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Question

when does a car in motion on a banked road skids and when it manages to be in the circular motion without skidding:

i.e., what happens when

centripetal force friction force

and when

friction force centripetal force

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Solution

In the banking of road, Centrepital force acting on the car when moving in circular motion, is balanced by the sinθ component of teh normal reaction.Downward weight of the car is balanced by the cosθ component of the normal reaction.mv2r = N sinθmg = N cosθwhere r is the radius of the circular pathv is the maximum velocity with which car can travel without skidding.N is normal reaction and θ is thebanking agle.on solving these two equations we getV = rgtanθ

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