This question is with reference to a problem in "Problems in General Physics by IE IRODOV" (Particularly problem 1.42 ).
The original problem is :
A particle moves along the plane trajectory $y(x)$ with velocity $v$ whose modulus is constant. Find the acceleration of the particle at the point $x=0$ and the curvature radius of the trajectory at that point if the trajectory has the form:
a) of a parabola $y=ax^2$
b) of an ellipse $\frac{x^2}{a^2}+\frac{y^2}{b^2}=1$
The way I solved it was by making use of the curvature radius formula taught in calculus, for a function $y=f(x)$.
$$\text{ROC}=\frac{\left[1+\left(\frac{dy}{dx}\right)^2 \right]^{\frac{3}{2}}}{\left| \frac{d^2y}{dx^2} \right|}$$ From there I calculated the acceleration by $\frac{v^2}{\text{ROC}}=a_{\perp}$
However, I find this method quite unintuitive. I am looking for a better approach for this problem.
So my question is:
Is there a better approach to solve above problem, rather than using a strictly mathematical approach like I did?
I was thinking of taking components of the velocity, and finding a relation b/w them to get to velocity as a function of $(x,y)$. But I can't seem to get any reasonable arguments to relate the components.