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Dynamics  ›  Lesson

Spin: Angular Velocity, Center of Mass and Inertia

Angular Velocity 15 minAn off-centre force creates torque about a body's center of mass, and dividing that torque by the moment of inertia gives the angular acceleration that changes its angular velocity.

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 ω\omega (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 x=0x = 0 strapped to a 5 kg anchor at x=2x = 2 has its center of mass at (15×0+5×2)/20=0.5(15 \times 0 + 5 \times 2) / 20 = 0.5.

A force applied at an offset r\mathbf{r} from the center of mass creates a torque, which in 2D is

τ=rxFy−ryFx\tau = r_x F_y - r_y F_x

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 II plays the part of mass for turning: angular acceleration = τ/I\tau / I. It grows with the mass and with the square of how far that mass sits from the center. For a thin plank of mass mm and length LL, turning about its middle, I=mL2/12I = mL^2 / 12. 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.

Wind lifts the end of the 2 m, 6 kg gangplankStep 1 of 5
  1. 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 r\mathbf{r} 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.

The gangplank turns at 3 rad/s. How many radians does it turn in one 0.02 s step?
3×0.02= ?3 \times 0.02 = \,?
quick drill

A 15 kg crate at x = 0 is strapped to a 5 kg anchor at x = 2. Where is the center of mass?

quick drill

A push points straight through a crate's center of mass. What happens?

quick drill

Two planks have the same mass, but one is twice as long. How does its moment of inertia compare?

Torque in 2D is rx × Fy − ry × Fx. What is it for r = (1, 0) and F = (0, −10)?
1×(−10)−0×0= ?1 \times (-10) - 0 \times 0 = \,?

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.

Practice — level up

0/1 solved

Write your answer, then compare it with a rubric and a model answer.

ExplainThe spinning gangplank

Wind pushes 10 N upward on one end of Harbour Hopper's 2 m, 6 kg gangplank. Explain how the physics step turns that push into spin: the torque, the moment of inertia, and the angular velocity after half a second from rest.