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Ich said:Then I didn't understand. You're suggesting that a clock's state is somehow unmeasurably/unpredictably dependent on its acceleration history?
I'm suggesting that it's in a well defined state depending on momentary proper acceleration.
The case I thought we were referring to was the one in which a clock's rate depends in a measurable, predictable way on its acceleration history. But because it depends on the *history*, not just the boundary conditions on a spacelike surface, it means that we can't predict the future evolution of a system based on knowledge of the boundary conditions. That is, the standard way of stating initial conditions in a classical field theory would be to give the coordinates and their first derivatives on some timelike surface. In the case where the clock's behavior depends on its history, you would need more information that in the standard statement of the initial value problem. Given a system in a known state, without knowledge of its history, you would be unable to predict its future evolution.
That's based on the argument I gave in #20.Ich said:I see that in such a theory there's some argument about how time should be defined, and that it's not a simple geometric theory (ii). But why should (i) or (iii) follow?