Car on a Banked Curve (no friction)

In summary, the forces acting on a car traveling in a circle on a banked curve without friction are the normal force and gravitational force. When using a x-y coordinate system, the horizontal component of normal force provides the centripetal force and the vertical component cancels out the force of gravity. However, in a coordinate system with axes parallel and perpendicular to the plane, the normal force and force of gravity perpendicular to the plane cancel out, leaving only the parallel force of gravity down the plane. This is due to the fact that the car's acceleration is horizontal, with components parallel and perpendicular to the plane. To determine the necessary banking angle for a given speed and radius of curvature, the equations for the horizontal and vertical components of normal force
  • #1
stumped101
1
0
Hi,

If we have a car traveling in a circle on a banked curve without friction, the forces acting on the car would only be the normal force and gravitational force.

Using a x-y coordinate system, the horizontal component of normal (Nsintheta) provides the centripetal force Fc and it's vertical component (Ncostheta) cancels out the force of gravity. Everything works out here.

However, if you were to the draw the forces in a coordinate system that had axes parallel and perpendicular to the plane, you would find the normal force being canceled out by the force of gravity perpendicular to the plane (Fgcostheta) and leaving us with just a net force of the parallel force of gravity down the plane. What's stopping the car from sliding down the curve now and what's providing the centripetal force on this diagram?

Thank you.
 
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  • #2
stumped101 said:
you would find the normal force being canceled out by the force of gravity perpendicular to the plane (Fgcostheta)

This is where you were wrong.
This component of gravity force is canceled, but the normal force isn't, which leaves a component perpendicular to the plane. It, along with the parallel one, forms the net force, which is the centripetal force.
 
  • #3
No matter what coordinate system you select you'e still going to get the normal force having a horizontal component of N sin theta (which must be equal to centripetal force mv^2/r) and a vertical component of N cos theta (which must be equal to the weight mg).

A handy way to get the banking angle that you need, for a given radius of curvature and speed, is to divide those two equations, which results in tan theta = v^2/rg.
 
  • #4
The important thing here is to analyse why the vertical component of normal force is higher than gravity.
Place a stationary block on the same banked curve. It will slide down. In that case the vertical component of normal force would get defeated by gravity. Drawing force diagrams isn't the only part of physics in this situation. You just found that it had misled you.
 
  • #5
stumped101 said:
However, if you were to the draw the forces in a coordinate system that had axes parallel and perpendicular to the plane, you would find the normal force being canceled out by the force of gravity perpendicular to the plane (Fgcostheta) and leaving us with just a net force of the parallel force of gravity down the plane.
No, the normal force isn't 'canceled out'. You are tacitly assuming that the acceleration perpendicular to the plane is zero, but it's not. The acceleration is horizontal, which has components parallel and perpendicular to the plane.
 

1. What is a car on a banked curve without friction?

A car on a banked curve without friction refers to a situation where a car is moving along a curved track without any external force or resistance, such as friction, acting on it.

2. How does the banked angle affect the car's motion?

The banked angle, which is the angle at which the curve is inclined, affects the car's motion by providing a centripetal force that helps to keep the car moving along the curve. This force is perpendicular to the curve and allows the car to maintain a constant speed and direction.

3. What is the role of gravity in a car on a banked curve without friction?

Gravity plays a crucial role in a car on a banked curve without friction. It provides the centripetal force necessary for the car to maintain its curved path. The banked angle of the curve is designed to work in conjunction with gravity to ensure the car stays on the track without any external forces acting on it.

4. Can a car on a banked curve without friction go faster than a car on a flat track?

Yes, a car on a banked curve without friction can go faster than a car on a flat track. The banked angle helps to provide the necessary centripetal force, allowing the car to maintain a constant speed as it moves along the curved track. This allows the car to go faster without losing control or slipping off the track.

5. What happens if there is friction present on a banked curve?

If there is friction present on a banked curve, it will cause the car to slow down and potentially lose control. Friction acts against the centripetal force provided by the banked angle, making it harder for the car to maintain its curved path. This can lead to the car sliding off the track or spinning out of control.

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