Download presentation
Presentation is loading. Please wait.
1
Curved Tracks
2
Force on a Curve A vehicle on a curved track has a centripetal acceleration associated with the changing direction. The curve doesn’t have to be a complete circle. There is still a radius (r) associated with the curveThere is still a radius (r) associated with the curve The force is still F c = mv 2 /r directed inwardThe force is still F c = mv 2 /r directed inward r FcFc
3
Friction on a Wheel A rolling wheel does not slip. It exhibits static friction. As a car accelerates the tire pushes at the point of contact. The ground pushes back, accelerating the car. Point in contact doesn’t slip Acceleration of the contact point is upward F WG F GW
4
Curves and Friction On a turn the force of static friction provides the centripetal acceleration. In the force diagram there is no other force acting in the centripetal direction. r FcFc
5
Skidding The limit of steering in a curve occurs when the centripetal acceleration equals the maximum static friction. A curve on a dry road ( s = 1.0) is safe at a speed of 90 km/h. What is the safe speed on the same curve with ice ( s = 0.2)? 90 km/h = 25 m/s r dry = v 2 / s g = 64 m v 2 icy = s g r = 120 m 2 /s 2 v icy = 11 m/s = 40 km/h
6
Banking Curves intended for higher speeds are banked. Without friction a curve banked at an angle can supply a centripetal force F c = mg tan . The car can turn without any friction. next
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.