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We continued exploring candidate symmetry transformations, adding space rotations and Galilean boosts to our first two (space and time translations). These four transformations together form the "Galilean group", the classical analog to the Lorentz group in special relativity. They leave the E-L equations unchanged if they change the Lagrangian only by a total time derivative dF/dt -- a question we investigate by direct calculation of tex2html_wrap_inline10 .

We then derived one of the most elegant and widely valid theorems in physics, Noether's theorem. It says that for every continuous symmetry a system has, there exists a conserved charge Q. Specifically, for a symmetry transformation tex2html_wrap_inline14 , which changes the Lagrangian by tex2html_wrap_inline16 , the charge tex2html_wrap_inline18 is conserved.

We then looked at the consequences of Noether's theorem for a system of coupled oscillators whose Lagrangian was space-translation invariant. We found that the conserved quantity given by Noether's theorem for the symmetry of translation by tex2html_wrap_inline20 was the tex2html_wrap_inline22 - component of linear momentum.

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Katherine Benson
Fri Nov 8 15:32:54 EST 1996