- #1
Thomas Rigby
- 22
- 3
I read about Noether's theorem that says how for every symmetry there is a conserved quantity. Seems kind of obvious. Does anyone understand it well enough that they can explain precisely why that notion is profound?
Well, what's "profound" is something of a matter of taste, but...I read about Noether's theorem that says how for every symmetry there is a conserved quantity. Seems kind of obvious. Does anyone understand it well enough that they can explain precisely why that notion is profound?
And yet, if you phrase Noether's Thm in that too-simplistic way, the statement is false.I read about Noether's theorem that says how for every symmetry there is a conserved quantity. Seems kind of obvious.
One can deduce various features of a (class of) systems by examining its symmetries, more easily than exhaustively solving its equations of motion. E.g., solving for Kepler orbits leads to a transcendental equation which cannot be solved analytically. But a study of the various symmetries of that problem (energy conservation, momentum conservation, the LRL vectors, and the K3 dilation symmetry) allow many useful features of the orbits to be deduced. E.g., what's the relation between orbital radius and tangential velocity, and so on.Does anyone understand it well enough that they can explain precisely why that notion is profound?
She was described by Pavel Alexandrov, Albert Einstein, Jean Dieudonné, Hermann Weyl and Norbert Wiener as the most important woman in the history of mathematics.Well, what's "profound" is something of a matter of taste, but...
Please, prove it.Seems kind of obvious.