The disk has an angular acceleration $\backslash$alpha $=8$ra$($d$)/($s$^(2))$ and

angular velocity $\backslash$omega $=3$ra$($d$)/($s$)$ at the instant shown. If it does

not slip at A$,$ determine the acceleration of point B$.$

$\backslash$omega $=3$ra$($d$)/($s$)$

$\backslash$alpha $=8$ra$($d$)/($s$^(2))$

$16-116-$SP$-$FUQ $($Special Problem $-$ Follow$-$Up Question$)$

Imagine a rock gets stuck in a tire at point A $,$ then becomes dislodged at point B $.$

ax $-$ yx being

horizontal to the right, and y being straight up