Undergrad Is ##p^k = \partial L / \partial \dot{x}^k## true for all ##L##'s?

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The discussion centers on the relationship between generalized momentum and the Lagrangian in classical mechanics, specifically questioning whether the equation p^k = ∂L/∂dot{x}^k holds for all Lagrangians. An example using the Lagrangian L = T - U = (1/2)mv^2 - U demonstrates that the equation is valid for this case, yielding p^k = m dot{x}^k. The conversation seeks to establish a general proof for this relationship across all Lagrangians. A reference to generalized coordinates is provided to support the discussion. The inquiry highlights the need for a deeper understanding of momentum definitions in the context of Lagrangian mechanics.
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TL;DR
Is the relation Is ##p^k = \partial L / \partial \dot{x}^k## true for all Lagrangians?
Using the Lagrangian $$L=T-U=\frac{1}{2}mv^2-U$$ we clearly have $$ \frac{\partial L}{\partial \dot{x}^k} = m\dot{x}^k = p^k $$ i.e., the ##k##'th component of momentum. How does one show that the relation $$p^k = \frac{\partial L}{\partial \dot{x}^k} $$ holds for all Lagrangians?
 
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“The generalized momentum "canonically conjugate to" the coordinate qi is defined by

{\displaystyle p_{i}={\frac {\partial L}{\partial {\dot {q}}_{i}}}.}
https://en.m.wikipedia.org/wiki/Generalized_coordinates
 
Thanks. I did not phrase the question very well. I have made a more detailed post of the question here:
 
Topic about reference frames, center of rotation, postion of origin etc Comoving ref. frame is frame that is attached to moving object, does that mean, in that frame translation and rotation of object is zero, because origin and axes(x,y,z) are fixed to object? Is it same if you place origin of frame at object center of mass or at object tail? What type of comoving frame exist? What is lab frame? If we talk about center of rotation do we always need to specified from what frame we observe?

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