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Physics · Ch 5 — Motion of System of Particles and Rigid Bodies

Work Done by Torque

5.5.3

Work Done by Torque

Consider a rigid body rotating about a fixed axis perpendicular to the page, and a point PP on the body acted on by a tangential force FF. As the body rotates, PP undergoes a small displacement dsds along its circular arc, and the work done by the force over this small displacement is, as in ordinary translational motion,

dW=F ds.dW=F\,ds.

The small arc length dsds, the corresponding small angle of rotation dθd\theta, and the radius rr (the distance of PP from the axis) are related by the standard geometric relation ds=r dθds=r\,d\theta. Substituting:

dW=F(r dθ)=(Fr) dθ.dW=F(r\,d\theta)=(Fr)\,d\theta.

The quantity FrFr is exactly the torque τ\tau produced by the force about the axis, so

dW=τ dθ.dW=\tau\,d\theta. …

Figure 5.29Work done by torque

What this figure shows. A point P on a rigid body rotates about a fixed axis perpendicular to the page; a tangential force F acts on P and produces a small displacement ds along the circular arc, corresponding to a small angle of rotation dθ, the geometric relation ds = r dθ that is used to convert the elementary work F ds into the …