Centripetal Force (F = mv²/r)

Also known as circular motion force

Fc=mv2rF_c = \frac{m v^2}{r}

Worked example: 1200 kg at 20 m/s, r = 100 m → F = 4800 N — press Try an example to run it live, then adjust anything.

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Centripetal Force (F = mv²/r) explained

rmvFc

An object moving in a circle is accelerating even at constant speed, because its direction keeps changing — and sustaining that requires a net inward force of mv²/r. Swing a ball on a string and the string's tension supplies it; drive through a curve and tire friction does. A 1,200 kg car rounding a 50 m curve at 20 m/s needs FcF_c = (1200)(20²)/50 = 9,600 N of sideways grip — nearly the car's own weight.

The v² is the part engineers respect: doubling speed quadruples the required force, which is why exit ramps post low advisory speeds and why racetracks bank their turns — banking tilts the road's normal force inward so friction isn't doing all the work. Solving for v takes the principal positive square root, since speed is a magnitude. And centripetal force is not a new kind of force; it's simply the name for whatever real force happens to point toward the centre.

Centripetal Force (F = mv²/r) formula

Fc=mv2rF_c = \frac{m v^2}{r}
Where
  • FcF_c= Centripetal force (N)
  • mm= Mass (kg)
  • vv= Speed (m/s)
  • rr= Radius (m)