There is a problem given in Goldstein's Classical Mechanics Chapter-1 as
20. A particle of mass $\,m\,$ moves in one dimension such that it has the Lagrangian \begin{equation} L\boldsymbol{=}\dfrac{m^2\dot{x}^4}{12}\boldsymbol{+}m\dot{x}^2V\!\left(x\right)\boldsymbol{-}V^2\!\left(x\right) \nonumber \end{equation} where $\,V\,$ is some differentiable function of $\,x$. Find the equation of motion for $\,x\left(t\right)\,$ and describe the physical nature of the system on the basis of this equation.
$L=T-U$ is only for the cases when the all the forces acting on the system is conservative and the potential is dependent on coordinates only.
In the above case, the potential is dependent on coordinates only.
So, our Lagrangian has conservative forces and there may or may not be some non-conservative forces included in the Lagrangian.
After solving the Lagrange's equation I get the following equation of motion,
$$\Big(m\ddot{x}+\frac{dV}{dx}\Big)\Big(m\dot{x}^2+2V(x)\Big)=0.$$
I have the following doubts
We know that when we use generalized coordinates the kinetic energy term involves
$T_o$(independent of $\dot{x}$) + $T_1$ (linear in $\dot{x}$) + $T_2$ (quadratic in $\dot{x}$).
But in the Lagrangian how we get the term $(\dot{x})^4$ (biquadratic term in generalized in velocity)? How is this possible?The equation which we get in the bold what is its physical implications?
Like we can say that
Either $\Big(m\ddot{x}+\frac{dV}{dx}\Big)=0$ or $\Big(m\dot{x}^2+2V(x)\Big)=0$ or both
$\implies$ Either $m\ddot{x}=-\frac{dV}{dx}=F_{conservative}$ or $\frac{1}{2}m\dot{x}^2+V(x)=0$ or both.
$m\ddot{x}=F_{conservative}$ means that the only force acting in the system is a conservative force.
But what does the second term $\frac{1}{2}m\dot{x}^2+V(x)=0$ implies? If we interpret $\frac{1}{2}m\dot{x}^2$ as kinetic energy then we can say total energy is 0. But I think we can't interpret it as kinetic energy because then in Lagrangian there can't be a term biquadratic in $\dot{q}$.
I am able to solve the Lagrange's equation but I am not able to resolve my above two doubts which in short are 1) structure of Lagrangian and 2) the physical interpretation of motion.
Please help me in clarifying the doubt.
Addendum -
I have one more doubt which is very closely related to this one, so I don't want to ask a new question for that.
We know that if $L'=L+\frac{dF(q,t)}{dt}$, then $L'$ gives same equation of motion as that given by the $L$ after solving the Lagrange's equation.
In the above example, $L\boldsymbol{=}\dfrac{m^2\dot{x}^4}{12}\boldsymbol{+}m\dot{x}^2V\!\left(x\right)\boldsymbol{-}V^2\!\left(x\right)$ gives same equation as that of $L=\frac{m\dot{x}^2}{2}-V(x)$.
So, I want to know is there some specific class of functions on the Lagrangian which gives same equation of motion as that of the original or simplest Lagrangian $(L=T-V)$ after solving the Lagrange's equation?