
A cyclist bends while taking a turn so that:
Answer
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Hint:When a cyclist takes a turn, he or she should take care of one thing that the angle of turning and force applied should be good so that he or she won’t fall while turning.The centripetal force causes a body to follow a curved direction. It always moves in the opposite direction of the body, towards the fixed point of the path's instantaneous centre of curvature.
Complete step by step answer:
"A force by which bodies are drawn or impelled, or in some way tend, towards a point as to a centre," wrote Isaac Newton. Gravity provides the centripetal force that causes astronomical orbits in Newtonian mechanics. The centripetal force on an object of mass m moving at tangential speed $v$ along a path with radius of curvature $r$ has the following magnitude:
${F_c} = m{a_c} = \dfrac{{m{v^2}}}{r}$
When riding on a curved track, a force known as centripetal force holds the cyclist on the course. The friction on the tyres provides this force. However, due to the cyclist's high speed, additional force is required to hold the cyclist on the road. The horizontal part of the cyclist's regular force is responsible for this force. The force that opposes gravity is known as the normal force. The normal force's orientation tilts as it bends, resulting in a vertical and horizontal aspect of the force.
Note: The case in which a body travels at a constant speed along a circular path is a typical example of centripetal force. The centripetal force is guided at right angles to the motion as well as along the radius of the circular path towards the middle.
Complete step by step answer:
"A force by which bodies are drawn or impelled, or in some way tend, towards a point as to a centre," wrote Isaac Newton. Gravity provides the centripetal force that causes astronomical orbits in Newtonian mechanics. The centripetal force on an object of mass m moving at tangential speed $v$ along a path with radius of curvature $r$ has the following magnitude:
${F_c} = m{a_c} = \dfrac{{m{v^2}}}{r}$
When riding on a curved track, a force known as centripetal force holds the cyclist on the course. The friction on the tyres provides this force. However, due to the cyclist's high speed, additional force is required to hold the cyclist on the road. The horizontal part of the cyclist's regular force is responsible for this force. The force that opposes gravity is known as the normal force. The normal force's orientation tilts as it bends, resulting in a vertical and horizontal aspect of the force.
Note: The case in which a body travels at a constant speed along a circular path is a typical example of centripetal force. The centripetal force is guided at right angles to the motion as well as along the radius of the circular path towards the middle.
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