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Angular Displacement, Velocity and Acceleration

Angular velocity is rate of change of angle. Angular acceleration is rate of change of angular velocity.
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Derivation

The need for angular quantities

When a rigid body rotates, every point on it moves in a circle. Different points have different speeds and different accelerations. But one thing is the same for all points: they all rotate through the same angle in the same time.

Angular quantities — angle, angular velocity, angular acceleration — describe this shared rotational behaviour, independent of which point you look at.

Angular displacement θ\theta

Angular displacement is the angle through which a body has rotated from a reference position.

Unit: radian (rad)

One radian is the angle subtended at the centre of a circle by an arc equal in length to the radius.

2π rad=360°    1 rad=180°π57.3°2\pi \text{ rad} = 360° \implies 1 \text{ rad} = \frac{180°}{\pi} \approx 57.3°

Angular displacement is a scalar for small angles but behaves as a vector (along the rotation axis) for finite rotations.

Angular velocity ω\omega

Angular velocity is the rate of change of angular displacement:

ω=dθdt\omega = \frac{d\theta}{dt}

Unit: rad/s

For uniform rotation (constant ω\omega):

ω=θt=2πT=2πf\omega = \frac{\theta}{t} = \frac{2\pi}{T} = 2\pi f

where TT is the period and ff is the frequency.

Direction: By the right-hand rule — curl the fingers of the right hand in the direction of rotation, the thumb points along ω\vec{\omega}.

Angular acceleration α\alpha

Angular acceleration is the rate of change of angular velocity:

α=dωdt=d2θdt2\alpha = \frac{d\omega}{dt} = \frac{d^2\theta}{dt^2}

Unit: rad/s²

Positive α\alpha: angular velocity increasing (speeding up in positive direction) Negative α\alpha: angular velocity decreasing (slowing down, or speeding up in negative direction)

The complete analogy with linear motion

LinearAngular
Displacement xxAngle θ\theta
Velocity v=dxdtv = \frac{dx}{dt}Angular velocity ω=dθdt\omega = \frac{d\theta}{dt}
Acceleration a=dvdta = \frac{dv}{dt}Angular acceleration α=dωdt\alpha = \frac{d\omega}{dt}
Mass mmMoment of inertia II
Force FFTorque τ\tau
Momentum p=mvp = mvAngular momentum L=IωL = I\omega

Every linear quantity has a rotational analogue. Every linear equation has a rotational counterpart.

Instantaneous vs average

Average angular velocity over interval Δt\Delta t:

ωˉ=ΔθΔt\bar{\omega} = \frac{\Delta\theta}{\Delta t}

Instantaneous angular velocity:

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

Same distinction as linear velocity — average over an interval vs value at an instant.

Note
Angles must be in radians for the formulas $v = r\omega$, $a_t = r\alpha$, etc. to give correct SI units. Converting degrees to radians is essential before substituting into any rotational formula.