Classical-Mechanics · Unit 2 · Video 6 · Interactive Practice

Multiplying Vectors Into a New Dimension: The Cross Product

IKey Formulas

Formula Name Description
∣A×B∣=∣A∣ ∣B∣sin⁡θ\lvert \mathbf{A}\times\mathbf{B}\rvert = \lvert\mathbf{A}\rvert\,\lvert\mathbf{B}\rvert\sin\theta Magnitude Equals area of the parallelogram spanned by A\mathbf{A} and B\mathbf{B} (0≤θ≤π0 \le \theta \le \pi)
Right-hand rule Direction Curl fingers from A\mathbf{A} toward B\mathbf{B}; thumb gives A×B\mathbf{A}\times\mathbf{B}, perpendicular to their plane
A×B=− B×A\mathbf{A}\times\mathbf{B} = -\,\mathbf{B}\times\mathbf{A} Anti-commutativity Swapping order flips the sign
(A+B)×C=A×C+B×C(\mathbf{A}+\mathbf{B})\times\mathbf{C} = \mathbf{A}\times\mathbf{C} + \mathbf{B}\times\mathbf{C} Distributive Scalars factor out; product distributes over sums

IIInteractive Visualizations

Visualization 1 — Parallelogram Area

The magnitude ∣A×B∣\lvert\mathbf{A}\times\mathbf{B}\rvert is the area of the parallelogram the two vectors span.

💡 Challenge: double just ∣A∣\lvert\mathbf{A}\rvert and check whether the area doubles too.

Visualization 2 — Direction & the Right-Hand Rule

The product points perpendicular to the plane, and reversing the order flips it to the opposite side.

Visualization 3 — Magnitude Versus Angle

Because the magnitude follows sin⁡θ\sin\theta, it peaks at 90∘90^\circ and vanishes when the vectors line up (∣A∣=∣B∣=1\lvert\mathbf{A}\rvert = \lvert\mathbf{B}\rvert = 1).

💡 The dot product (dashed) follows cos⁡θ\cos\theta — it peaks exactly where the cross product vanishes.

IIIQuiz Questions

Question 1

Two vectors satisfy ∣A∣=3\lvert\mathbf{A}\rvert = 3 and ∣B∣=4\lvert\mathbf{B}\rvert = 4, and the angle between them is θ=90°\theta = 90°.

What is the magnitude ∣A×B∣\lvert\mathbf{A}\times\mathbf{B}\rvert?

✅ Correct! At 90°, sin θ = 1, so the magnitude is 3·4·1 = 12.

❌ Not quite. Apply |A×B| = |A||B|sin θ with sin 90° = 1.

Show solution

Solution:

Use the magnitude formula: ∣A×B∣=∣A∣ ∣B∣sin⁡θ=3⋅4⋅sin⁡90°=12⋅1=12.\lvert\mathbf{A}\times\mathbf{B}\rvert = \lvert\mathbf{A}\rvert\,\lvert\mathbf{B}\rvert\sin\theta = 3 \cdot 4 \cdot \sin 90° = 12 \cdot 1 = 12.

At θ=90°\theta = 90°, sin⁡θ=1\sin\theta = 1, which gives the maximum possible magnitude for these lengths — equal to the area of the rectangle they span.

Question 2

A vector A\mathbf{A} is crossed with another vector that points in the same direction (the two vectors are parallel, θ=0\theta = 0).

What is ∣A×B∣\lvert\mathbf{A}\times\mathbf{B}\rvert?

✅ Correct! Parallel vectors give sin 0 = 0, so the cross product vanishes.

❌ Not quite. The cross product uses sin θ, not cos θ. With θ = 0, sin 0 = 0.

Show solution

Solution:

For parallel vectors θ=0\theta = 0, and sin⁡0=0\sin 0 = 0, so ∣A×B∣=∣A∣ ∣B∣sin⁡0=0.\lvert\mathbf{A}\times\mathbf{B}\rvert = \lvert\mathbf{A}\rvert\,\lvert\mathbf{B}\rvert\sin 0 = 0.

Geometrically the parallelogram collapses to a line with zero area. The common mistake is to use cos⁡θ\cos\theta (that's the dot product) — the cross product uses sin⁡θ\sin\theta, which is zero here. In particular, a vector crossed with itself is always zero.

Question 3

True or False: For any two vectors, A×B=B×A\mathbf{A}\times\mathbf{B} = \mathbf{B}\times\mathbf{A} (the cross product is commutative, just like the dot product).

✅ Correct! The cross product is anti-commutative: A×B = −B×A.

❌ Not quite. Swapping the order flips the direction, so A×B = −B×A.

Show solution

Solution:

The statement is False. The cross product is anti-commutative: A×B=− B×A.\mathbf{A}\times\mathbf{B} = -\,\mathbf{B}\times\mathbf{A}.

Reversing the order makes the right-hand rule arc sweep the opposite way, so your thumb flips to the opposite direction. The magnitude stays the same, but the direction reverses. This is a sharp contrast with the dot product, which is commutative.

Question 4

Given that A×B=C\mathbf{A}\times\mathbf{B} = \mathbf{C}, what is the value of the expression (2A)×B+B×A(2\mathbf{A})\times\mathbf{B} + \mathbf{B}\times\mathbf{A}?

Hint: use the scalar rule and anti-commutativity.

✅ Correct! 2C + (−C) = C, combining the scalar rule and anti-commutativity.

❌ Not quite. (2A)×B = 2C and B×A = −C, so the sum is 2C − C = C.

Show solution

Solution:

Apply the algebraic properties term by term.

Scalar rule: (2A)×B=2(A×B)=2C.(2\mathbf{A})\times\mathbf{B} = 2(\mathbf{A}\times\mathbf{B}) = 2\mathbf{C}.

Anti-commutativity: B×A=−(A×B)=−C.\mathbf{B}\times\mathbf{A} = -(\mathbf{A}\times\mathbf{B}) = -\mathbf{C}.

Add them: 2C+(−C)=C.2\mathbf{C} + (-\mathbf{C}) = \mathbf{C}.

So the expression equals C\mathbf{C}.

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