Imagine we perform a Gallilean transformation on a particle undergoing simple harmonic motion, such that the velocity at every other pass through the equilibrium postion is zero. It’s clear that at every other pass through the equilibrium position the particle is at rest and the net force applied is zero. It’s also clear there’s no points along its trajectory where its velcoity is zero and there is a net force applied. The particle still manages to move, and I bring this up to demonstrate that the idea that a net force is applied to a particle at rest in order to get it to move is actually too simplistic to be a general rule in Newtonian mechanics. You need further clarification and Norton’s dome is consisitent with Newton’s 2nd law as usually stated nowadays, unless you place additional restrcitions.
I would avoid the term random as that is often taken to mean stochastic. The net force is not indeterminate* in Norton’s dome and is always zero at the apex, as mentioned above it is the 2nd derivative of force wrt to time that is indeterminate at the apex.
It is correct to say that this is a highly unstable situation in the sense that any peturbation takes us away from the situation that we are interested in. As I said though I’m making a point about the theory not reality, so that is not important.
The basic argument of the link you posted is that Norton’s dome demonstrates that Newtonian mechanics is incomplete. This is not an unreasonable opinion, but its not a rebuttal.
*NB this depends on how the problem is set up, but the important thing is it can be set so the force is always defined.