Noether’s theorem can be defined for the invariance of the action under variations of paths induced by a coordinate transformation which depends continuously on a parameter, $\epsilon$, $q_i(t) \rightarrow \bar{q}_i(t, ε)$, $\bar{q}_i(t, 0) = q_i(t)$.
What differences are there between the variations, $δ_{q_i}$, considered in Hamilton’s principle, and the variations considered in Noether’s theorem?