DaleSpam said:
Such a scenario would be much better as it deals only with SR effects and does not add GR effects into the mix. For convenience let us speak of clock A on the rim of a rotating "wheel type" space station, and clock B in the hub. If we were to draw the spacetime diagram we would get http://upload.wikimedia.org/wikipedia/commons/thumb/8/87/060322_helix.svg/250px-060322_helix.svg.png" like the one posted by JesseM in post 133 as the worldline of clock A. The worldline of clock B would simply be the axis of the helix.
Note, that clocks A and B never meet so you have to define the endpoints of each worldline completely separately. One typical choice would be to choose the intersection of each worldline with a "beginning" and an "ending" hypersurface of simultaneity, usually defined using Einstein synchronization in the rest frame of the hub.
Now, if you do that you find that the interval along worldline A is shorter than the interval along worldline B. So if clock A and B are set to zero at the beginning then clock A will read less than clock B at the ending. Each clock still measures the same 1 second/light-second along their respective paths, but clock A just travels a shorter path.
In case you missed them in the paragraph above that is a yes for your "lagging" question and a no for your "go more slowly" question. In (Euclidean) geometrical terms this scenario is analogous to the fact that the distance from the Atlantic coast to the Pacific coast is shorter when measured from Veracruz to Acapulco than when measured from New York to Los Angeles.
Whilst you point out that clocks A and B never meet this does
not comply with Einstein's chapter 4 depiction which starts off with two synchronous clocks alongside each other. One of them moves in a closed curve until it returns to its original location and is once again alongside the other clock where it is found that the traveled clock will lag behind the clock that has remained at rest.
On the basis that they
do meet we, presumably, do
not "have to define the endpoints of each worldline completely separately."
The rest of your post applies to the mathematically determined Minkowski spacetime concept which, as I have pointed out on several occasions, is
not - according to
Einstein - reality.
I note that you declined to respond to my question regarding the HKX and other salient points so I will repeat same:-
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Did the Hafele-Keating clocks 'go more slowly' than the laboratory clocks? i.e. did they tick over at a slower rate than the laboratory clocks after gravitational time variation effects were taken into account and removed from the equations as Will's did in 'Was Einstein Right?'?
I'm specifically talking about what physically happened to those clocks not what a Minkowski spacetime diagram 'shows'.
Was the paper to which you refer published in a peer-reviewed science journal? Has it been accepted by the physics community?
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Here is another question which although applicable to GR also applies to Einstein's chapter 4 SR depiction specifically a polygonal line clock A relocation but which has similarly been ignored by others in this thread - an observer is located on top of a mountain; he notes that a clock at that location ticks over at the same rate as his own clock which is obviously ticking over at it's 'normal' rate. He moves to sea-level and again notes that a clock at that location ticks over at the same rate as his own clock - which is still ticking over at it's 'normal' rate.
Does he insist that the clock at the top of the mountain and the clock at sea-level are ticking over at the
same rate as each other as determined by his observations or does he apply his knowledge of the Wallops Island experiment and general theory and realize that although the sea-level clock
appears to be ticking over at the same rate as the mountain top clock it is
physically ticking over at a
slower rate?
An astronaut comes to a stop at the end of his outward-bound journey and notes the rate of operation of his clock. He then accelerates and again looks at his clock which, although appearing to be ticking over at a normal rate, is physically ticking over at a slower rate than it was before he started accelerating in the same way that the above mentioned mountain-descending observer's clock ticks over at a slower rate than it did before
he started moving.
My
specific interest is in relation to what is
physically happening to the clocks!
Although I am of the opinion that this analogy is highly relevant it will most likely be emitted from your response as were the above-referred to salient points.