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When a particle moves in a circle, it is constantly changing direction, which means it is accelerating even if its speed is constant. This centripetal acceleration is directed towards the centre of the circle and requires a centripetal force.
If a particle moves in a circle of radius r, its angular speed omega is:
omega = d theta/dt
where theta is the angle swept out. The SI unit is rad s^(-1).
For one complete revolution: theta = 2pi, time = T (period).
omega = 2pi/T = 2pi f
where f is the frequency (revolutions per second).
The linear speed v (tangential speed) is related to angular speed by:
v = r omega
A particle moving at constant speed v in a circle of radius r has acceleration directed towards the centre:
a = v^2/r = r omega^2
This is the centripetal acceleration. It changes the direction of the velocity but not its magnitude.
By Newton's Second Law, the force required to maintain circular motion is:
F = mv^2/r = mr omega^2
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