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Rotational Motion: Torque, Moment of Inertia and Angular Momentum

Physics Grade 10 Difficulty 2/5

Beginning of the lesson

A rotating turntable with movable masses, a tangential force, torque and the correct relations tau equals I alpha and L equals I omega
Torque changes rotation, while mass distribution controls moment of inertia and angular momentum.

Rotational motion

Rotation has its own position, velocity, acceleration, inertia, force effect and momentum. Each has a direct connection to linear motion.

Learning goals: use radians and angular variables; calculate torque and moment of inertia; apply τnet = Iα; explain angular-momentum conservation; calculate rotational kinetic energy.

1. Angular description

Angular displacement θ is measured in radians, with one revolution equal to 2π rad. Angular velocity is ω = Δθ/Δt and angular acceleration is α = Δω/Δt. For a point at radius r, arc length s = rθ, tangential speed v = rω, and tangential acceleration at = rα. Points on one rigid body share ω but have different tangential speeds when their radii differ.

2. Torque and rotational inertia

A force turns most effectively when perpendicular to the radius: τ = rF sin θ. The rotational form of Newton's second law is Στ = Iα. Moment of inertia I measures resistance to angular acceleration and depends on how mass is distributed relative to the axis. For point masses, I = Σmr²; moving the same mass outward increases I strongly because radius is squared.

rFω
A tangential force produces torque about the central axis.

3. Angular momentum and energy

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