recall and use F = mrω2 and F = mv2 / r

Published by Patrick Mutisya · 14 days ago

Cambridge A-Level Physics 9702 – Centripetal Acceleration

Centripetal Acceleration

Learning Objective

Recall and use the equations

\$F = m r \omega^{2}\$

and

\$F = \frac{m v^{2}}{r}\$

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\$.

Thus the average acceleration is

\$a_c = \frac{\Delta v}{\Delta t} = \frac{v\omega\Delta t}{\Delta t}=v\omega = r\omega^{2}.\$

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

SymbolQuantitySI UnitTypical \cdot alues (A‑Level)
\$F\$Centripetal forcenewton (N)0.1 – 10⁴
\$m\$Mass of the objectkilogram (kg)0.01 – 10
\$r\$Radius of the circular pathmetre (m)0.1 – 5
\$\omega\$Angular velocityradian per second (rad s⁻¹)1 – 100
\$v\$Linear speedmetre per second (m s⁻¹)0.5 – 200
\$a_c\$Centripetal accelerationmetre 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.

  1. Identify the required formula: \$F = \dfrac{m v^{2}}{r}\$ because \$v\$ is given.
  2. Substitute the known values:

    \$F = \frac{(0.50\ \text{kg})(4.0\ \text{m s}^{-1})^{2}}{0.75\ \text{m}}\$

  3. Calculate:

    \$F = \frac{0.50 \times 16.0}{0.75} = \frac{8.0}{0.75} \approx 10.7\ \text{N}\$

  4. 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.