Conserved charge generates symmetry transformation in Hamiltonian Mechanics

Join the discussion
Registration is free. Start your own thread to ask a follow-up.
1 reply · 3K views
kakarukeys
Messages
187
Reaction score
0
[tex]Q[/tex] is a conserved charge if [tex]\{Q, H\} = 0[/tex]
Show that [tex]q+\epsilon\delta q[/tex] satisfies the equation of motion.
[tex]\delta q = \{q, Q\}[/tex]

I couldn't find the proof. Anybody knows?
My workings:
[tex]\delta q = \{q, Q\}[/tex]
[tex]\delta\dot{q} = \{\{q,Q\},H\} = - \{\{Q,H\},q\} - \{\{H,q\},Q\}[/tex]
[tex]\delta\dot{q} = \{\{q,Q\},H\} = \{\{q,H\},Q\}[/tex]
[tex]\delta\dot{q} = \{\{q,Q\},H\} = \{\dot{q},Q\}[/tex]
Let [tex]q' = q+\epsilon\delta q[/tex]
Show that [tex]\dot{q'} = \{q,H\}|_{q'}[/tex]
L.H.S. is [tex]\dot{q}+\epsilon\delta\dot{q}[/tex]
R.H.S is [tex]\{q,H\}+\epsilon\partial_q\{q,H\}\delta q[/tex]
Therefore we have to prove [tex]\{\dot{q},Q\} = \partial_q\{q,H\}\{q,Q\}[/tex]
...
No clue how to continue
 
Physics news on Phys.org