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: , where runs from the axis to the point where the force acts and is the angle between 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, . Rotational inertia, , grows with the square of distance, so mass far from the axis matters most. A common error is measuring 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
- The rope pulls along the tangent, perpendicular to the radius, so τ = rF = (0.40)(33) = 13.20 N·m.
- = 13.20 ÷ 0.99 = 13.3 rad/s².
Answer: 13.3