Car on a Banked Curve (no friction)

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Discussion Overview

The discussion revolves around the dynamics of a car traveling on a banked curve without friction, focusing on the forces acting on the car and the implications of different coordinate systems in analyzing these forces. Participants explore the balance of forces, the role of the normal force, and the conditions necessary for maintaining circular motion.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes the forces acting on a car on a banked curve, noting that the normal force and gravitational force are the only forces present, with the horizontal component of the normal force providing the centripetal force.
  • Another participant challenges the initial claim, asserting that the normal force is not canceled out by the gravitational force perpendicular to the plane, and emphasizes that both components of the normal force contribute to the net force.
  • A third participant reiterates that regardless of the coordinate system used, the normal force has both horizontal and vertical components that must satisfy the conditions for circular motion.
  • One participant introduces a practical example of a stationary block on the banked curve, suggesting that it would slide down, indicating that the vertical component of the normal force cannot exceed gravity in that scenario.
  • Another participant counters the previous points by arguing that the assumption of zero acceleration perpendicular to the plane is incorrect, emphasizing that the acceleration is horizontal and has components in both directions.

Areas of Agreement / Disagreement

Participants express disagreement regarding the role and behavior of the normal force in different coordinate systems. There is no consensus on the interpretation of the forces acting on the car or the implications for maintaining circular motion on a banked curve.

Contextual Notes

Participants highlight potential misunderstandings related to the assumptions made about acceleration and the effects of different coordinate systems on force analysis. The discussion reveals complexities in the dynamics of banked curves that are not fully resolved.

stumped101
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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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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.
 
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.
 
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.
 
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.
 

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