We know that the initial frequency of the tires is 3 times per second, the frequency and angular velocity are related by:
[tex]f=\frac{\omega}{2\pi}[/tex]Then the initial angular velocity is:
[tex]\begin{gathered} 3=\frac{\omega}{2\pi} \\ \omega=6\pi \end{gathered}[/tex]Now, we know that we stop at the end, that means that the final angular velocity is:
[tex]\omega_f=0[/tex]Now, since the angular acceleration is constant we can use the formula:
[tex]\omega^2_f-\omega^2_0=2\alpha(\theta-\theta_0)[/tex]We know that the change in angular position is related to the change in linear position by:
[tex]s=\theta r[/tex]where r is the radius of the motion. Then:
[tex]\theta=\frac{s}{r}[/tex]Hence the change in angular position in this problem is:
[tex]\theta-\theta_0=\frac{60}{r}[/tex]Then the angular accelaration is:
[tex]\begin{gathered} 0-(6\pi)^2=2\alpha(\frac{60}{r}) \\ -36\pi^2=\frac{120}{r}\alpha \\ -\frac{36}{120}\pi^2r=\alpha \\ \alpha=-\frac{3}{10}\pi^2r \end{gathered}[/tex]Therefore the angular accelaration is:
[tex]\alpha=-\frac{3}{10}\pi^2r[/tex]radians per second squared.
(We leave the answer is terms of the radius since we can't relate the angular motion with a linear motion in other way).