To solve this problem we will apply the kinematic equations of angular motion, we will begin by defining the centripetal acceleration which is given by,
[tex]a = \frac{v^2}{r}[/tex]
Here,
v = Tangential velocity
r = Radius
The tangential velocity is also,
[tex]v = r\omega[/tex]
Where [tex]\omega[/tex] is the angular velocity, then the expression of centripetal acceleration is,
[tex]a = r\omega^2[/tex]
At the same time the angular velocity can be expressed in terms of angular acceleration as
[tex]\omega = \alpha t[/tex]
At t = 3s
[tex]\omega = 3\alpha[/tex]
Then at t = 6s
[tex]\omega = 3\alpha + \alpha (6-3)[/tex]
[tex]\omega = 6\alpha[/tex]
Since r is constant, we have proportionally that the centripetal acceleration is proportional to the square of the angular velocity
[tex]a \propto \omega^2[/tex]
Then the relation between two acceleration is
[tex]\frac{a_2}{a_1} =(\frac{\omega_2}{\omega_1})^2[/tex]
At 6s the centripetal acceleration would be
[tex]a_2 = (\frac{6\alpha}{3\alpha})^2 (2)[/tex]
[tex]a_2 = 8m/s^2[/tex]
Therefore the magnitude of the centripedal acceleration of this point six seconds after the motion beings is [tex]8m/s^2[/tex]