Practice

Torque and rotational dynamics

Torque from a force at an angle, rotational inertia of point masses, balancing a seesaw, and angular acceleration from net torque.

The skill

Torque measures how effectively a force turns something: τ=rFsin⁡θ, where r runs from the axis to the point where the force acts and θ is the angle between r and the force. A force pointed along the radius makes no torque. Give each torque a sign for clockwise or counterclockwise; if they add to zero the system is in rotational equilibrium, and if not, α=τnet/I. Rotational inertia, I=∑mr2, grows with the square of distance, so mass far from the axis matters most. A common error is measuring r from the end of the object instead of from the axis.

A worked example

A wheel has rotational inertia 0.99 kg·m² about its axle, and friction at the axle is negligible. A rope wrapped around the wheel at radius 0.40 m is pulled with a constant tangential force of 33 N.

What is the wheel's angular acceleration, in rad/s²? Give your answer to three significant figures.

Solution

  1. The rope pulls along the tangent, perpendicular to the radius, so τ = rF = (0.40)(33) = 13.20 N·m.
  2. αsys=τnet/Isys = 13.20 ÷ 0.99 = 13.3 rad/s².

Answer: 13.3

Your turn

Lessons behind these problems