A skater pulls in her arms and spins faster. A ladder stays at rest against a wall. A disc rolls down a slope and beats a ring. In this course we define angular momentum and use its conservation, we write the two conditions of equilibrium of a rigid body to solve problems on beams and ladders, and we study rolling motion, its kinetic energy and its motion on an inclined plane.
3 lessons, about 1 h 15 min3 simulations12 problems6 practice questionsPython in every lesson
Angular momentum is for a particle, and for a body turning about a fixed axis. Torque is its rate of change: . With no external torque, angular momentum is conserved, so a body that pulls its mass inward spins faster. Its kinetic energy then grows, paid for by the work of pulling in.
A rigid body is in equilibrium when the net external force is zero (no acceleration of the centre of mass) and the net torque about every point is zero (no angular acceleration). In practice: balance the forces along two axes, and take torques about a well-chosen point, often where an unknown force acts. A couple, two equal and opposite forces not along one line, has zero net force but a torque.
Rolling without slipping is moving along at plus turning at : the point touching the ground is at rest, the top moves at . Its kinetic energy is . Down a slope, : a solid ball beats a disc, which beats a ring, whatever their sizes.
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