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Legendre Transformation

The above image shows the Legendre Transformation in the context of an introduction to the Hamiltonian formalism.

My question is in 4.6, wherein $u(x, y)$ has been defined; what is the guarantee that we would be able to invert this relation in order to get $x(u, y)$? Or in other words, what is the guarantee that we would be able to write $\dot{q_{i}}$ as $\dot{q_{i}}(p_{i}, q_{i}, t)?$. And doesn't that affect the invertibility of the Legendre transformation as a whole as written in the lines following equation 4.9?

Another question: Is time supposed to be a spectator variable when it comes to a Legendre Transformation in Hamiltonian dynamics?

Could somebody possibly dwell on this rigorously? Thanks.

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