Angular Displacement (\theta)
- Definition
- Measures the angle through which an object moves along a circular path.
- Answers the question “How far around the circle did it go?” in angular terms.
- Unit
- Radian (rad); a dimensionless ratio that relates arc length to radius.
- Core Formulae
- \theta = \frac{s}{r}
- s = arc length (linear distance along the circumference).
- r = radius of the circle.
- Rearranged: s = r\,\theta (useful for converting between linear and angular measures).
- Worked Example
- Given: r = 0.5\,\text{m}, s = 3.14\,\text{m}.
- Compute: \theta = \frac{3.14}{0.5} = 6.28\,\text{rad} (≈ one full revolution).
- Significance & Connections
- Direct bridge between linear (arc length) and rotational motion.
- Radians keep calculus simple (derivatives/integrals of trig functions remain clean).
- One full revolution = 2\pi \text{ rad} \approx 6.283\text{ rad}.
Angular Velocity (\omega)
- Definition
- Rate of change of angular displacement with respect to time.
- Describes “how fast” an object is rotating.
- Units
- Radians per second (rad/s).
- Core Formulae
- Average/angular velocity: \omega = \frac{\theta}{t} (for uniform motion).
- Kinematic form (constant \alpha): \omega = \omega_0 + \alpha t where
- \omega_0 = initial angular velocity,
- \alpha = angular acceleration,
- t = elapsed time.
- Worked Example (Fan)
- Complete revolutions → radians: 10 \text{ rev} = 10\times 2\pi = 20\pi\,\text{rad}.
- Time: t = 20\,\text{s}.
- Compute: \omega = \frac{20\pi}{20} = \pi \approx 3.14\,\text{rad/s}.
- Extra Insights
- Linear tangential speed v relates by v = r\,\omega.
- Direction given by right-hand rule (out of page for CCW rotation).
Angular Acceleration (\alpha)
- Definition
- Rate of change of angular velocity with respect to time.
- Captures how quickly a spinning object speeds up or slows down.
- Units
- Radians per second squared (rad/s$^2$).
- Core Formulae
- Average/angular acceleration: \alpha = \frac{\omega - \omega_0}{t}.
- If \alpha is constant, other rotational kinematic relations mirror linear ones, e.g.
- \theta = \omega_0 t + \tfrac{1}{2}\alpha t^2,
- \omega^2 = \omega_0^2 + 2\alpha \theta.
- Worked Example (Disc)
- Given start from rest: \omega_0 = 0, final \omega = 4\,\text{rad/s}, t=8\,\text{s}.
- Compute: \alpha = \frac{4 - 0}{8} = 0.5\,\text{rad/s}^2.
- Practical Implications
- Positive \alpha → speeding up in the chosen positive direction; negative → slowing down or accelerating in opposite sense.
- Torque (\tau) links via Newton’s 2nd law for rotation: \tau = I\alpha.
Additional Study Connections & Tips
- Always convert revolutions, degrees, or turns to radians before plugging into formulas.
- The rotational kinematic equations are direct analogues of linear motion:
- Linear d=v0 t + \tfrac{1}{2}at^2 ↔ Rotational \theta = \omega0 t + \tfrac{1}{2}\alpha t^2.
- Real-world relevance
- Engineers calculate \omega and \alpha for gears, motors, turbines.
- Medical imaging (MRI) magnets & astrophysics (rotating galaxies) use same principles.
- Ethical & Safety Note
- High \alpha can cause structural failure (e.g.
centrifuge accidents). Engineers must respect material limits (yield stress relates to v = r\omega).
- Memory aids
- “SAR” triangle: \theta (S), r (R), s (A for arc) — cover one to recall \theta = s/r.
- Right-hand rule demos: curl fingers in rotation direction, thumb points along \omega.