to solve problems involving objects moving in a circular path.
Key Concepts
Uniform circular motion: motion at constant speed along a circular path.
Centripetal force: the net force directed towards the centre of the circle that keeps the object in circular motion.
Centripetal acceleration: the acceleration associated with the change in direction of the velocity vector, given by \$a_c = r\omega^{2} = \dfrac{v^{2}}{r}\$.
Angular velocity (\$\omega\$): the rate of change of angular displacement, measured in rad s\(^{-1}\).
Linear speed (\$v\$): the magnitude of the tangential velocity, related to \$\omega\$ by \$v = r\omega\$.
Derivation of the Formulas
Consider an object of mass \$m\$ moving in a circle of radius \$r\$ with constant speed \$v\$.
The change in velocity over a small time \$\Delta t\$ points towards the centre and has magnitude \$\Delta v = v\Delta\theta\$, where \$\Delta\theta = \omega\Delta t\$.
Multiplying by the mass gives the required centripetal force:
\$Fc = m ac = m r \omega^{2}.\$
Using \$v = r\omega\$ we can also write
\$F_c = m\frac{v^{2}}{r}.\$
When to Use Which Form
Use \$F = m r \omega^{2}\$ when the angular speed \$\omega\$ is known or more convenient.
Use \$F = \dfrac{m v^{2}}{r}\$ when the linear speed \$v\$ is given.
Both forms are interchangeable via \$v = r\omega\$.
Variables and Units
Symbol
Quantity
SI Unit
Typical \cdot alues (A‑Level)
\$F\$
Centripetal force
newton (N)
0.1 – 10⁴
\$m\$
Mass of the object
kilogram (kg)
0.01 – 10
\$r\$
Radius of the circular path
metre (m)
0.1 – 5
\$\omega\$
Angular velocity
radian per second (rad s⁻¹)
1 – 100
\$v\$
Linear speed
metre per second (m s⁻¹)
0.5 – 200
\$a_c\$
Centripetal acceleration
metre per second squared (m s⁻²)
0.1 – 10⁴
Worked Example
A 0.50 kg mass is attached to a string and whirled in a horizontal circle of radius 0.75 m at a constant speed of 4.0 m s⁻¹. Find the tension in the string.
Identify the required formula: \$F = \dfrac{m v^{2}}{r}\$ because \$v\$ is given.
Interpretation: The tension in the string must provide a centripetal force of about 11 N (to 2 sf).
Common Mistakes
Confusing centripetal (towards centre) with centrifugal (apparent outward) force.
Using \$v = 2\pi r\$ instead of \$v = r\omega\$ when angular speed is given.
Forgetting to convert revolutions per minute (rpm) to rad s⁻¹: \$\omega = 2\pi \times \text{rpm}/60\$.
Omitting the radius in the denominator of \$F = \dfrac{m v^{2}}{r}\$.
Suggested diagram: A top‑view sketch of an object of mass \$m\$ moving in a circle of radius \$r\$, showing the velocity vector \$v\$ tangent to the path and the centripetal force \$F_c\$ directed towards the centre.