Interactive Lecture
Understanding Angular Motion and Centripetal Forces
by Dr Arnaldo Delli Carri
Angular velocity (\(\omega\)) represents the rate of change of angular displacement. It describes how quickly an object rotates about a fixed axis.
When an object moves in a circle at constant speed, it experiences centripetal acceleration directed towards the centre. Despite constant speed, the velocity vector continuously changes direction.
For a bead whirled on a string, the string tension \(T\) is the centripetal force: \(T = F_c = m\omega^2 r\).
The equations of angular motion parallel those of linear motion, with angular quantities replacing linear ones:
| Linear Motion | Angular Motion | Relationship |
|---|---|---|
| \(v = u + at\) | \(\omega = \omega_0 + \alpha t\) | \(v = r\omega\) |
| \(s = ut + \frac{1}{2}at^2\) | \(\theta = \omega_0 t + \frac{1}{2}\alpha t^2\) | \(s = r\theta\) |
| \(v^2 = u^2 + 2as\) | \(\omega^2 = \omega_0^2 + 2\alpha\theta\) | \(a_t = r\alpha\) |
| \(s = \frac{1}{2}(u + v)t\) | \(\theta = \frac{1}{2}(\omega_0 + \omega)t\) | - |
Angular acceleration (\(\alpha\)) is the rate of change of angular velocity. It describes how quickly the rotation speed changes.
When angular velocity changes, the object experiences both centripetal and tangential accelerations:
Circular motion governs the behaviour of these engineering systems:
| Concept | Equation | Description |
|---|---|---|
| Linear-Angular Relationship | \(v = r\omega\) | Linear speed from angular velocity |
| Centripetal Acceleration | \(a_c = \frac{v^2}{r} = \omega^2 r\) | Acceleration towards centre of circle |
| Centripetal Force | \(F_c = \frac{mv^2}{r} = m\omega^2 r\) | Force required for circular motion |
| Tangential Acceleration | \(a_t = r\alpha\) | Tangential component (non-uniform motion) |
| Total Acceleration | \(a_{total} = \sqrt{a_c^2 + a_t^2}\) | Magnitude of resultant acceleration |
| Angular Kinematics | \(\omega = \omega_0 + \alpha t\) \(\theta = \omega_0 t + \frac{1}{2}\alpha t^2\) \(\omega^2 = \omega_0^2 + 2\alpha\theta\) |
Equations for angular motion (analogous to linear) |
A bead of mass 50 g is attached to a string of length 0.8 m and rotates in a horizontal circle at a constant angular velocity of 5 rad/s. Calculate:
Show Solution
Given: \(m = 0.05\) kg, \(r = 0.8\) m, \(\omega = 5\) rad/s
a) Linear speed:
\(v = r\omega = 0.8 \times 5 = 4\) m/s
b) Centripetal acceleration:
\(a_c = \omega^2 r = 5^2 \times 0.8 = 25 \times 0.8 = 20\) m/s²
c) Tension (Centripetal force):
\(T = F_c = ma_c = 0.05 \times 20 = 1.0\) N
Answer: \(v = 4\) m/s, \(a_c = 20\) m/s², \(T = 1.0\) N
A wheel starts from rest and accelerates uniformly to 120 rpm in 4 seconds. Find:
Show Solution
Given: \(\omega_0 = 0\), \(\omega = 120\) rpm \(= 120 \times \frac{2\pi}{60} = 4\pi\) rad/s, \(t = 4\) s, \(r = 0.3\) m
a) Angular acceleration:
\(\alpha = \frac{\omega - \omega_0}{t} = \frac{4\pi}{4} = \pi\) rad/s² \(\approx 3.14\) rad/s²
b) Angular displacement:
\(\theta = \omega_0 t + \frac{1}{2}\alpha t^2 = 0 + \frac{1}{2} \times \pi \times 16 = 8\pi\) rad
Number of revolutions \(= \frac{8\pi}{2\pi} = 4\) revolutions
c) Tangential acceleration:
\(a_t = r\alpha = 0.3 \times \pi \approx 0.942\) m/s²
Answer: \(\alpha = \pi \approx 3.14\) rad/s², 4 revolutions, \(a_t \approx 0.942\) m/s²
A particle moves in a circle of radius 2 m with an angular velocity that increases from 2 rad/s to 6 rad/s over a distance of \(4\pi\) radians. Calculate:
Show Solution
Given: \(r = 2\) m, \(\omega_0 = 2\) rad/s, \(\omega = 6\) rad/s, \(\theta = 4\pi\) rad
a) Angular acceleration:
Using \(\omega^2 = \omega_0^2 + 2\alpha\theta\)
\(36 = 4 + 2\alpha(4\pi)\)
\(32 = 8\pi\alpha\)
\(\alpha = \frac{4}{\pi} \approx 1.27\) rad/s²
b) Time taken:
\(\omega = \omega_0 + \alpha t\)
\(6 = 2 + \frac{4}{\pi}t\)
\(t = \frac{4\pi}{4} = \pi \approx 3.14\) s
c) Total acceleration at \(\omega = 4\) rad/s:
\(a_c = \omega^2 r = 16 \times 2 = 32\) m/s²
\(a_t = r\alpha = 2 \times \frac{4}{\pi} \approx 2.55\) m/s²
\(a_{total} = \sqrt{32^2 + 2.55^2} \approx 32.1\) m/s²
Answer: \(\alpha = \frac{4}{\pi} \approx 1.27\) rad/s², \(t = \pi \approx 3.14\) s, \(a_{total} \approx 32.1\) m/s²