Difference between different radial and centripetal accelerations:(Doubt) In cylindrical coordinates I had derived the acceleration as :

for the first component of acceleration, what is the difference between  radial and centripetal ?
 A: The radial acceleration, $\ddot r$, is responsible to change the rate of change of the radius vector, $\dot r$, which in turn is responsible to change the magnitude $r$ of the radius vector, its length.
The centripetal acceleration $-r \dot \theta^{2}$ is what makes the particle describe some curvilinear path. The "minus" signal in front of the centripetal acceleration indicates it's inward.
A: If we consider only the radial component in the case when $\dot{\theta} = 0$, then it becomes clear that $\ddot{r}$ is a radial acceleration, i.e. since the angular component of velocity is $0$, the particle is only moving along a straight line through the origin, and $\ddot{r}$ is the acceleration along this line.
$$\\$$ Now if we consider when $\ddot{r} = 0$, with $\dot{r} = 0$ also (incidentally, this is just the condition for circular motion around the origin), then $-r{\dot{\theta}}^2$ must be the source of what is making us turn.
A: The only thing I can add to the existing answers that may be helpful is a visual representation, which can be found on Saif Rayyan's MIT course page here and is reproduced below
