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dv/dt = a Now, at every instant before slipping the frictional force f equals the resultant of centripetal and tangential forces f2 = (mv2/R)2 + (m(dv/dt))2 For no slipping, f< N (mv2/R)2 + (m(dv/dt))2 <( mg)2 (v2/R)2 + a2 < 2g2 v < [( 2g2 - a2 )R2]1/4 Hence the speed at which the car slips v = [( 2g2 - a2 )R2]1/4
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