A bowling ball of mass M = 6.50 kg, radius R = 10.0 cm, and moment of inertia I = $(2/5)MR^2$ is given an initial center of mass velocity $v_0 = 3.00 m/s$ that is parallel to a horizontal surface. The ball initially slips alon the floor, but eventually rolls w/o slipping. The coefficient of kinetic friction between the ball and the floor is $\mu_k = .300$.
Part (a) asks for the acceleration of the center of mass of the ball, which = -2.94 m/s^2.
Part (b) asks for the angular acceleration of the bowling ball.
The correct answer is 73.6 rad/s^2. I used the approach below, but I'm not sure why it's wrong:
$a_t = r \alpha$
$\alpha = \frac{a_t}{r} = -29.4 rad/s$
Why is the above approach wrong?