Physics

2. Circular Motion

Uniform and non-uniform motion in circular paths

Circular Motion

Definitions

Angular Velocity (ω)

  • Rate of change of angular displacement, measured in rad/s

Centripetal Acceleration

  • Acceleration directed toward the center of circular motion, a=v2ra = \frac{v^2}{r}

Centripetal Force

  • Net force directed toward the center that keeps an object in circular motion, F=mv2rF = \frac{mv^2}{r}

 

Derivations

starting with arc length and linear displacement

s=Δθrs = \Delta \theta r s=vΔts = v \Delta t

equating these expressions

vΔt=Δθrv \Delta t = \Delta \theta r

rearranging

vr=ΔθΔt\dfrac{v}{r} = \dfrac{\Delta \theta}{\Delta t}

by definition, angular velocity is the rate of change of angular displacement

ω=ΔθΔt\omega = \dfrac{\Delta \theta}{\Delta t}

taking the limit as Δt0\Delta t \to 0

ω=limΔt0ΔθΔt=dθdt\omega = \lim_{\Delta t \to 0} \dfrac{\Delta \theta}{\Delta t} = \dfrac{d\theta}{dt}

therefore, the relationship between linear and angular velocity is

v=ωrv = \omega r

 

Useful Equations

ω=θt,s=θr,v=ωr\omega = \frac{\theta}{t}, \quad s = \theta r, \quad v = \omega r a=v2r=ω2ra = \frac{v^2}{r} = \omega^2 r F=mv2r=mω2rF = \frac{mv^2}{r} = m\omega^2 r

 

Example 1

A particle moves in a circle of radius 2 m with angular velocity 3 rad/s. What is its linear velocity?

Answer

Using v=ωrv = \omega r

v=3×2=6 m/sv = 3 \times 2 = 6 \text{ m/s}

 

Example 2

A car travels around a circular track of radius 50 m at 20 m/s. What centripetal acceleration does it experience?

Answer

Using a=v2ra = \frac{v^2}{r}

a=20250=40050=8 m/s2a = \frac{20^2}{50} = \frac{400}{50} = 8 \text{ m/s}^2