Until now, you have worked with forces and work to explain and predict object motion. You've even used work and energy to begin to explain that objects can rotate, but you haven't yet unpacked how that occurs – only that a system can share energy between translation and rotation. In these notes, you will read about torque, which is a force applied at a distance from a specific point that causes a twisting or rotating about that point.

Torque is a vector quantity that describes how you can change the rotation of an object. Specifically, the torque about a point A is the vector (cross) product of the vector that points from A to the point where the force is applied and the force itself. That's a mouthful, but you can think about it in terms of the figure to the right.

Consider a bolt that is located at A in the figure to the right. You attach a wrench to location A and push on the end of the wrench with the force indicated. The vector that points from A to the end of the wrench where the force is applied is $\vec{r}_A$. This distance is often called the “lever arm.” It indicates the point of application of the force relative to the rotation axis.

In this situation, the force that you apply to the end of the wrench is not “100% effective” because only the component of the force applied perpendicular to the lever arm contributes to the rotation of the bolt. In any event, the bolt will rotate in a counter-clockwise manner as the end of the wrench moves around the dotted circle. The torque that is applied is related to the lever arm and the applied force by the cross product.

$$\vec{\tau}_{A} = \vec{r}_A \times \vec{F}$$

The torque is a vector; it has both a magnitude and direction. This is the first physical quantity that you have seen that seen that depends on the cross (vector) product between two vectors. It's worth taking some time to understand how this mathematics works.

The magnitude of the the torque depends on the component of the force that is perpendicular to the lever arm. In the figure above, the perpendicular component of the force is given by,

$$F_{\perp} = F\sin\theta$$

So that the magnitude of the torque around location A is given by,

$$\left|\vec{\tau}_{A}\right| = \left|\vec{r}_A \times \vec{F}\right| = r_{A} F\sin\theta$$

This mathematical relationship holds for any cross product. The magnitude of a general cross product is the product of the magnitudes of the vectors multiplied by the sine of the angle between them.

$$\left|\vec{B} \times \vec{C}\right| = \left|\vec{B}\right|\left|\vec{C}\right|\sin \theta_{BC}$$

So, as shown in the figure to the right, the torque is only due to the component of the force that is perpendicular to the lever arm ($F_{\perp}$).

Torque is a vector quantity; it has a direction. How can you determine that direction? In general, this is done mathematically by taking the determinant of a special matrix, which you might have seen in other mathematics courses. For most purposes, you will consider motion in the plane (e.g., $x-y$ plane). This is a bit easier to think about than cross products in general ¹⁾. If the lever arm ($\vec{r}_A$) and the applied force ($\vec{F}$) live in the $x-y$ plane, the torque points in the $z$-direction (either + or -).

Here's the proof of that. Consider a lever arm in the $x-y$ plane that locates a force with respect to some rotation axis: $\vec{r}_A = \langle r_x, r_y, 0\rangle$ and a force that similar lives in the $x-y$ plane: $\vec{F} = \langle F_x, F_y, 0\rangle$. You want to take the cross product to find the torque:

$$\vec{\tau}_{A} = \vec{r}_A \times \vec{F} = det\begin{vmatrix} \hat{x} & \hat{y} & \hat{z} \\ r_x & r_y & 0 \\ F_x & F_y & 0 \\ \end{vmatrix} $$

Taking the cross product as described in these notes:

$$\vec{\tau}_A = \left(r_y(0)-0(F_y)\right)\hat{x} - \left(r_x(0)-0(F_x)\right)\hat{y} + \left(r_xF_y-r_yF_x\right)\hat{z} = \left(r_xF_y-r_yF_x\right)\hat{z} $$

$$\vec{\tau}_A = \langle 0,0,r_xF_y-r_yF_x\rangle$$

When working with forces and lever arms that exist is a plane (e.g., $x-y$ plane), the torque always points in the $z$-direction. So, it becomes useful to think about the torque as having a sign, either + or - depending on whether in points in the $+z$ or $-z$ direction. The “right-hand rule” is helpful to think about this.

To use this rule point your fingers in the direction of the