Rotational Motion

Explore angular kinematics, torque, rotational inertia, and angular momentum through interactive simulations.

Angular Kinematics

Rotational motion describes objects spinning around an axis. Just as linear motion has position, velocity, and acceleration, rotational motion has angular position (θ), angular velocity (ω), and angular acceleration (α).

Angular Displacement

θ = s / r

where s is arc length and r is radius (measured in radians)

Angular Velocity

ω = Δθ / Δt

Rate of change of angular position (rad/s)

Angular Acceleration

α = Δω / Δt

Rate of change of angular velocity (rad/s²)

Rotational Kinematics Equations

ω = ω₀ + αt
θ = θ₀ + ω₀t + ½αt²
ω² = ω₀² + 2αΔθ

Relationship to Linear Motion

v = rω
a_t = rα
a_c = v² / r = rω²

where a_t is tangential acceleration and a_c is centripetal acceleration

Torque and Rotational Dynamics

Torque is the rotational equivalent of force. It causes angular acceleration and depends on both the magnitude of the force and the distance from the axis of rotation (lever arm).

Torque

τ = r × F = rF sin(θ)

where r is the distance from axis, F is force, and θ is the angle between them

Newton's Second Law for Rotation

τ_net = Iα

where I is rotational inertia (moment of inertia)

Rotational Inertia

I = Σ m_i r_i²

Resistance to rotational acceleration, depends on mass distribution

Common moments of inertia:

• Point mass: I = mr²

• Solid disk/cylinder: I = ½mr²

• Hollow cylinder: I = mr²

• Solid sphere: I = ⅖mr²

• Thin rod (center): I = 1/12 mL²

Rotational Kinetic Energy

KE_rot = ½Iω²

Energy of rotation, analogous to ½mv² for linear motion

Torque Visualizer
Apply forces at different positions and angles to see how torque causes rotation

Torque

7.50 N⋅m

Angular Velocity

0.00 rad/s

Angular Acceleration

0.38 rad/s²

Moment of Inertia

20.00 kg⋅m²

Rotational Inertia Explorer
Compare how different mass distributions affect rotational acceleration

Moment of Inertia

2.500 kg⋅m²

Angular Acceleration

0.80 rad/s²

Angular Velocity

0.00 rad/s

Notice: With the same torque and mass, the disk accelerates fastest (lowest I), the ring accelerates slowest (highest I), and the rod is in between. This demonstrates how mass distribution affects rotational inertia.

Angular Momentum

Angular momentum is the rotational equivalent of linear momentum. It is conserved in the absence of external torques, leading to fascinating phenomena like ice skaters spinning faster when they pull their arms in.

Angular Momentum

L = Iω

For a point mass: L = mvr sin(θ)

Conservation of Angular Momentum

L_initial = L_final
I₁ω₁ = I₂ω₂

When no external torque acts on a system

Torque and Angular Momentum

τ_net = ΔL / Δt

Net torque equals the rate of change of angular momentum

Rolling Motion

KE_total = ½mv² + ½Iω²

Total kinetic energy includes both translational and rotational components

For rolling without slipping: v = rω

Angular Momentum Conservation
Observe how changing rotational inertia affects angular velocity

Start simulation first

Moment of Inertia

12.25 kg⋅m²

Angular Velocity

0.00 rad/s

Angular Momentum

0.00 kg⋅m²/s

Rotational KE

0.00 J

Conservation of Angular Momentum: Notice that angular momentum (shown in green) stays constant at 24.50 kg⋅m²/s even as you change arm extension. When arms pull in (decreasing I), angular velocity increases proportionally. This is why ice skaters spin faster when they pull their arms in!