Illustrated · 1 min

Given two three-dimensional vectors v⃗\vec v and w⃗\vec w, the cross product of v⃗\vec v and w⃗\vec w, denoted by v⃗×w⃗\vec v\times \vec w, is defined as the vector that is perpendicular to both v⃗\vec v and w⃗\vec w, and whose magnitude is ∣v⃗∣∣w⃗∣sin⁡θ|\vec v||\vec w| \sin\theta. Note that the cross product is a vector, not a real number.

Note that there are actually two vectors that satisfy the above condition. In order to maintain a consistent definition, we use the right hand rule: v⃗×w⃗\vec v\times \vec w is the direction your thumb points to if your index finger is v⃗\vec v and middle finger is w⃗\vec w in your right hand.

The cross product satisfies many properties.

  • The cross product is anticommutative: a×b=−(b×a)a\times b=-(b\times a).
  • If two vectors a,ba,b are parallel, then the angle between them is θ=0\theta=0. Thus, sin⁡θ=0\sin\theta=0, so a×b=0a\times b=0.
  • The cross product distributes over addition.
  • The cross product satisfies Jacobi's Identity: a×(b×c)+b×(c×c)+c×(a×b)=0a\times(b\times c)+b\times(c\times c)+c\times(a\times b)=0

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Stub

The 2-D "cross product" is actually better understood in 3-D.

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

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