Bending of a cyclist
A cyclist has to bend slightly towards the centre of the circular track in order to take a safe turn without slipping. Imagine a cyclist taking a turn towards his right on a circular path of radius r. Let m be the mass of the cyclist along with the bicycle and v, the velocity. When the cyclist negotiates the curve, he bends inwards from the vertical, by an angle θ . Let R be the reaction of the ground on the cyclist. The reaction R may be resolved into two components: (i) the component R sinθ, acting towards the centre of the curve providing necessary centripetal force for circular motion and (ii) the component R cos θ, balancing the weight of the cyclist along with the bicycle. Thus for less bending of cyclist (i.e for θ to be small), the velocity v should be smaller and radius r should be larger.
For a banked road , let h be the elevation of the outer edge of the road above the inner edge and l be the width of the road . Obviously, a road or track can be banked correctly only for a particular speed of the vehicle. Therefore, the driver must drive with a particular speed at the circular turn. If the speed is higher than the desired value, the vehicle tends to slip outward at the turn but then the frictional force acts inwards and provides the additional centripetal force. Similarly, if the speed of the vehicle is lower than the desired speed it tends to slip inward at the turn but now the frictional force acts outwards and reduces the centripetal force.
When the centripetal force is greater than the frictional force, skidding occurs. If μ is the coefficient of friction between the road and tyre, then the limiting friction (frictional force) is f = μ R where normal reaction R = mg . (i.e) when the tangent of the angle of banking is greater than the coefficient of friction, skidding occurs.
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