Suppose we have to solve the ODE: $$\frac{dx}{dt} = f(x) ,\forall t\geq 0 \text{ and } x(0) = x^{*}$$ where $f(x^{*}) = 0$
If we don't know anything about f(x), one obvious solution is $x(t) = x^{*}, \forall t \geq 0$. It satisfies both the ODE and the initial condition.
Intuitively this should be the only solution: we start from a point at which the rate of change of the state vector is $0$, so we should remain there for ever.
Can this be proven?
Under which circumstances is this true?
Are there any edge cases, maybe depending on f(x) e.g. if it is not continuous etc?
I am aware of the uniqueness-existence theorem, however since this seems to be a special problem, if you could help me with intuition.
Any help is appreciated!
Does a dynamical system imply that derivatives of higher order not contained in the ODE are zero?
E.g. $f(x) = \sqrt{x}$ has infinite slope at $0+$ and in the example with Norton's dome, someone noted that the acceleration of acceleration was non-zero.
– Anonymous Apr 10 '22 at 11:23