What is Centripetal Force & Acceleration?
Any object moving in a circular path requires a centripetal ("center-seeking") force directed inward toward the center of the circle. Without this force, the object would travel in a straight line per Newton's First Law. Centripetal force is not a new type of force — it is always provided by an existing physical force such as gravity (orbits), friction (cars turning), or tension (ball on a string).
Mathematical Foundation
Laws & Principles
- Centripetal ≠ Centrifugal: Centrifugal force is a fictitious (pseudo) force that only appears in the rotating reference frame. In an inertial frame, the only real force is centripetal — always pointing inward. Never draw centrifugal force on a free-body diagram.
- v² Scaling Law: Because velocity is squared, doubling the speed of a car in a turn requires 4× the friction force. This is why highway exit ramp speed limits drop dramatically for tight curves.
- Derived Quantities: Period T = 2πr/v (time for one revolution). Angular velocity ω = v/r (radians per second). g-Force = a_c / 9.80665.
Step-by-Step Example Walkthrough
" A 1,500 kg car takes a curve of radius 50 m at 20 m/s (72 km/h). "
- 1. Calculate centripetal acceleration: a_c = v²/r = (20)²/50 = 400/50 = 8.0 m/s².
- 2. Convert to g-force: 8.0 / 9.81 = 0.82g.
- 3. Calculate centripetal force: F_c = m × a_c = 1500 × 8.0 = 12,000 N.
- 4. Calculate period: T = 2π(50)/20 = 15.7 seconds per revolution.