Incline Plane versus Banked Curve

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SUMMARY

The discussion clarifies the differences between the normal force in incline plane problems and banked curve scenarios. In incline plane situations, the normal force is calculated as the weight of the object multiplied by the cosine of the angle of incline. Conversely, in banked curve problems, the normal force contributes to both vertical and horizontal components, with the horizontal component providing the necessary centripetal force, calculated as the weight multiplied by the sine of the angle of incline. This distinction is crucial for understanding motion on curved paths without friction.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of forces and components in physics
  • Familiarity with circular motion concepts
  • Basic trigonometry, specifically sine and cosine functions
NEXT STEPS
  • Study the derivation of centripetal force in banked curves
  • Explore frictionless motion in circular paths
  • Learn about the effects of different angles of incline on normal force
  • Investigate real-world applications of banked curves in road design
USEFUL FOR

Students of physics, educators teaching mechanics, and anyone interested in the principles of motion on inclined planes and banked curves.

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Okay, so I've been working on incline plane and then banked curve problems. From the incline plane problems and the definitions in my book I believed that normal force was just the y component of the weight, ie the weight times the cos of the angle of incline and no x component, ie parallel to the surface. This assumptions worked for the inclined plane problems, but when I got to the banked curve problems, a car going in a circular banked path with now friction, the centripetal force was now the normal force times sin of the angle of incline, the "x-component" of the normal force. Can anyone explain?
 
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The normal force is the force that is perpendicular to the surface. In an inclined plane, the normal force is equal to the weight of the object multiplied by the cosine of the angle of incline. However, in a banked curve, the normal force is not only perpendicular to the surface but also acts as the centripetal force, meaning it has both a vertical component (equal to the weight of the object multiplied by the cosine of the angle of incline) and a horizontal component (equal to the weight of the object multiplied by the sine of the angle of incline). The combination of these two components provides the centripetal force needed to keep the object on a circular path.
 

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