Spin: Angular Velocity, Center of Mass and Inertia
A gust catches one end of the long gangplank as the crew carries it aboard, and the plank swings round. Push a crate squarely in the middle, though, and it just slides. Where a force lands decides whether a body spins, and how its mass is spread out decides how easily.
The rule
Push through the center: it slides. Push off-center: it spins too.
Angular velocity (omega) is how fast a body turns, in radians per second. In 2D it is a single number, positive for counter-clockwise. It updates exactly like position: angle += omega * dt.
The center of mass is the mass-weighted average position of a body, and it's the point the body naturally spins about. A 15 kg crate at strapped to a 5 kg anchor at has its center of mass at .
A force applied at an offset from the center of mass creates a torque, which in 2D is
A force aimed straight through the center of mass has zero torque: it only slides the body. An off-center force slides it and spins it.
The moment of inertia plays the part of mass for turning: angular acceleration = . It grows with the mass and with the square of how far that mass sits from the center. For a thin plank of mass and length , turning about its middle, . Double the length and it becomes four times harder to spin.
The shortcut
Only the sideways part of a push, times its distance from the center, makes spin. After that, treat turning exactly like moving: torque ÷ I gives angular acceleration, just as force ÷ mass gives acceleration.
Offset and force
The push lands on the plank's end, r = (1, 0) from the center. The wind pushes up: F = (0, 10) N.
The trap is measuring from the wrong point, such as the plank's end or the world origin. Torque that drives spin is always measured from the center of mass.
Drills
Answer fast — trust the rule.
A 15 kg crate at x = 0 is strapped to a 5 kg anchor at x = 2. Where is the center of mass?
A push points straight through a crate's center of mass. What happens?
Two planks have the same mass, but one is twice as long. How does its moment of inertia compare?
Remember
- Angular velocity updates like position: angle += omega × dt.
- Torque = the sideways part of a push times its distance from the center of mass; a push through the center makes no spin.
- Angular acceleration = torque ÷ I, and I grows with the square of distance, so long things are slow to spin.
