bhobba
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DirkMan said:And how does Noether define energy ? I couldn't figure it out reading those links.
Its the conserved Noether charge from time symmetry.
If that's gooblygook you have to know the theorem:
http://phys.columbia.edu/~nicolis/NewFiles/Noether_theorem.pdf
The situation is this. The theorem states given any symmetry then there exists a conserved quantity. For time symmetry, ie the laws of physics do not change with time, that is defined as energy, so from its very definition is conserved. Its beauty is not only does it define what it is, it explains why it's conserved.
'if the Lagrangian is invariant under time translations, that is if it does not depend explicitly on time, then the Hamiltonian of the system is conserved In most physically relevant cases the value of the Hamiltonian is the total energy. We thus discovered that the conservation of energy is a direct consequence of the invariance of the Lagrangian under time translations. Under stable conditions, if you perform a lab experiment today or tomorrow you expect to get the same results. This fact alone implies that energy is conserved.'
The other advantage is it works in mechanics or field theory. It explains why you can't define energy in GR in a straightforward way - because in GR you have space-time curvature:
http://motls.blogspot.com.au/2010/08/why-and-how-energy-is-not-conserved-in.html
Its usually only encountered in advanced treatments, but most when they first see it are simply dumbfounded - its implications are very deep. As Shyan pointed out when Einstein found out about it he was just as amazed.
The other interesting thing about it, is I have found most philosophy types are blissfully unaware of it.
Thanks
Bill