I am trying to develop intuition about Why happen to be true the Hamilton's principle of stationary action, and after seen this video I have a few questions that are more related to maths than physics.
I know beforehand than in general, searching for a stationary points of a function $F(t,\vec{x})$ will lead to different answers than looking for stationary points of the function $|F(t,\vec{x})|$ (it is under the absolute value function).
Now, since the Lagrangian of a system is defined as $\textit{L}=E_k - U$ where $E_k$ is the kinetic energy and $U$ is the potential energy, so the action will be $S=\int\limits_{t_0}^{t_f} \textit{L}\, dt$, the statinonary path will lead to the Euler-Lagrange equations.
Now, there are other external assumptions that will affect how the equations will look like, like having a time-invariant potential will make the forces equal to the negative of its gradient, or the abscence of dissipative forces will make the time derivatives of the lagrangian equal the derivatives of the momentum.
Now for the main question:
- What will happen if instead of solving for the classic action, I will start looking for the stationary points of the following? $$S^*=\int\limits_{t_0}^{t_f} |E_k-U|\, dt$$
- Under which assumptions $S^*$ will have the same stationary points that $S$?
- or they will never happen to be equivalent?