Answer:
[tex]a = R\alpha\sqrt{1 + \alpha^2t^4}[/tex]
Explanation:
As we know that the acceleration of a point on the rim of the disc is in two directions
1) tangential acceleration which is given as
[tex]a_t = R\alpha[/tex]
2) Centripetal acceleration
[tex]a_c = \omega^2 R[/tex]
here we know that
[tex]\omega = \alpha t[/tex]
[tex]a_c = (\alpha t)^2 R[/tex]
now we know that net linear acceleration is given as
[tex]a = \sqrt{a_c^2 + a_t^2}[/tex]
so we have
[tex]a = \sqrt{R^2\alpha^2 + R^2(\alpha t)^4}[/tex]
[tex]a = R\alpha\sqrt{1 + \alpha^2t^4}[/tex]