Confirm my reasoning on a generating function proof

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SUMMARY

This discussion centers on the proof related to equation (6.5) in the context of Hamilton's principle and Lagrangian mechanics. The author clarifies that variations in the variables ##q## and ##Q## must be zero at the endpoints to ensure the action integrals are identifiable. It is established that the term involving ##F## vanishes under these conditions, affirming that ##F## should depend solely on ##q##, ##Q##, and potentially on ##t##. The distinction between Lagrangian and Hamiltonian forms is emphasized, highlighting that Hamilton's principle allows for more general variations in phase space.

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It's about equation (6.5) I'm not entirely getting the reasoning explained by the author so I came up with the following, can anyone confirm or refute. One way to look at equation (6.5) would be:

We create variations on the ##q## variables, in the form of ##\delta q(t)##. Since ##Q=Q(q,p,t)## the former variation induces a unique variation ##\delta Q(t)##. Since I want both of the action integrals to make sense, both ##\delta q(t) = \delta Q(t) ## have to be ##0## on the end points. This is not so subtle because technically a variation in ##q(t)## could change ##p(t)## in a non trivial way and ##\delta Q(t)## wouldn't be zero on the end points. However I have to make thsi a condition for both integrals over the Lagrangians to be identifiable as the action.

Under these conditions it is clear that the extra term with the ##F## vanishes.

Is this totally wrong, is this partially correct?
 
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It's correct. That's why ##F## must depend only on ##q##, ##Q## (and perhaps explicitly on ##t##). Note that there are no canonical momenta involved here since the proof deals with Hamilton's principle in the Lagrangian form. I'd also not call these transformations "canonical", because in the Lagrangian formalism you can only do point transformations, i.e., transformations between old and new configuration-space variables, since in the Lagrangian form the variation is with respect to curves in configuration space.

It's important to note that the Hamilton principle in the Hamiltonian form is more general than in the Lagrangian form, because it's about variations in phase space (unrestricted for the momenta and at fixed boundary values for the position variables). Then you have more freedom and thus also more symmetry transformations, namely the canonical ones of the Hamilton description of the dynamics (see the other thread about canonical transformations, last discussed yesterday).
 
Thanks so much for helping me out. About yesterdays thread, I wrote some kind of a summary at the end. I would appreciate it if you could confirm or refute
 

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