and A meet, A reads 80 seconds and B reads 100 seconds. So B ticked forward by 64 seconds, while A ticked forward by 80 seconds, therefore B was ticking slower during this period, from the perspective of this frame. If you don't disagree with the math--and I can show you that these numbers follow directly from applying the Lorentz transformation to the scenario described in the first paragraph from the perspective of B's rest frame--then how can you say you disagree with the statement that "there are perfectly valid inertial frames where it is B that's ticking slower during this period of time"?
cos said:
In my opinion B's rate of operation can in no way be affected by A's acceleration or deceleration or rate of uniform travel toward (or away from) B!
No one said anything about B's rate of operation being accelerated by A's acceleration! In the frame described by the second paragraph, B is
always ticking at a rate of 0.8 ticks per second of coordinate time, both before and after A accelerates. Before A accelerates A is also ticking at 0.8 ticks per second of coordinate time, but then after accelerating A comes to rest in this frame, and is now ticking at 1 tick per second of coordinate time. Here are a few numbers to make this clear:
At coordinate time of t=-30 seconds in this frame, A reads -24 seconds, B reads 12 seconds
At coordinate time of t=-20 seconds in this frame, A reads -16 seconds, B reads 20 seconds
At coordinate time of t=-10 seconds in this frame, A reads -8 seconds, B reads 28 seconds
At coordinate time of t=0 seconds in this frame (the moment that A accelerates), A reads 0 seconds, B reads 36 seconds
At coordinate time of t=10 seconds in this frame, A reads 10 seconds, B reads 44 seconds
At coordinate time of t=20 seconds in this frame, A reads 20 seconds, B reads 52 seconds
At coordinate time of t=30 seconds in this frame, A reads 30 seconds, B reads 60 seconds
...So, you can see that for each interval of 10 seconds of coordinate time
prior to A's acceleration, B advances forward by 8 seconds (from 20 to 28 seconds between t=-20 and t=-10 seconds, for example), and A
also advances forward by 8 seconds (from -16 to -8 seconds between t=-20 and t=-10). On the other hand, for each interval of 10 seconds of coordinate time
after A's acceleration, B still advances forward by the same amount of 8 seconds (from 44 to 52 seconds between t=10 and t=20, for example), while A now advances forward at the faster rate of 10 seconds (from 10 to 20 seconds between t=10 and t=20).
So B's rate of ticking never changes in this frame, only A's rate of ticking changes, from ticking at the same rate as B before it accelerates to ticking faster than B afterwards. Again, do you disagree that these are the numbers we get if we apply the Lorentz transformation to the scenario as it was described in B's rest frame, or do you agree with the math but think that the description in B's rest frame describes what "really", "actually" happens while the description in this second frame is some sort of illusion?
cos said:
So when you say that it is B that's ticking slower during this period of time this is nothing more than a comparison of the calculated rate of operation of B to that of the rate of operation of clock A thus clock A 'is' ticking over at a faster rate than it was before it started accelerating however I am of the understanding that the concept of time contraction was, for Einstein, unacceptable.
You still have never explained what "time contraction" means. You can see in the above scenario that even though A speeds up after accelerating, its rate of ticking can never be
faster than the rate that coordinate time is passing--is that what you mean by time contraction? Or do you just think relativity forbids a clock's rate from ever speeding up at all after it changes velocities? If the latter, you're incorrect, if a clock changes velocities in such a way that its speed becomes smaller in a given frame, then its rate of ticking will get faster than what it was before changing velocities, from the perspective of that frame.
cos said:
In my opinion, which is probably controversial, clock A's instantaneous velocity can be substituted for v in the Lorentz transformations.
Sure, if you want to figure out what things look like in the frame where A is instantaneously at rest at that instant (but in this frame A was not
always at rest if it is accelerating; by definition an inertial frame must travel at the same constant velocity forever).
cos said:
A is accelerating toward B and has attained a instantaneous velocity of s. He switches his rockets off and at that very instant is moving at the same (albeit, now) uniform velocity of s (i.e he is moving toward B at the same speed as he was at the very instant the rocket shut down).
Of course, did you think I had suggested otherwise?
cos said:
I fail to see why the calculated rate of operation of clock A from B's point of view (or the calculated rate of clock B from A's point of view) will be any different if A has attained an instantaneous velocity of s or is moving toward B with a uniform velocity of s.
In SR we're only calculating things from the "point of view" of particular inertial coordinate systems, I don't know what it means to calculate things "from A's point of view" since A changes velocity at a certain point. If you want to calculate things from the point of view of the inertial frame where A is at rest after accelerating, that is exactly what I was doing in the second paragraph of my numerical example above.
cos said:
Saying that B 'is' ticking slower (or faster) than A in certain choices of frames is NOT the same as saying that B ticks over at slower (or faster) rates than it did before A started moving (or accelerating).
As I point out above, I have never claimed this, so I don't know why you're making this point. When I said "...there are perfectly valid inertial frames where it is B that's ticking slower during this period of time", I thought it was fairly clear from the context that I meant B is ticking
slower than A during this period of time, not that B is ticking slower than B was ticking prior to A's acceleration. Perhaps you misunderstood my meaning? If so, now that I have clarified, do you disagree that "there are perfectly valid inertial frames where it is B that's ticking
slower than A during this period of time" (i.e. the period of time between A accelerating and A and B meeting)? If you don't disagree, then would you say that B is "physically", "really", and "actually" ticking slower than A during this period of time, from the perspective of these frames?