In a mechanical system with some equilibrium point $r_0$, one can do an analysis in order to check if such point is stable or unstable, i.e. the motion of a particle around of it is bounded or unbounded. There are two ways of testing this:
Taking a small perturbation $\epsilon$ around the equlibrium point. One replaces $r=r_0+\epsilon$ into the equation of motion and approximates to first order in $\epsilon$. Then, one must see what kind of solutions has the differential equation, convergent ($r_0$ is stable) or divergent ($r_0$ is unstable).
Calculating the second deriative of the potential, then checking if it is positive ($r_0$ is stable) or negative ($r_0$ is unstable).
Is one of these tests more general (maybe better) than the other? or both of them should work at the same level?
Particularly, I'm having trouble with the Lagrangian system with kinetic energy $T=\frac{1}{2}(\dot{r}^2+r^2\dot{\theta}^2)$ and $V=\beta r$, then:
$$\mathscr{L}=\frac{1}{2}\dot{r}^2+\frac{1}{2}\dot{\theta}^2 r^2-\beta r,$$
which seem to yield different results for each of these tests ($\alpha$ and $\beta$ are positive constants, the system has constant angular velocity $\dot{\theta}=\omega$).