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Chapter 10 · Vector Algebra

Exercise 10.4 · Q6: a⃗⋅b⃗=0\vec a\cdot\vec b=0 and a⃗×b⃗=0⃗\vec a\times\vec b=\vec 0⁠: what follows?

Exercise 10.4Scalar and vector products together · Sections 10.6.1 and 10.6.3
The question

Given that a⃗⋅b⃗=0\vec a\cdot\vec b = 0 and a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0⁠. What can you conclude about the vectors a⃗\vec a and b⃗\vec b⁠?

Exam answer

Suppose a⃗≠0⃗\vec a \ne \vec 0 and b⃗≠0⃗\vec b \ne \vec 0⁠, and let θ\theta be the angle between them.

a⃗⋅b⃗=0⇒∣a⃗∣∣b⃗∣cos⁡θ=0⇒cos⁡θ=0a⃗×b⃗=0⃗⇒∣a⃗∣∣b⃗∣sin⁡θ=0⇒sin⁡θ=0\begin{aligned} \vec a\cdot\vec b = 0 &\Rightarrow |\vec a||\vec b|\cos\theta = 0 \\ &\Rightarrow \cos\theta = 0 \\ \vec a\times\vec b = \vec 0 &\Rightarrow |\vec a||\vec b|\sin\theta = 0 \\ &\Rightarrow \sin\theta = 0 \end{aligned}

But sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1⁠, so sin⁡θ\sin\theta and cos⁡θ\cos\theta cannot both be 0. So the supposition is false.

∴\therefore either a⃗=0⃗\vec a = \vec 0 or b⃗=0⃗\vec b = \vec 0⁠, that is, ∣a⃗∣=0|\vec a| = 0 or ∣b⃗∣=0|\vec b| = 0⁠.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

For nonzero vectors at angle θ\theta⁠, the scalar product carries cos⁡θ\cos\theta and the vector product carries sin⁡θ\sin\theta⁠:

∣a⃗⋅b⃗∣=∣a⃗∣∣b⃗∣∣cos⁡θ∣,∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ.\begin{aligned} |\vec a\cdot\vec b| &= |\vec a||\vec b||\cos\theta|, \\ |\vec a\times\vec b| &= |\vec a||\vec b|\sin\theta. \end{aligned}

A cosine and a sine of the same angle are never both 0, so both products can vanish only if one of the vectors is 0⃗\vec 0⁠.

Given, to find, and the plan
Given
a⃗⋅b⃗=0\vec a\cdot\vec b = 0 and a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0⁠.
To find
What this tells us about a⃗\vec a and b⃗\vec b⁠.
Plan
(1) Read each condition for nonzero vectors. (2) Show they cannot both hold, so one vector is 0⃗\vec 0⁠. (3) Check that a zero vector really satisfies both. (4) Confirm with an identity that holds for all vectors.

Basics you need

1The scalar product

For nonzero vectors, a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec a\cdot\vec b = |\vec a||\vec b|\cos\theta with 0≤θ≤π0 \le \theta \le \pi⁠; if either vector is 0⃗\vec 0⁠, a⃗⋅b⃗=0\vec a\cdot\vec b = 0 (Definition 2, Section 10.6.1). Lesson: the dot product

2The vector product

For nonzero vectors, a⃗×b⃗=∣a⃗∣∣b⃗∣sin⁡θ n^\vec a\times\vec b = |\vec a||\vec b|\sin\theta\,\hat n with n^\hat n a unit vector; if either vector is 0⃗\vec 0⁠, a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0 (Definition 3, Section 10.6.3). Lesson: the cross product

3sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1

So sin⁡θ\sin\theta and cos⁡θ\cos\theta are never both 0. Basics: cos θ is a shadow, sin θ is a height

Solution

  1. What each condition says for nonzero vectors

    Suppose a⃗≠0⃗\vec a \ne \vec 0 and b⃗≠0⃗\vec b \ne \vec 0⁠, at angle θ\theta⁠. Then ∣a⃗∣∣b⃗∣>0|\vec a||\vec b| > 0⁠, and

    a⃗⋅b⃗=0⇒∣a⃗∣∣b⃗∣cos⁡θ=0⇒cos⁡θ=0,a⃗×b⃗=0⃗⇒∣a⃗∣∣b⃗∣sin⁡θ=0⇒sin⁡θ=0.\begin{aligned} \vec a\cdot\vec b = 0 &\Rightarrow |\vec a||\vec b|\cos\theta = 0 \\ &\Rightarrow \cos\theta = 0, \\ \vec a\times\vec b = \vec 0 &\Rightarrow |\vec a||\vec b|\sin\theta = 0 \\ &\Rightarrow \sin\theta = 0. \end{aligned}
    We may divide by ∣a⃗∣∣b⃗∣|\vec a||\vec b| because it is positive. For the vector product, ∣a⃗∣∣b⃗∣sin⁡θ n^=0⃗|\vec a||\vec b|\sin\theta\,\hat n = \vec 0 with ∣n^∣=1|\hat n| = 1 forces the number ∣a⃗∣∣b⃗∣sin⁡θ|\vec a||\vec b|\sin\theta to be 0. So the first condition says the vectors are perpendicular (θ=π2\theta = \frac{\pi}{2}⁠) and the second says they are parallel (θ=0\theta = 0 or π\pi⁠).
    Definitions of the two products (Sections 10.6.1 and 10.6.3). Lesson: the cross product
  2. Both cannot hold

    sin⁡2θ+cos⁡2θ=1≠0+0.\sin^2\theta + \cos^2\theta = 1 \ne 0 + 0.

    So the supposition is false: a⃗=0⃗\vec a = \vec 0 or b⃗=0⃗\vec b = \vec 0⁠.

    Two nonzero vectors cannot be perpendicular and parallel at the same time. Since assuming both are nonzero leads to a contradiction, at least one of them is the zero vector. "a⃗=0⃗\vec a = \vec 0" is the same as "∣a⃗∣=0|\vec a| = 0", the form in the answer key.
    sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1⁠. Basics: cos θ is a shadow, sin θ is a height
  3. The conclusion is exact

    Conversely, if a⃗=0⃗\vec a = \vec 0 (or b⃗=0⃗\vec b = \vec 0⁠), then a⃗⋅b⃗=0\vec a\cdot\vec b = 0 and a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0 for every choice of the other vector.

    Both definitions set the product to zero when either vector is 0⃗\vec 0 (the angle is then not defined). So the two conditions together say exactly "one of the vectors is 0⃗\vec 0"; nothing more can be said about the other vector, which may be any vector.
    Products with the zero vector (Definitions 2 and 3, Sections 10.6.1 and 10.6.3). Lesson: the dot product
  4. A second route that covers every case

    For all vectors a⃗=a1i^+a2j^+a3k^\vec a = a_1\hat i + a_2\hat j + a_3\hat k and b⃗=b1i^+b2j^+b3k^\vec b = b_1\hat i + b_2\hat j + b_3\hat k⁠, expanding both sides in components shows

    ∣a⃗×b⃗∣2+(a⃗⋅b⃗)2=∣a⃗∣2∣b⃗∣2.|\vec a\times\vec b|^2 + (\vec a\cdot\vec b)^2 = |\vec a|^2|\vec b|^2.

    Here the left side is 0+00 + 0⁠, so ∣a⃗∣2∣b⃗∣2=0|\vec a|^2|\vec b|^2 = 0⁠, and ∣a⃗∣=0|\vec a| = 0 or ∣b⃗∣=0|\vec b| = 0⁠.

    For nonzero vectors this identity is ∣a⃗∣2∣b⃗∣2(sin⁡2θ+cos⁡2θ)|\vec a|^2|\vec b|^2(\sin^2\theta + \cos^2\theta)⁠, the same fact as Step 2; written in components it holds even when a vector is 0⃗\vec 0⁠, so this route needs no case split. A product of two real numbers is 0 only when one of them is 0.
    Products in components (Sections 10.6.1 and 10.6.3). Lesson: the cross product, exercises
Result

At least one of the vectors is the zero vector: either a⃗=0⃗\vec a = \vec 0 or b⃗=0⃗\vec b = \vec 0⁠, that is, ∣a⃗∣=0|\vec a| = 0 or ∣b⃗∣=0|\vec b| = 0⁠.

(Textbook answer: either ∣a⃗∣=0|\vec a| = 0 or ∣b⃗∣=0|\vec b| = 0⁠.)

Check it with numbers

Perpendicular but nonzero: a⃗=i^\vec a = \hat i⁠, b⃗=j^\vec b = \hat j give a⃗⋅b⃗=0\vec a\cdot\vec b = 0 but a⃗×b⃗=k^≠0⃗\vec a\times\vec b = \hat k \ne \vec 0⁠.

Parallel but nonzero: a⃗=i^\vec a = \hat i⁠, b⃗=2i^\vec b = 2\hat i give a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0 but a⃗⋅b⃗=2≠0\vec a\cdot\vec b = 2 \ne 0⁠.

The identity of Step 4 with a⃗=i^+2j^+3k^\vec a = \hat i + 2\hat j + 3\hat k⁠, b⃗=2i^−j^+k^\vec b = 2\hat i - \hat j + \hat k⁠: a⃗×b⃗=5i^+5j^−5k^\vec a\times\vec b = 5\hat i + 5\hat j - 5\hat k⁠, so 75+32=84=14×675 + 3^2 = 84 = 14 \times 6⁠.

Common mistakes
  1. Answering "a⃗\vec a and b⃗\vec b are perpendicular and parallel". Nonzero vectors cannot be both; the only way out is a zero vector.
  2. Concluding that both vectors are 0⃗\vec 0⁠. One zero vector is enough; the other can be anything.
  3. Dividing by ∣a⃗∣∣b⃗∣|\vec a||\vec b| without saying it is nonzero. That division is exactly what the supposition a⃗,b⃗≠0⃗\vec a, \vec b \ne \vec 0 allows.
What to take away
  1. a⃗⋅b⃗=0\vec a\cdot\vec b = 0 means perpendicular (or a zero vector); a⃗×b⃗=0⃗\vec a\times\vec b = \vec 0 means parallel (or a zero vector).
  2. Both together force a⃗=0⃗\vec a = \vec 0 or b⃗=0⃗\vec b = \vec 0⁠.
  3. ∣a⃗×b⃗∣2+(a⃗⋅b⃗)2=∣a⃗∣2∣b⃗∣2|\vec a\times\vec b|^2 + (\vec a\cdot\vec b)^2 = |\vec a|^2|\vec b|^2 links the two products.

Every fact used, and where it comes from

FactUsed inSource
a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec a\cdot\vec b = |\vec a||\vec b|\cos\theta⁠; zero if a vector is 0⃗\vec 0Steps 1, 3Section 10.6.1, Definition 2 (Lesson: the dot product)
a⃗×b⃗=∣a⃗∣∣b⃗∣sin⁡θ n^\vec a\times\vec b = |\vec a||\vec b|\sin\theta\,\hat n⁠; 0⃗\vec 0 if a vector is 0⃗\vec 0Steps 1, 3Section 10.6.3, Definition 3 (Lesson: the cross product)
sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1Steps 2, 4Trigonometry (Basics: cos θ is a shadow)
Both products in componentsStep 4Sections 10.6.1 and 10.6.3
The question and the answerResultExercise 10.4 Q6; NCERT answer key (Lesson: the cross product, exercises)
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