The frictional force is responsible for causing the coin to slip. This force is given by \( f_r = m \cdot \omega^2 r \), where \( \omega \) is the angular velocity and \( r \) is the distance from the center.
Given that the angular velocity is halved, we use the equation \( \omega^2 \cdot r^2 = \text{constant} \). When the angular velocity is halved, the distance \( r \) from the center at which the coin slips will be:
\[
r_2 = 4 \, \text{cm}
\]
Thus, when the angular velocity is halved, the coin will slip at a distance of 4 cm from the center.