2.) When we have $[A,H]=0$ than that operator $A$ commutes with the Hamiltonian and the quantity is conserved and also we can measure one without distrurbing the measurment of the other. Cool.
I found out of examples: $[x,p_y]=0$
$[L^2,H]=0$ - for Hydrogen atom (spherically symetric)
Do you know of any more examples (maybe less known) ?