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Cross Product Properties

Properties

Let u, v, wR3\vec{u},\ \vec{v},\ \vec{w} \in \reals^3 be vectors.
Let cRc \in \reals be a scalar.
  • u ×v=(v×u)\vec{u}\ \times\vec{v}=-\left(\vec{v}\times\vec{u}\right)
  • c(u×v)  =  (cu)×v  =  u×(cv)c\left(\vec{u}\times\vec{v}\right) \ \ =\ \ \left(c\vec{u}\right)\times\vec{v} \ \ =\ \ \vec{u}\times\left(c\vec{v}\right)
  • u×(v+w) = u×v + u×w\vec{u}\times\left(\vec{v}+\vec{w}\right)\ =\ \vec{u}\times\vec{v}\ +\ \vec{u}\times\vec{w}
  • (u+v)×w = u×w + v×w\left(\vec{u}+\vec{v}\right)\times\vec{w} \ =\ \vec{u}\times\vec{w}\ +\ \vec{v}\times\vec{w}
  • v×v=0\vec{v}\times\vec{v}=\vec{0}
  • v×0=0\vec{v}\times\vec{0}=\vec{0}
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Cross Product and Angles

Like the dot product, there is another formula for the cross product involving the angle between vectors.
For vectors u, vR3\vec u, \ \vec v \in \reals^3 and angle θ\theta between u\vec u and v\vec v:
u×v=uvsinθ\boxed{\quad \lVert \vec{u} \times \vec{v} \rVert = \lVert\vec{u} \rVert \lVert \vec{v} \rVert \sin\theta \quad}

Watch Out!
Don't forget to take the norm on the LHS!
This is a scalar equation, just like the similar dot product formula: uv=uvcosθ\vec u \cdot \vec v = \lVert \vec u \rVert \lVert \vec v \rVert \cos \theta

Note
If u×v=0\vec u \times \vec v = \vec 0 then u\vec u and v\vec v are parallel (or one of the vectors is 0\vec 0)

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Example: Cross Product and Angles

Given a=4, b=3\lVert \vec a \rVert = 4, \ \lVert \vec b \rVert = 3 and b×a=6\lVert \vec b \times \vec a \rVert = 6, what is the angle between a\vec a and b\vec b?
Recall the formula involving the cross product and angle and rearrange:
a×b=absinθ(b×a)ab=sinθ1 b×aab=sinθ6(4)(3)=sinθ12=sinθ\begin{aligned} \lVert \vec{a} \times \vec{b} \rVert &=\lVert\vec{a} \rVert \lVert \vec{b} \rVert \sin\theta\\[0.5em] \dfrac{\lVert -(\vec{b} \times \vec{a}) \rVert}{\lVert\vec{a} \rVert \lVert \vec{b} \rVert} &= \sin\theta\\[1em] \dfrac{\lvert -1 \rvert\ \lVert \vec{b} \times \vec{a} \rVert}{\lVert\vec{a} \rVert \lVert \vec{b} \rVert} &= \sin\theta\\[1em] \dfrac{6}{(4)(3)} &= \sin\theta\\ \dfrac{1}{2} &= \sin\theta\\ \end{aligned}



Based on the special triangle: θ=π6\boxed{\theta = \dfrac{\pi}{6}}

Note: By the CAST rule, sin\sin is also positive in the 2nd quadrant (top-left), so there is another possible answer found there.

Quadrant 2 contains angles between π2\frac{\pi}{2} and π\pi. Take our "basic" solution and subtract it from π\pi to get the alternative answer:

ππ6 = 5π6\pi-\frac{\pi}{6}\ =\ \boxed{\frac{5\pi}{6}}
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Example: Cross Product Properties

Given that u×v=[k240k+2]\vec u \times \vec v= \begin{bmatrix} k^2-4\\ 0\\ \sqrt{k+2}\\ \end{bmatrix} , determine the value(s) of kk such that u\vec u and v\vec v are collinear.
The vectors are collinear/parallel if the cross product is the zero vector:
u×v=0[k240k+2]=[000]\begin{aligned} \vec u \times \vec v &= \vec 0\\[0.5em] \begin{bmatrix} k^2-4\\ 0\\ \sqrt{k+2}\\ \end{bmatrix} &= \begin{bmatrix} 0\\ 0\\ 0\\ \end{bmatrix} \end{aligned}
Equation 1:
k24=0k2=4k=±2\begin{aligned} k^2 - 4 &= 0\\ k^2 &= 4\\ k &= \pm 2 \end{aligned}
Equation 2:
k+2=0k+2=0k=2\begin{aligned} \sqrt{k+2} &= 0\\ k+2 &= 0\\ k &= -2 \end{aligned} (no new information)

Equation 3:
k+2=0k+2=0k=2\begin{aligned} \sqrt{k+2} &= 0\\ k+2 &= 0\\ k &= -2 \end{aligned}

Therefore only k=2\boxed{k=-2} will ensure that all components are zero.
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Practice: Cross Product Properties

Use the cross product and dot product properties to prove:
u×v2+(uv)2=u2v2{\lVert \vec u \times \vec v \rVert}^2 + (\vec u \cdot \vec v)^2 = {\lVert \vec u \rVert}^2 {\lVert \vec v \rVert}^2

Practice: Cross Product Properties

Let u, v, wR3\vec u ,\ \vec{v} ,\ \vec w \in \reals^3 be vectors.
Let c, dRc,\ d \in \reals be scalars.

Select all of the following that produce a vector.
Extra Practice