james fairclear said:
something must be physically affecting the tick rate of clocks in motion as otherwise their indicated times would not vary.
This argument is wrong. You have already been told why it is wrong in this thread. Consider the odometer analogy in post #40. Do the different odometer readings for drivers who take different routes between two points mean that "something must be physically affecting the tick rate" of the odometers?
james fairclear said:
If so then the results of the Hafele Keating experiment disprove the principle.
No, they don't. You have already been told why in this thread. See above.
james fairclear said:
There is nothing stated or implied in the first postulate that motion is not something physical.
"Not physical" in this connection means "not invariant" (because "motion" is frame-dependent) or "not directly observable" (because there is no experiment you can do that will tell you that you are "moving" in any absolute sense). So your statement is wrong; the first postulate
does say that motion is "not physical" in this sense.
james fairclear said:
My original question is "Considering an atom within a rigid body, does the angular momentum of an electron within the atom vary when the body is put in motion?"
And the question as you originally phrased it is not well-defined, which is why it does not have a single well-defined answer.
james fairclear said:
Some of the responses provided on this forum suggest that the answer is yes
Because if "angular momentum" includes "orbital angular momentum around some chosen external point", then an electron in an atom at rest relative to that point
does have different "angular momentum" than an electron in an atom that is moving relative to that point. But this definition of "angular momentum" is frame-dependent; it's not something you directly measure, it's something you calculate after you've chosen a particular point, which implies choosing a particular frame in which that point is at rest.
However, when physicists talk about the "angular momentum" of an electron in an atom, they normally don't mean the frame-dependent thing above. They mean the angular momentum (orbital plus spin) of the electron relative to the nucleus of the atom, which is
not frame-dependent and which
can be directly observed, and which is the same regardless of the atom's state of motion relative to some external point. As has already been explained in this thread.
james fairclear said:
which implies that motion will have a physical effect.
No, it implies that some definitions of "angular momentum" are frame-dependent. See above.
james fairclear said:
If there is no physical effect on a body when put into motion
"Put into motion" is ambiguous. If it just means choosing a different frame of reference without doing anything to the body itself, obviously this has no physical effect. But if it means exerting an actual force on the body, which will change its motion relative to other bodies, obviously this
does have a physical effect. But if you use the same term to refer to both of these things, obviously you're just going to confuse yourself.
james fairclear said:
there should be no need to take into account relativistic effects.
This is fallacious reasoning, both because of the issue just stated above and because "relativistic effects" include things that are directly observable.
james fairclear said:
A clock ticking at its highest possible tick rate could be considered to be at rest relative to any other clock ticking at a slower rate.
Wrong, for two reasons.
First, as has already been explained (see my reference to the odometer analogy above), "tick rate" is the wrong way to think about this issue. The correct way to think about it is "distance through spacetime, i.e., elapsed time, along different paths".
Second, there is no such thing as "highest distance through spacetime" in any general sense. To give that any meaning, you first have to pick two particular events in spacetime--for example, "clocks all start out together in a run of the H-K experiment", and "clocks all come back together after completing a run of the H-K experiment". Once you have picked two particular events, then yes, there will be
some particular path through spacetime (worldline) that has the longest possible length (elapsed time) between those events. Or, more generally, you can always compare elapsed times along different paths through spacetime between those two chosen events, and those comparisons will be invariant--all observers will agree on them and they are independent of any choice of reference frame. (Note, btw, that in the actual H-K experiment,
none of the paths taken in the experiment were the absolute longest possible paths between the two relevant events, but, as just noted, the comparisons between the elapsed times on the different clocks are still invariant.)