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Circular Motion and Centripetal Force

Classical Mechanics

Anything moving in a circle is constantly changing direction, which means it is constantly accelerating — even if its speed stays the same. That acceleration needs a force pointing toward the centre of the circle, called the centripetal force. From the Moon orbiting Earth to a car taking a bend, the same rule governs every turn.

a = v^2 / r
Centripetal acceleration equals speed squared divided by radius.
F = m v^2 / r
Centripetal force equals mass times speed squared divided by radius.

Why circular motion needs a force

An object moving in a circle at a constant speed has a constant speed but a changing velocity, because velocity includes direction. Changing velocity means acceleration, and acceleration needs a net force. That acceleration always points toward the centre of the circle and is called **centripetal acceleration**. The force that produces it is the **centripetal force**. It is not a new kind of force: it is simply the name for whichever real force — tension, gravity, friction, or a normal force — happens to be pointing toward the centre in that situation.

The formulas

For an object of speed v moving in a circle of radius r, the centripetal acceleration is **a = v² / r**. Multiply by the mass and you get the centripetal force: **F = m v² / r**. These formulas show two important patterns: a faster object needs much more force (force grows with v²), and a tighter circle needs more force (force grows as r shrinks). That is why taking a bend too fast or too sharply is dangerous — the friction available from the tyres may not be enough to supply the centripetal force, and the car slides outward.

Where you see it

A car rounding a bend relies on friction between its tyres and the road for centripetal force. A satellite stays in orbit because Earth's gravity supplies the centripetal force, pulling it toward the centre even as it moves forward. A stone whirled on a string is held in by the tension in the string — let go, and the stone flies off in a straight line along the tangent, not outward from the centre. A roller coaster loop works because the track pushes on the cars toward the centre of the loop, and clothes in a washing machine are spun dry as water escapes through holes while the drum supplies the centripetal force.

📝 Worked example: a car taking a bend

A car of mass 1000 kg takes a bend of radius 50 m at a speed of 20 m/s. Centripetal acceleration a = v² / r = (20 m/s)² / 50 m = 400 / 50 = 8 m/s². Centripetal force F = m a = 1000 kg x 8 m/s² = 8000 N. Answer: a force of 8000 N toward the centre of the bend is needed, supplied by friction between the tyres and the road.

Common mistakes

Practice questions

  1. A 2 kg ball on a string moves in a circle of radius 1 m at 4 m/s. What is the tension in the string?
    Show answer

    F = m v² / r = 2 x 16 / 1 = 32 N.

  2. If the speed of an object in a circle doubles, what happens to the centripetal force?
    Show answer

    It quadruples, because F depends on v²: 2² = 4 times as much.

  3. A satellite orbits Earth. What supplies its centripetal force?
    Show answer

    Gravity — Earth's gravitational pull acts toward the centre of the orbit.

Frequently asked questions

What is the difference between centripetal and centrifugal force?

Centripetal force is the real inward force that keeps an object turning. Centrifugal force is only an apparent outward effect felt in a rotating frame, not a real force.

Does the centripetal force do work?

No. It acts at right angles to the motion, so it changes direction but not speed, and does no work.