\(\def \u#1{\,\mathrm{#1}}\) \(\def \abs#1{\left|#1\right|}\) \(\def \ast{*}\) \(\def \deg{^{\circ}}\) \(\def \tau{\uptau}\) \(\def \ten#1{\times 10^{#1}}\) \(\def \redcancel#1{{\color{red}\cancel{#1}}}\) \(\def \BLUE#1{{\color{blue} #1}}\) \(\def \RED#1{{\color{red} #1}}\) \(\def \PURPLE#1{{\color{purple} #1}}\) \(\def \th#1,#2{#1,\!#2}\) \(\def \lshift#1#2{\underset{\Leftarrow\atop{#2}}#1}}\) \(\def \rshift#1#2{\underset{\Rightarrow\atop{#2}}#1}}\) \(\def \dotspot{{\color{lightgray}{\circ}}}\) \(\def \ccw{\circlearrowleft}\) \(\def \cw{\circlearrowright}\)
Chapter 1: Equilibrium
23. (Problem Solving)

Calculating Torque

There are two other ways we can write this equation, if the two vectors are not perpendicular. First, we can write $$\tau=rF_\perp$$ where \(F_\perp\) is the component of the force which is perpendicular to the lever arm. A little trig will show us that \(F_\perp=F\sin\theta\), which is where this equation comes from.

We can also write $$\tau=r_\perp F$$ where \(r_\perp\) is the component of the lever arm that is perpendicular to the force. (This quantity \(r_\perp\) is sometimes called the moment arm, but we will avoid this term to avoid confusion with the lever arm \(\vec r\).)