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Consider three vectors in 3-D space: a⃗=<a1,a2,a3>\vec{a}=<a_1,a_2,a_3>, b⃗=<b1,b2,b3>\vec{b}=<b_1,b_2,b_3>, and c⃗=<c1,c2,c3>\vec{c}=<c_1,c_2,c_3>.

The scalar triple product of a⃗\vec{a}, b⃗\vec{b}, and c⃗\vec{c} is a⃗⋅(b⃗\vec{a}\cdot(\vec{b} x c⃗)\vec{c}). Take note of the fact that this is a scalar, not a vector.

Since the dot product is commutative and the cross product is anticommutative, the scalar triple product does not change in magnitude when one permutes the three vectors. We have the following:

a⃗⋅(b⃗×c⃗)=b⃗⋅(c⃗×a⃗)=c⃗⋅(a⃗×b⃗)\vec{a}\cdot(\vec{b} \times \vec{c})=\vec{b}\cdot(\vec{c} \times \vec{a})=\vec{c}\cdot(\vec{a} \times \vec{b}) c⃗⋅(b⃗×a⃗)=b⃗⋅(a⃗×c⃗)=a⃗⋅(c⃗×b⃗)\vec{c}\cdot(\vec{b} \times \vec{a})=\vec{b}\cdot(\vec{a} \times \vec{c})=\vec{a}\cdot(\vec{c} \times \vec{b})

The two expressions above are opposite in sign as well. Notice that when a⃗\vec{a}, b⃗\vec{b}, and c⃗\vec{c} are cycled, the product stays the same, while when the vector order is flipped, the product changes sign.

Using components, a⃗⋅(b⃗×c⃗)=a1b2c3−a1b3c2+a2b3c1−a2b1c3+a3b1c2−a3b2c1.\vec{a}\cdot(\vec{b} \times \vec{c})=a_1b_2c_3-a_1b_3c_2+a_2b_3c_1-a_2b_1c_3+a_3b_1c_2-a_3b_2c_1. This follows directly from the algebraic definitions of the dot product and the cross product. We can use this formula to verify the above equalities regarding the order of a⃗\vec{a}, b⃗\vec{b}, and c⃗\vec{c}.

Perhaps more interesting is the neat geometric interpretation of the scalar triple product.

We know that b⃗\vec{b} x c⃗\vec{c} produces a vector whose magnitude is equal to the area of the parallelogram determined by b⃗\vec{b} and c⃗\vec{c}. Since b⃗\vec{b} and c⃗\vec{c} determine a plane, let θ\theta denote the angle between a⃗\vec{a} and this plane.

Since b⃗\vec{b} x c⃗\vec{c} is perpendicular to the previously mentioned plane, the angle between a⃗\vec{a} and b⃗\vec{b} x c⃗\vec{c} is 90∘−θ90^{\circ}-\theta.

Computing the scalar triple product, a⃗⋅(b⃗×c⃗)=∣a⃗∣∣b⃗×c⃗∣cos⁡(90∘−θ)=∣a⃗∣∣b⃗×c⃗∣sin⁡θ.\vec{a}\cdot(\vec{b} \times \vec{c})=\left|\vec{a}\right|\left|\vec{b} \times \vec{c}\right|\cos(90^{\circ}-\theta)=\left|\vec{a}\right|\left|\vec{b} \times \vec{c}\right|\sin\theta.

Notice that ∣b⃗×c⃗∣\left|\vec{b} \times \vec{c}\right| is the area of the parallelogram determined by b⃗\vec{b} and c⃗\vec{c}.

Also, the absolute value of ∣a⃗∣sin⁡θ\left|\vec{a}\right|\sin\theta is the height that a⃗\vec{a} reaches above the plane.

Using simple volume calculations, we see that the absolute value of the scalar triple product a⃗⋅(b⃗×c⃗)\vec{a}\cdot(\vec{b} \times \vec{c}) is the volume of the parallelipiped determined by a⃗\vec{a}, b⃗\vec{b}, and c⃗\vec{c}.

Type a concept, like “slope” or “photosynthesis”.

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