Applications of Centripetal Force in Various Scenarios
This page expands on the concept of centripetal force by presenting more complex examples and introducing the idea of motion in a vertical circle.
The page begins with two additional examples of centripetal force calculations:
- A skater moving in a circular path, demonstrating the conversion of weight to mass in imperial units.
- Determining the maximum velocity a car can achieve while rounding a turn, given the maximum force the road can exert on the tires.
Example: For a 160-lb skater moving in a 20 ft radius circle at 10 ft/s, the centripetal force is calculated as 25 lb.
The page then introduces the concept of motion in a vertical circle, which is crucial for understanding tension in vertical circle motion. In this scenario, the tension in the string varies with the object's position due to the influence of gravity.
Highlight: In vertical circular motion, the centripetal force is the vector sum of the tension in the string and the component of the object's weight towards the center of the circle.
Two key equations are presented for the tension at different points in the vertical circle:
- At the top of the circle: T = Fc - w
- At the bottom of the circle: T = Fc + w
Where T is tension, Fc is centripetal force, and w is the object's weight.
An example is provided to illustrate these concepts:
Example: A 1-kg stone is whirled in a vertical circle with a 0.5 m string at 5 m/s. The tension in the string is calculated at both the top (40.2 N) and bottom (59.8 N) of the circle.
This example demonstrates how the tension varies depending on the position in the vertical circle, providing a practical application of the formulas and concepts introduced.




