(2010 Pre)
Solution:
For the coin to revolve without slipping, the static friction must provide the necessary centripetal force. Required centripetal force \( F_{\text{c}} = mr\omega^2 \). Maximum static friction \( f_{\text{s,max}} = \mu mg \). So, \( mr\omega^2 \le \mu mg \). This simplifies to \( r\omega^2 \le \mu g \), or \( r \le \frac{\mu g}{\omega^2} \).
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