Why Does a Car Run Off the Road When Going Too Fast on a Curve?

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A car runs off the road when going too fast on a curve due to insufficient centripetal force to maintain circular motion, which is influenced by the vehicle's speed and the curve's banking angle. When a car exceeds the optimal velocity for a given banking angle, it will move off in a tangent rather than follow the curve. The relationship between centripetal force and velocity indicates that if velocity doubles, the required centripetal force quadruples, which can lead to confusion when considering real-world driving scenarios. Friction between the tires and the road is crucial for steering, and without adequate friction or banking, the car cannot stay on the curve. Understanding these dynamics is essential for grasping the physics of circular motion in vehicles.
physicsdude12
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Hey everyone,

I'm having trouble understanding a few aspects in circular motion and specifically in the application of road curves.

Would it possible for someone explain why a car runs off a road when it is going to fast? Basically, i know that a velocity greater than the optimal velocity for a banking angle causes the car to move off in a tangent, but I'm having trouble understanding why this occurs.

Also, the relationship between centripetal force and velocity (centripetal force directly proportional to velocity squared) has confused me even more. Basically, that relationship says that if the velocity doubles, the centripetal force quadruples! This can't be true because when a car is going very fast around a curve, the centripetal force is not enough to keep it in circular motion.

If someone could help me, i would greatly appreciate it.
Thanks,

Also, i am very sorry for my English, it is not the greatest :S
 
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On a surface, friction between the tires and the road keep allow the car to apply a tractive force. On a curve without banking the frictional force allows the car to be steered (turned) in the curve. With banking (inward), there is a horizontal component of force applied by the road.

See - http://hyperphysics.phy-astr.gsu.edu/hbase/mechanics/carbank.html

and http://hyperphysics.phy-astr.gsu.edu/hbase/cf.html

Since Fcentripetal = mv2/r, when v is doubled, Fcentripetal is quadrupled.

Similarly, for linear kinetic energy, KE = 1/2mv2, when v is doubled, the kinetic energy is quadrupled, but the momentum, mv, only doubles.
 
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Thank you very much for your help! :!)
This was really confusing me :eek:
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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