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Physics · Ch 3 — Laws of Motion

Centripetal Force

3.7.1

Centripetal Force

For a particle in uniform circular motion (constant speed, radius rr), the centripetal acceleration is a=v2ra=\dfrac{v^2}{r}, directed toward the centre of the circle. By Newton's second law, there must therefore be a force of exactly this magnitude, also directed toward the centre — called the centripetal force:

Fcp=ma=mv2r=mω2r,F⃗cp=−mv2rr^.F_{cp}=ma=\frac{mv^2}{r}=m\omega^2r,\qquad \vec F_{cp}=-\frac{mv^2}{r}\hat r.

("Centripetal" literally means "centre-seeking".)

Note

Centripetal force is not a separate, independent kind of force (unlike gravity, tension, friction) — it is simply the name given to whatever real force happens to be providing the centre-directed net force in a particular situation.

Examples:

  1. In a whirling stone on a string, the string tension provides the centripetal force.
  2. In a satellite orbiting the Earth, the Earth's gravitational force provides it.
  3. In a car turning on a road, friction between the tyres and the road provides it.
  4. In a planet orbiting the Sun, the Sun's gravity provides it. …