We can use the following parametric equation to describe the motion of the object:
$$x=r \big(\cos(\omega t),\sin(\omega t)\big)$$
Where $r$ is the radius of the circle, and $\omega$ is the angular velocity of the object.
From this equation, we can get the following:$$\dot{x}=\dot r \big(\cos(\omega t),\sin(\omega t)\big)+r\omega \big(-\sin(\omega t),\cos(\omega t)\big)$$
Since $r$ is constant, we conclude that $\dot{r}=0$. So, we have the following:
$$\dot{x}=r\omega \big(-\sin(\omega t),\cos(\omega t)\big)$$
Differentiating again with respect to $t$, we get the following:
$$\ddot{x}=\left(r\dot{w}+\dot{r}w\right)\big(-\sin(\omega t),\cos(\omega t)\big)-r\omega^2\big(\cos(\omega t),\sin(\omega t)\big)$$
Again, since $\dot{r}=0$, we can simplify:
$$\ddot{x}=r\dot{w}\big(-\sin(\omega t),\cos(\omega t)\big)-r\omega^2\big(\cos(\omega t),\sin(\omega t)\big)$$
We notice that $\ddot{x}$ is the resultant acceleration. The first term on the right is the tangential acceleration, while the second is the centripetal acceleration. Notice that they are perpendicular to each other. You can use the Pythagorean Theorem to find the magnitude of the resultant acceleration. This only works if $\omega$ is measured in radians per second.