In classical mechanics non-relativistic Lagrangians rely only on the coordinates and their first derivatives to describe a physical system.
Is there a deep reason why particle acceleration etc does not make an appearance as a Lagrangian argument?
In classical mechanics non-relativistic Lagrangians rely only on the coordinates and their first derivatives to describe a physical system.
Is there a deep reason why particle acceleration etc does not make an appearance as a Lagrangian argument?