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Chapter 10 · Vector Algebra

Exercise 10.4 · Q7: Distributive law a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\vec a\times(\vec b+\vec c)=\vec a\times\vec b+\vec a\times\vec c

Exercise 10.4Vector product in components, distributive law · Section 10.6.3
The question

Let the vectors a⃗,b⃗,c⃗\vec a, \vec b, \vec c be given as a1i^+a2j^+a3k^a_1\hat i + a_2\hat j + a_3\hat k⁠, b1i^+b2j^+b3k^b_1\hat i + b_2\hat j + b_3\hat k⁠, c1i^+c2j^+c3k^c_1\hat i + c_2\hat j + c_3\hat k⁠. Then show that a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\vec a\times(\vec b + \vec c) = \vec a\times\vec b + \vec a\times\vec c⁠.

Exam answer a⃗×b⃗=∣i^j^k^a1a2a3b1b2b3∣=(a2b3−a3b2)i^−(a1b3−a3b1)j^+(a1b2−a2b1)k^…(i)\begin{aligned} \vec a\times\vec b &= \begin{vmatrix} \hat i & \hat j & \hat k \\ a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \end{vmatrix} \\ &= (a_2b_3 - a_3b_2)\hat i \\ &\quad - (a_1b_3 - a_3b_1)\hat j \\ &\quad + (a_1b_2 - a_2b_1)\hat k \quad\ldots(\text{i}) \end{aligned}

Similarly,

a⃗×c⃗=(a2c3−a3c2)i^−(a1c3−a3c1)j^+(a1c2−a2c1)k^…(ii)\begin{aligned} \vec a\times\vec c &= (a_2c_3 - a_3c_2)\hat i \\ &\quad - (a_1c_3 - a_3c_1)\hat j \\ &\quad + (a_1c_2 - a_2c_1)\hat k \quad\ldots(\text{ii}) \end{aligned}

Now b⃗+c⃗=(b1+c1)i^\vec b + \vec c = (b_1 + c_1)\hat i +(b2+c2)j^+(b3+c3)k^+ (b_2 + c_2)\hat j + (b_3 + c_3)\hat k⁠. So

a⃗×(b⃗+c⃗)=∣i^j^k^a1a2a3b1+c1b2+c2b3+c3∣=[a2(b3+c3)−a3(b2+c2)]i^−[a1(b3+c3)−a3(b1+c1)]j^+[a1(b2+c2)−a2(b1+c1)]k^\begin{aligned} &\vec a\times(\vec b + \vec c) \\ &= \begin{vmatrix} \hat i & \hat j & \hat k \\ a_1 & a_2 & a_3 \\ b_1 + c_1 & b_2 + c_2 & b_3 + c_3 \end{vmatrix} \\ &= [a_2(b_3 + c_3) - a_3(b_2 + c_2)]\hat i \\ &\quad - [a_1(b_3 + c_3) - a_3(b_1 + c_1)]\hat j \\ &\quad + [a_1(b_2 + c_2) - a_2(b_1 + c_1)]\hat k \end{aligned}

Opening the brackets and grouping the bb terms and the cc terms,

a⃗×(b⃗+c⃗)=(a2b3−a3b2)i^−(a1b3−a3b1)j^+(a1b2−a2b1)k^+(a2c3−a3c2)i^−(a1c3−a3c1)j^+(a1c2−a2c1)k^=a⃗×b⃗+a⃗×c⃗[by (i), (ii)]\begin{aligned} &\vec a\times(\vec b + \vec c) \\ &= (a_2b_3 - a_3b_2)\hat i \\ &\quad - (a_1b_3 - a_3b_1)\hat j \\ &\quad + (a_1b_2 - a_2b_1)\hat k \\ &\quad + (a_2c_3 - a_3c_2)\hat i \\ &\quad - (a_1c_3 - a_3c_1)\hat j \\ &\quad + (a_1c_2 - a_2c_1)\hat k \\ &= \vec a\times\vec b + \vec a\times\vec c \quad [\text{by (i), (ii)}] \end{aligned}

∴ a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\therefore\ \vec a\times(\vec b + \vec c) = \vec a\times\vec b + \vec a\times\vec c⁠. Hence proved.

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

The one idea this problem is built on

Every component of a⃗×b⃗\vec a\times\vec b is a difference of two products, each with one factor from b⃗\vec b⁠. Replacing b⃗\vec b by b⃗+c⃗\vec b + \vec c and multiplying out splits each component into a "bb part" plus a "cc part". Collecting the bb parts gives a⃗×b⃗\vec a\times\vec b⁠; collecting the cc parts gives a⃗×c⃗\vec a\times\vec c⁠.

Given, to show, and the plan
Given
a⃗=a1i^+a2j^+a3k^\vec a = a_1\hat i + a_2\hat j + a_3\hat k⁠, b⃗=b1i^+b2j^+b3k^\vec b = b_1\hat i + b_2\hat j + b_3\hat k⁠, c⃗=c1i^+c2j^+c3k^\vec c = c_1\hat i + c_2\hat j + c_3\hat k⁠.
To show
a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\vec a\times(\vec b + \vec c) = \vec a\times\vec b + \vec a\times\vec c⁠.
Plan
(1) Write a⃗×b⃗\vec a\times\vec b and a⃗×c⃗\vec a\times\vec c in components. (2) Write b⃗+c⃗\vec b + \vec c and a⃗×(b⃗+c⃗)\vec a\times(\vec b + \vec c) in components. (3) Multiply out and regroup. (4) Compare, and check with numbers.

Basics you need

1Vector product in components

a⃗×b⃗=(a2b3−a3b2)i^\vec a\times\vec b = (a_2b_3 - a_3b_2)\hat i −(a1b3−a3b1)j^- (a_1b_3 - a_3b_1)\hat j +(a1b2−a2b1)k^+ (a_1b_2 - a_2b_1)\hat k⁠, the expansion of the determinant with i^,j^,k^\hat i, \hat j, \hat k on top (Section 10.6.3). Basics: a determinant measures a signed area

2Adding vectors in components

b⃗+c⃗=(b1+c1)i^+(b2+c2)j^\vec b + \vec c = (b_1 + c_1)\hat i + (b_2 + c_2)\hat j +(b3+c3)k^+ (b_3 + c_3)\hat k (Section 10.5.1). Lesson: components

3Ordinary algebra

p(q+r)=pq+prp(q + r) = pq + pr⁠, and terms can be added in any order. Basics: expanding brackets

Solution

  1. a⃗×b⃗\vec a\times\vec b and a⃗×c⃗\vec a\times\vec c in components

    a⃗×b⃗=(a2b3−a3b2)i^−(a1b3−a3b1)j^+(a1b2−a2b1)k^,a⃗×c⃗=(a2c3−a3c2)i^−(a1c3−a3c1)j^+(a1c2−a2c1)k^.\begin{aligned} \vec a\times\vec b &= (a_2b_3 - a_3b_2)\hat i - (a_1b_3 - a_3b_1)\hat j \\ &\quad + (a_1b_2 - a_2b_1)\hat k, \\ \vec a\times\vec c &= (a_2c_3 - a_3c_2)\hat i - (a_1c_3 - a_3c_1)\hat j \\ &\quad + (a_1c_2 - a_2c_1)\hat k. \end{aligned}
    These are the determinant formula with b⃗\vec b⁠, then c⃗\vec c⁠, in the bottom row. The second line is the first with every bb replaced by cc⁠.
    The determinant form of the vector product (Section 10.6.3). Lesson: the cross product
  2. a⃗×(b⃗+c⃗)\vec a\times(\vec b + \vec c) in components

    The components of b⃗+c⃗\vec b + \vec c are b1+c1b_1 + c_1⁠, b2+c2b_2 + c_2⁠, b3+c3b_3 + c_3⁠, so they form the bottom row:

    a⃗×(b⃗+c⃗)=∣i^j^k^a1a2a3b1+c1b2+c2b3+c3∣=[a2(b3+c3)−a3(b2+c2)]i^−[a1(b3+c3)−a3(b1+c1)]j^+[a1(b2+c2)−a2(b1+c1)]k^.\begin{aligned} &\vec a\times(\vec b + \vec c) \\ &= \begin{vmatrix} \hat i & \hat j & \hat k \\ a_1 & a_2 & a_3 \\ b_1 + c_1 & b_2 + c_2 & b_3 + c_3 \end{vmatrix} \\ &= [a_2(b_3 + c_3) - a_3(b_2 + c_2)]\hat i \\ &\quad - [a_1(b_3 + c_3) - a_3(b_1 + c_1)]\hat j \\ &\quad + [a_1(b_2 + c_2) - a_2(b_1 + c_1)]\hat k. \end{aligned}
    The same formula as in Step 1, with b1+c1b_1 + c_1 in place of b1b_1⁠, and so on. Brackets keep each sum together.
    Adding vectors in components (Section 10.5.1). Lesson: components
  3. Multiply out and regroup

    Take the i^\hat i component:

    a2(b3+c3)−a3(b2+c2)=a2b3+a2c3−a3b2−a3c2=(a2b3−a3b2)+(a2c3−a3c2).\begin{aligned} &a_2(b_3 + c_3) - a_3(b_2 + c_2) \\ &= a_2b_3 + a_2c_3 - a_3b_2 - a_3c_2 \\ &= (a_2b_3 - a_3b_2) + (a_2c_3 - a_3c_2). \end{aligned}

    In the same way, the j^\hat j bracket is (a1b3−a3b1)+(a1c3−a3c1)(a_1b_3 - a_3b_1) + (a_1c_3 - a_3c_1) and the k^\hat k bracket is (a1b2−a2b1)+(a1c2−a2c1)(a_1b_2 - a_2b_1) + (a_1c_2 - a_2c_1)⁠.

    Each bracket is opened by p(q+r)=pq+prp(q + r) = pq + pr⁠, and then the four terms are put in a different order: the two with a bb first, the two with a cc second. The minus sign in front of the j^\hat j bracket applies to both groups, so it stays in front of each.
    Distributive law for numbers; rearranging a sum. Basics: expanding brackets
  4. Compare with Step 1

    a⃗×(b⃗+c⃗)=[(a2b3−a3b2)i^−(a1b3−a3b1)j^+(a1b2−a2b1)k^]+[(a2c3−a3c2)i^−(a1c3−a3c1)j^+(a1c2−a2c1)k^]=a⃗×b⃗+a⃗×c⃗.\begin{aligned} &\vec a\times(\vec b + \vec c) \\ &= [(a_2b_3 - a_3b_2)\hat i - (a_1b_3 - a_3b_1)\hat j \\ &\qquad + (a_1b_2 - a_2b_1)\hat k] \\ &\quad + [(a_2c_3 - a_3c_2)\hat i - (a_1c_3 - a_3c_1)\hat j \\ &\qquad + (a_1c_2 - a_2c_1)\hat k] \\ &= \vec a\times\vec b + \vec a\times\vec c. \end{aligned}
    The first square bracket is exactly a⃗×b⃗\vec a\times\vec b from Step 1 and the second is exactly a⃗×c⃗\vec a\times\vec c⁠. Since the components agree one by one, the vectors are equal. This is Property 3 (i) of Section 10.6.3, proved here from the component formula. (The book itself obtains the determinant formula, just before Example 22, by expanding the brackets with this law; so within the book the exercise shows that the formula and the law agree, and with the determinant formula taken as the starting point it is a complete proof.)
    Vectors are equal iff their components are equal (Section 10.5.1). Lesson: the cross product, exercises
  5. Check with numbers

    Take a⃗=i^+2j^+k^\vec a = \hat i + 2\hat j + \hat k⁠, b⃗=2i^−j^+k^\vec b = 2\hat i - \hat j + \hat k⁠, c⃗=j^+2k^\vec c = \hat j + 2\hat k⁠. Then b⃗+c⃗=2i^+3k^\vec b + \vec c = 2\hat i + 3\hat k⁠, and

    a⃗×(b⃗+c⃗)=i^(6−0)−j^(3−2)+k^(0−4)=6i^−j^−4k^,a⃗×b⃗=i^(2+1)−j^(1−2)+k^(−1−4)=3i^+j^−5k^,a⃗×c⃗=i^(4−1)−j^(2−0)+k^(1−0)=3i^−2j^+k^.\begin{aligned} \vec a\times(\vec b + \vec c) &= \hat i(6 - 0) - \hat j(3 - 2) \\ &\quad + \hat k(0 - 4) \\ &= 6\hat i - \hat j - 4\hat k, \\ \vec a\times\vec b &= \hat i(2 + 1) - \hat j(1 - 2) \\ &\quad + \hat k(-1 - 4) \\ &= 3\hat i + \hat j - 5\hat k, \\ \vec a\times\vec c &= \hat i(4 - 1) - \hat j(2 - 0) \\ &\quad + \hat k(1 - 0) \\ &= 3\hat i - 2\hat j + \hat k. \end{aligned}

    And (3i^+j^−5k^)+(3i^−2j^+k^)=6i^−j^−4k^(3\hat i + \hat j - 5\hat k) + (3\hat i - 2\hat j + \hat k) = 6\hat i - \hat j - 4\hat k⁠.

    A numerical example cannot prove a general law, but it is a quick test that the algebra above has no slip; the general proof is Steps 1 to 4.
    The determinant form of the vector product (Section 10.6.3). Basics: a determinant measures a signed area
Result

a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\vec a\times(\vec b + \vec c) = \vec a\times\vec b + \vec a\times\vec c for all vectors a⃗,b⃗,c⃗\vec a, \vec b, \vec c⁠. Hence proved.

(Textbook answer: the answer key has no entry for this "show that" question.)

Check it with numbers

With the sample of Step 5, component by component: i^\hat i⁠: 6=3+36 = 3 + 3⁠; j^\hat j⁠: −1=1+(−2)-1 = 1 + (-2)⁠; k^\hat k⁠: −4=−5+1-4 = -5 + 1⁠.

A second sample, a⃗=k^\vec a = \hat k⁠, b⃗=i^\vec b = \hat i⁠, c⃗=j^\vec c = \hat j⁠: k^×(i^+j^)=j^−i^\hat k\times(\hat i + \hat j) = \hat j - \hat i⁠, and k^×i^+k^×j^=j^+(−i^)\hat k\times\hat i + \hat k\times\hat j = \hat j + (-\hat i)⁠, the same vector.

Common mistakes
  1. Proving it with one numerical example. A sample only checks; the proof must use general components a1,…,c3a_1, \ldots, c_3⁠.
  2. Dropping the minus sign in front of the j^\hat j bracket. It belongs to both (a1b3−a3b1)(a_1b_3 - a_3b_1) and (a1c3−a3c1)(a_1c_3 - a_3c_1)⁠.
  3. Using the law to prove itself. Writing "a⃗×(b⃗+c⃗)=a⃗×b⃗+a⃗×c⃗\vec a\times(\vec b + \vec c) = \vec a\times\vec b + \vec a\times\vec c by distributivity" assumes what is to be shown; the components do the work.
What to take away
  1. Each component of a⃗×b⃗\vec a\times\vec b is linear in the components of b⃗\vec b⁠, so sums in b⃗\vec b split.
  2. To prove a vector identity in components, compare the i^\hat i⁠, j^\hat j⁠, k^\hat k parts one at a time.
  3. Check a general identity on a numerical sample before trusting the algebra.

Every fact used, and where it comes from

FactUsed inSource
a⃗×b⃗\vec a\times\vec b as a determinant in componentsSteps 1, 2, 5Section 10.6.3 (Basics: a determinant measures a signed area)
Sum of vectors in components; equal vectors have equal componentsSteps 2, 4Section 10.5.1 (Lesson: components)
p(q+r)=pq+prp(q + r) = pq + pr for numbersStep 3Algebra (Basics: expanding brackets)
Distributivity of the vector product (the statement proved)Step 4Section 10.6.3, Property 3 (i) (Lesson: the cross product)
k^×i^=j^\hat k\times\hat i = \hat j⁠, k^×j^=−i^\hat k\times\hat j = -\hat iCheckSection 10.6.3, Observations 4 and 7
The questionResultExercise 10.4 Q7 (no answer-key entry) (Lesson: the cross product, exercises)
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