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3.16 The vector productIB Maths: Analysis and Approaches HL: Revision notes

Section 1

What is the vector product?

The vector product (or cross product) of two vectors v\mathbf{v} and w\mathbf{w} is a vector, defined by v×w=∣v∣∣w∣sin⁡θ n,\mathbf{v}\times\mathbf{w} = |\mathbf{v}||\mathbf{w}|\sin\theta\,\mathbf{n}, where θ\theta is the angle between v\mathbf{v} and w\mathbf{w} (0≤θ≤π0 \le \theta \le \pi) and n\mathbf{n} is a unit vector perpendicular to both v\mathbf{v} and w\mathbf{w}. The direction of n\mathbf{n} is given by the right-hand screw rule: turn a screw from v\mathbf{v} towards w\mathbf{w} and it moves in the direction of n\mathbf{n}.

So v×w\mathbf{v}\times\mathbf{w} is perpendicular to both vectors, which is why it is so useful for finding normals to planes. Compare the scalar product v⋅w=∣v∣∣w∣cos⁡θ\mathbf{v}\cdot\mathbf{w} = |\mathbf{v}||\mathbf{w}|\cos\theta, which is a number.

Key termsvector productright-hand screw ruleunit normal
Exam tip

i×j=k\mathbf{i}\times\mathbf{j} = \mathbf{k}, j×k=i\mathbf{j}\times\mathbf{k} = \mathbf{i}, k×i=j\mathbf{k}\times\mathbf{i} = \mathbf{j}. Going the other way round the cycle gives a minus sign, e.g. j×i=−k\mathbf{j}\times\mathbf{i} = -\mathbf{k}.

Section 2

How do we calculate it from components?

The formula booklet gives v×w=(v2w3−v3w2v3w1−v1w3v1w2−v2w1).\mathbf{v}\times\mathbf{w} = \begin{pmatrix} v_2w_3 - v_3w_2 \\ v_3w_1 - v_1w_3 \\ v_1w_2 - v_2w_1 \end{pmatrix}. Many students prefer the determinant layout: put i,j,k\mathbf{i}, \mathbf{j}, \mathbf{k} in the top row, v\mathbf{v} in the second and w\mathbf{w} in the third, then expand, remembering the minus sign on the j\mathbf{j} term.

Example: u=2i−j+3k\mathbf{u} = 2\mathbf{i} - \mathbf{j} + 3\mathbf{k}, v=i+4j−2k\mathbf{v} = \mathbf{i} + 4\mathbf{j} - 2\mathbf{k} gives u×v=(2−12)i+(3+4)j+(8+1)k=−10i+7j+9k.\mathbf{u}\times\mathbf{v} = (2 - 12)\mathbf{i} + (3 + 4)\mathbf{j} + (8 + 1)\mathbf{k} = -10\mathbf{i} + 7\mathbf{j} + 9\mathbf{k}. Check with the scalar product: (−10)(2)+(7)(−1)+(9)(3)=0(-10)(2) + (7)(-1) + (9)(3) = 0, so the answer is perpendicular to u\mathbf{u}, as it must be.

Key termsdeterminant method
Common mistake

Forgetting to negate the j\mathbf{j}-component. The middle component is v3w1−v1w3v_3w_1 - v_1w_3, not v1w3−v3w1v_1w_3 - v_3w_1.

Exam tip

Always check your answer is perpendicular to both vectors by dotting: both scalar products must be 0.

Section 3

Which algebraic rules does it obey?

  • Anti-commutative: v×w=−w×v\mathbf{v}\times\mathbf{w} = -\mathbf{w}\times\mathbf{v}. Order matters.
  • Distributive: u×(v+w)=u×v+u×w\mathbf{u}\times(\mathbf{v}+\mathbf{w}) = \mathbf{u}\times\mathbf{v} + \mathbf{u}\times\mathbf{w}.
  • Scalars come out: (kv)×w=k(v×w)(k\mathbf{v})\times\mathbf{w} = k(\mathbf{v}\times\mathbf{w}).
  • v×v=0\mathbf{v}\times\mathbf{v} = \mathbf{0}, because sin⁡0=0\sin 0 = 0.
  • For non-zero vectors, v×w=0\mathbf{v}\times\mathbf{w} = \mathbf{0} exactly when v\mathbf{v} and w\mathbf{w} are parallel.

Example: (a+b)×(a−b)=a×a−a×b+b×a−b×b=−2(a×b)(\mathbf{a}+\mathbf{b})\times(\mathbf{a}-\mathbf{b}) = \mathbf{a}\times\mathbf{a} - \mathbf{a}\times\mathbf{b} + \mathbf{b}\times\mathbf{a} - \mathbf{b}\times\mathbf{b} = -2(\mathbf{a}\times\mathbf{b}).

Key termsanti-commutativeparallel test
Common mistake

Expanding brackets as if the product were commutative. b×a\mathbf{b}\times\mathbf{a} does not cancel with −a×b-\mathbf{a}\times\mathbf{b}; it equals it.

Section 4

What does the magnitude measure?

∣v×w∣=∣v∣∣w∣sin⁡θ|\mathbf{v}\times\mathbf{w}| = |\mathbf{v}||\mathbf{w}|\sin\theta is the area of the parallelogram with sides v\mathbf{v} and w\mathbf{w} (base ∣v∣|\mathbf{v}|, height ∣w∣sin⁡θ|\mathbf{w}|\sin\theta). The triangle with the same two sides has half this area: area of triangle ABC=12∣AB→×AC→∣.\text{area of triangle ABC} = \tfrac{1}{2}|\overrightarrow{AB}\times\overrightarrow{AC}|. Because area =12×= \frac{1}{2}\times base ×\times height, you can also find the perpendicular distance from C to the line AB: h=∣AB→×AC→∣∣AB→∣h = \dfrac{|\overrightarrow{AB}\times\overrightarrow{AC}|}{|\overrightarrow{AB}|}.

Example: for A(1,0,2)(1,0,2), B(5,4,4)(5,4,4), C(−2,4,3)(-2,4,3), AB→×AC→=−4i−10j+28k\overrightarrow{AB}\times\overrightarrow{AC} = -4\mathbf{i} - 10\mathbf{j} + 28\mathbf{k} with magnitude 30, so the triangle has area 15 and C is 30÷6=530 \div 6 = 5 units from AB.

Key termsparallelogram areatriangle area
Common mistake

Using position vectors instead of side vectors. For triangle ABC you need AB→\overrightarrow{AB} and AC→\overrightarrow{AC}, not OB→\overrightarrow{OB} and OC→\overrightarrow{OC} (unless one vertex is the origin).

Section 5

Using the vector and scalar products together

Since ∣v×w∣=∣v∣∣w∣sin⁡θ|\mathbf{v}\times\mathbf{w}| = |\mathbf{v}||\mathbf{w}|\sin\theta and v⋅w=∣v∣∣w∣cos⁡θ\mathbf{v}\cdot\mathbf{w} = |\mathbf{v}||\mathbf{w}|\cos\theta, dividing gives tan⁡θ=∣v×w∣v⋅w.\tan\theta = \frac{|\mathbf{v}\times\mathbf{w}|}{\mathbf{v}\cdot\mathbf{w}}. For example, if a×b=2i−3j+6k\mathbf{a}\times\mathbf{b} = 2\mathbf{i} - 3\mathbf{j} + 6\mathbf{k} and a⋅b=12\mathbf{a}\cdot\mathbf{b} = 12, then ∣a×b∣=7|\mathbf{a}\times\mathbf{b}| = 7 and tan⁡θ=712\tan\theta = \frac{7}{12}.

To find an angle from vectors alone, the scalar product is safer: sin⁡θ\sin\theta cannot tell an acute angle from its obtuse partner, because ∣v×w∣≥0|\mathbf{v}\times\mathbf{w}| \ge 0 always.

Exam tip

The sign of v⋅w\mathbf{v}\cdot\mathbf{w} tells you whether θ\theta is acute (positive) or obtuse (negative).

Must know

  • v×w=∣v∣∣w∣sin⁡θ n\mathbf{v}\times\mathbf{w} = |\mathbf{v}||\mathbf{w}|\sin\theta\,\mathbf{n} is a vector perpendicular to both; direction by the right-hand screw rule.
  • Compute from components (formula booklet); check by dotting with each vector.
  • v×w=−w×v\mathbf{v}\times\mathbf{w} = -\mathbf{w}\times\mathbf{v}; distributive; scalars come out; v×v=0\mathbf{v}\times\mathbf{v} = \mathbf{0}.
  • Non-zero vectors are parallel if and only if their vector product is 0\mathbf{0}.
  • Parallelogram area =∣v×w∣= |\mathbf{v}\times\mathbf{w}|; triangle area =12∣v×w∣= \frac{1}{2}|\mathbf{v}\times\mathbf{w}|.

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