GeorgeDishman said:
OK, that has been the impression I was getting, my apologies if I got that wrong.
No need to apologise, I think it can be a natural dynamic of such discussions. When I understand the point I am making, I tend to presume that others will as well, so I might not always make the points clearly enough.
GeorgeDishman said:
Correct.
Correct.
In that case there is no problem the key is that while "relative" and "absolute" are different, both phrases refer to the same concept of simultaneity. That's what you said above so were are good up to here.
I think we're in agreement on here, but just to clarify. The term "simultaneity" in both concepts refers to the same thing i.e. happening at the same time.
But both are different concepts, in and of themselves.
GeorgeDishman said:
Is there or isn't there? You just said you weren't clear on it and then you say that it is clear there is no disagreement? This is very important because that is the single definition of simultaneity which the previous phrases share (and which we address later).
Again, apologies, I didn't elucidate that particular point clearly enough.
There is no disagreement over the concept of "simultaneity". I think we agree that it means "happen at the same time"
What I am not clear on is whether the equality of numerical values is a necessary requirement for determining simultaneity in Lorentzian relativity. As I see it, it boils down to a question of what the time co-ordinates represent.
In Lorentzian relativity "local clocks" don't tell the "true time", so I can't see how inferences can be made concerning the simultaneity of events, from inaccurate clocks. Those clocks can be used for the purpose of transforming co-ordinates from one reference frame to another, but I don't see how inferences about simultaneity can be made.
The inference of simultaneity of events appears to be only possible in the absolute rest frame, such that if they are simultaneous in that reference frame then they are simultaneous in all reference frames, regardless of the disagreement between observers.
That we cannot determine the absolute rest frame, is not necessarily important in determining whether LR incorporates AS, or not.
GeorgeDishman said:
Well you've got three of us all telling what the definitions are so that shouldn't be a problem.
And I think I have demonstrated that I have an understanding of those concepts; the issue lies in the conclusions I come to when applying critical reasoning to those concepts.
GeorgeDishman said:
It is the definition of simultaneity which is common to both the relative and absolute alternatives. I'll say it again slowly: the word "simultaneous" means "at the same time". "The same" in mathematically means "having equal values". The values assigned against a axis are called "coordinates" so "simultaneous" means "having the same time coordinate values".
...
Whether the times so allocated from local clocks are "equal for all observers if equal for one" or "equal for one but not for others in motion relative to the first" is the difference between absolute and relative simultaneity.
OK, the point I was making was slightly different, but I don't think it is necessary to go into it. The formulation above helps to clarify what I am trying to get at.
We agree on the idea that simultaneous means "happen at the same time"; where the issue is, as I see it, is in whether or not "at the same time" means having the same time co-ordinate values. The understanding I have is that under Einsteinian relativity it does mean this, but that it doesn't necessarily mean this under Lorentzian relativity.
The reasoning that has lead me to this conclusion is that the time co-ordinates provided by "local clocks", under the Lorentzian interpretation, are not the "true time" co-ordinates of an event. The "true time" co-ordinates can only be provided by a clock at rest in the absolute rest frame, and so, only these time co-ordinates can determine if events are actually simultaneous, or not.
GeorgeDishman said:
Local clocks are used in all the theories because otherwise you introduce an unknown component concerning the signal travel time between the clock and that which is being timed. Lorentzian philosophy included presentism but in the scientific theory clocks behaved identically to those in relativity.
This might be more helpful in clarifying the distinction, because I can't see how RoS is compatible with presentism i.e. the idea that there is only one, single present moment for all observers; the present moment isn't relative, it is the same for all observers.
This would mean that events which are simultaneous in the present of one observer, would have to be simultaneous in the present of all observers, since there is only one present moment for all observers. This would be the case despite the differing time co-ordinates provided by "local clocks" of relatively moving observers.
GeorgeDishman said:
No, generally we just talk of clocks and time, it is the method that matters and that's always the same. A time is what you read from a clock.
But the underlying assumptions about time are fundamentally different, such that what those clock readings represent are fundamentally different.
GeorgeDishman said:
Yes, and so are you

. Look back at what you said at the top of your reply:
I'm not certain about the claim that Lorentz's model didn't exhibit absolute simultaneity; insofar as it incorporates presentism, then it presumably must incorporate AS; for the reason outlined above.
GeorgeDishman said:
The two statements are equivalent, agreed?
I might be misunderstanding the point you are making here, but I wouldn't say the statements are equivalent at all, I would say that the two statements are incompatible.
The concept of simultaneity is the same in both, but RoS refers to the joint possibility of simultaneity and non-simultaneity of events, while AS only allows for one or the other; such that RoS is not compatible with AS because AS doesn't allow for the conditions which would constitute RoS.
This is something you agreed to above, so I must be misinterpreting what you mean by equivalent.
GeorgeDishman said:
I don't think there's any need now. Having resolved that, I would suggest you lay LET aside for the moment, it's philosophy is diametrically opposed to what you need to learn if you are to understand SR and will make it very difficult for you. You can always come back to it once you grasp SR, that's what I did.
I think we're getting closer to resolving it, anyway. A couple of the points you made have helped to clarify a number of the issues.
Ultimately I want to understand the physical world better; this requires an understanding of SR, but is not limited to it. In the context of this discussion, however, a large part of the question can be boiled down to what the necessary consequences of the Lorentz transform are; in that context, understanding LET is important, as it also utilises the transform; if there are differences in the theories, then we can make certain deductions about what are and what aren't the necessary consequences of the transform.