Week 3 Discussion Notes

Table of Contents

Cross Product

While it might look like a random definition, the cross product is the "best" way to find a vector perpendicular to two vectors. Geometrically, the cross product looks like the following:

The direction of v×w\vec{v} \times \vec{w} is determined by the right-hand rule, like the axes. If you look at the picture, you'll see that order matters! v×w\vec{v} \times \vec{w} and w×v\vec{w} \times \vec{v} point in opposite directions, and you can check that the directions are consistent with the right-hand rule.

Algebraically, you can calculate the cross product with the following determinant formula:

v×w=i^j^k^v1v2v3w1w2w3=v2v3w2w3i^v1v3w1w3j^+v1v2w1w2k^=(v2w3v3w2)i^(v1w3v3w1)j^+(v1w2v2w1)k^.\begin{aligned} \vec{v} \times \vec{w} &= \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ v_1 & v_2 & v_3 \\ w_1 & w_2 & w_3 \end{vmatrix} \\ &= \begin{vmatrix} v_2 & v_3 \\ w_2 & w_3 \end{vmatrix} \hat{i} - \begin{vmatrix} v_1 & v_3 \\ w_1 & w_3 \end{vmatrix} \hat{j} + \begin{vmatrix} v_1 & v_2 \\ w_1 & w_2 \end{vmatrix} \hat{k} \\ &= \p{v_2w_3 - v_3w_2} \hat{i} - \p{v_1w_3 - v_3w_1} \hat{j} + \p{v_1w_2 - v_2w_1} \hat{k}. \end{aligned}

Notice that there is an additional minus sign when calculating the j^\hat{j}-coordinate. Lastly, on #6 of this week's worksheet, you will show that the length of v×w\vec{v} \times \vec{w} is the area of parallelogram spanned by v\vec{v} and w\vec{w}:

The area of the parallelogram is the height (wsinθ\norm{\vec{w}} \sin\theta) times the base length (v\norm{\vec{v}}), which is what #6 tells you:

v×w=vwsinθ,\norm{\vec{v} \times \vec{w}} = \norm{\vec{v}} \norm{\vec{w}} \sin\theta,

where θ\theta is the angle between v\vec{v} and w\vec{w} measured in the interval [0,π]\br{0, \pi} (or [0,180]\br{0^\circ, 180^\circ} in degrees).

Triple Product

I made a GeoGebra graph to help show why u(v×w)=0\vec{u} \cdot \p{\vec{v} \times \vec{w}} = 0 tells you that u,v,w\vec{u}, \vec{v}, \vec{w} are coplanar.