Figure 8-19c shows another way to calculate the magnitude of the torque for the situation in Figure 8-19a. As this figure shows, the \(\textbf{line of action}\) of the force is just an extension of the force vector \(\vec{F}\) through the point where the force is applied. The \(\textbf{lever arm}\) of the force (also called the \(\textit{moment arm}\)) is the perpendicular distance from the rotation axis to the line of action of the force, which is why we denote it by the symbol \(r_\perp\) (\(\perp\) is mathematical shorthand for “perpendicular”). Trigonometry shows that the lever arm \(r_\perp\) equals \(r \sin{\phi}\), the same quantity that appears in Equation 8-18. Hence we can rewrite that equation as: