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bhobba said:You know the principle of general covarience is wrong don't you (or rather is totally vacuous as first pointed out by Kretchmann to Einstein - and Einstein agreed - but thought it still had heuristic value)? But that is best suited to the relativity forum.
Its modern version is the principle of general invariance: All laws of physics must be invariant under general coordinate transformations.
Is that what you mean?
Then yes I agree. My two examples of the modern version of classical mechanics would fit that as well.
But I am scratching my head about why the principles I gave from Ballentine would not fit that criteria?
Thanks
Bill
I learned GR from MTW, since they use the term general covariance it was what stuck with me.
Ballentines "derivation" is very much an axiomatic formalisation/deduction similar to using the Kolmogorov axioms to formalise probability theory. His "derivation" feels nothing at all like say deriving Maxwell's equations from experimental observations, like deriving Einstein's field equations from Gaussian gravity, or even like deriving the covariant formulation of electrodynamics from respecting the Minkowski metric. The key takeaway here is that Ballentine's 'principles' contain no actual observational content whatsoever, making them (mathematical) axioms not (physical) principles.
This of course is not to say that there aren't any first principles in QM, there definitely are, for example most famously Heisenberg's uncertainty principle, which is an experimental observation; a proper physics derivation of QM from first principles should contain a first principle like this, not some semantically (NB: I forgot the correct term) closed statement like the Born rule.