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Transcript
Dynamics of Uniform Circular Motion
⇒ An object in uniform circular motion is accelerating because its direction is constantly
changing.
Period (T): time for one complete revolution
Speed: v =
2π r
T
Centripetal Acceleration:
v2
r
⇒ direction is towards the center of the circular path.
⇒ magnitude is given by ac =
Centripetal Force:
The net force required to keep an object moving in uniform circular motion.
Newton’s 2nd law for circular motion:
Fc = mac =
mv 2
→
r
∑F =
mv 2
r
Note: centripetal force is not a new kind of force. It is usually a force or combination of forces
such as tension, weight, normal force, friction, …
Note: when doing uniform circular motion problems, it is customary to define positive in the
direction of acceleration (towards the center of the circle)
Banked and Unbanked Curves:
⇒ In an unbanked curve, static friction supplies the centripetal force.
max speed: v = μs gr
⇒ In a banked (frictionless) curve, a component of the normal force supplies the
centripetal force.
angle of banked curve: tan θ =
v2
rg