The Axiomatization of Physics?

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Discussion Overview

The discussion centers on the concept of axiomatization in physics, particularly the attempts by Hilbert and Weyl to establish a foundational set of axioms from which all physical laws could be derived. Participants explore the implications of this idea in the context of classical mechanics, quantum mechanics, and general relativity, as well as its philosophical underpinnings.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants suggest that axiomatization implies having a small set of axioms from which all of physics follows, questioning if this is already inherent in classical mechanics.
  • Others argue that a complete axiomatization is problematic, especially given the limitations of classical mechanics and the effective nature of forces like friction.
  • One participant notes that axiomatization aims to create universally valid physics based on self-evident truths, but expresses skepticism about its feasibility.
  • Concerns are raised about the circular definitions in general relativity, which some argue contradict the principles of axiomatic systems.
  • A participant highlights a flaw in the Dirac-von Neumann axiomatization of quantum mechanics, referring to Wigner's concept of 'Quantum Duality' where different axioms yield different results for the same physical situation.
  • Another participant suggests that the foundational issues in quantum mechanics do not necessarily impede the derivation of quantum field theory from quantum mechanics.

Areas of Agreement / Disagreement

Participants express a mix of agreement and disagreement regarding the feasibility and implications of axiomatization in physics. There is no consensus on whether a complete axiomatization can be achieved or if it is fundamentally flawed.

Contextual Notes

Participants mention limitations such as circular definitions in general relativity and the ambiguity in applying different axioms to the same physical situation in quantum mechanics, which remain unresolved.

"pi"mp
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So I have read that Hilbert and his student, Hermann Weyl both attempted to "axiomatize" physics. What exactly does this mean? I'm sort of naively assuming it means they should like to have a small set of axioms from which all of physics follows. Is that kind of the idea?

But isn't that sort of what physics is already? Like in classical mechanics, can't you make a leap of faith as to the relation between force and acceleration and everything follows very nicely?

Sorry if I'm way off base; just a curious undergrad...also does anyone know of any good books on this topic? or in regard to philosophy of math/physics in general?
 
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Perhaps he meant a complete axiomatization. In his day, they didn't have quantum mechanics, so many Newtonian forces like friction would just be "effective", not fundamental. Of course today, we believe that even the standard model of particle physics is effective (ie. wrong at high energies). And I'd be surprised if anyone can calculate friction from the standard model.
 
They wanted to build a proof of physics based on "axioms" or self-evidentially true statements. By creating a physics which was bourne out of a priori arguments, it could be accepted universally as valid. Axiomatization rarely works for anything, though.
 
"pi"mp said:
So I have read that Hilbert and his student, Hermann Weyl both attempted to "axiomatize" physics. What exactly does this mean? I'm sort of naively assuming it means they should like to have a small set of axioms from which all of physics follows. Is that kind of the idea?

But isn't that sort of what physics is already? Like in classical mechanics, can't you make a leap of faith as to the relation between force and acceleration and everything follows very nicely?

Sorry if I'm way off base; just a curious undergrad...also does anyone know of any good books on this topic? or in regard to philosophy of math/physics in general?

The 1932 book by von Neumann may be considered the answer to Hilbert's quest. See http://en.wikipedia.org/wiki/Von_Neumann#Quantum_mechanics
 
"pi"mp said:
So I have read that Hilbert and his student, Hermann Weyl both attempted to "axiomatize" physics. What exactly does this mean? I'm sort of naively assuming it means they should like to have a small set of axioms from which all of physics follows. Is that kind of the idea?

But isn't that sort of what physics is already? Like in classical mechanics, can't you make a leap of faith as to the relation between force and acceleration and everything follows very nicely?

Sorry if I'm way off base; just a curious undergrad...also does anyone know of any good books on this topic? or in regard to philosophy of math/physics in general?

Right, the idea was to have a small set of axioms from which all physics follows.

However general relativity is not built this way. The definitions are circular, which axiomatics does not allow.
 
PatrickPowers said:
Right, the idea was to have a small set of axioms from which all physics follows.

However general relativity is not built this way. The definitions are circular, which axiomatics does not allow.

It is easy to remove circularity from any set of postulates, just be rephrasing things properly.
Otherwise, Euclid's axioms for elementary geometry (_the_ paradigm fior an axiom system) would have to be regarded as circular, too.
 
Dear Student and Prof. Neumaier:

In my opiniion, and I am convinced this was Wigner's opinion too,
the Dirac--von Neumann axiomatisation of QM suffers from one (fatal) flaw that
means it is not 'Hilbertian'. Wigner called this 'The Problem of Quantum Duality'
and he did not mean wave-particle duality, which he believed was no big deal
and should not even have been called a duality. See his classic papers on
this reprinted in his collection *Symmetries and Reflections*. Wigner was
much influenced by Hilbert, and on this question of Quantum Measurement,
von Neumann learned from Wigner (they were good friends).

Briefly, this 'duality' is that different axioms can be applied to the
exact same physical situation and one gets different answers. This is a fatal
ambiguity or duality. This is the same flaw John Bell pointed to. See Bell's
classic articles reprinted in *Speakable and Unspeakable in Quantum Mechanics*
where he is always careful to distinguish his logical complaints from his
realism and intuition complaints.

I agree with Prof. Neumaier that Hilbert's problem would be
(essentially) solved if Dirac--von Neumann were acceptable, I think QFT
is derivable from QM in principle so introduces no foundational difficulties,
only the usual difficulties of finding practical working approximations that
will calculate answers. And I anticipate no problems unifying GenRel with
QM except that the lack of data means we are going to be unable to distinguish
which unification is correct...not an axiomatic problem.

Try googling on Wigner Quantum Duality to see what I mean.

Oddly enough, *I* am the problem of Wigner's friend since I am
a friend of (his son, David) Wigner and I am certainly a problem... jajajaja...
just ask him...
 

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