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Chapter 10 · Vector Algebra

Example 25: Area of the parallelogram on 3i^+j^+4k^3\hat i+\hat j+4\hat k and i^−j^+k^\hat i-\hat j+\hat k

ExamplesArea of a parallelogram by the vector product · Section 10.6.3
The question

Find the area of a parallelogram whose adjacent sides are given by the vectors a⃗=3i^+j^+4k^\vec a = 3\hat i + \hat j + 4\hat k and b⃗=i^−j^+k^\vec b = \hat i - \hat j + \hat k

Exam answer

The area of the parallelogram with adjacent sides a⃗\vec a and b⃗\vec b is ∣a⃗×b⃗∣|\vec a\times\vec b|⁠.

a⃗×b⃗=∣i^j^k^3141−11∣=i^(1+4)−j^(3−4)+k^(−3−1)=5i^+j^−4k^\begin{aligned} \vec a\times\vec b &= \begin{vmatrix} \hat i & \hat j & \hat k \\ 3 & 1 & 4 \\ 1 & -1 & 1 \end{vmatrix} \\ &= \hat i(1 + 4) - \hat j(3 - 4) \\ &\quad + \hat k(-3 - 1) \\ &= 5\hat i + \hat j - 4\hat k \end{aligned} ∣a⃗×b⃗∣=25+1+16=42\begin{aligned} |\vec a\times\vec b| &= \sqrt{25 + 1 + 16} \\ &= \sqrt{42} \end{aligned}

∴\therefore the required area is 42\sqrt{42} sq. units.

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

The one idea this problem is built on

The area of a parallelogram is base times height. With adjacent sides a⃗\vec a and b⃗\vec b at angle θ\theta⁠, that is ∣a⃗∣×∣b⃗∣sin⁡θ|\vec a| \times |\vec b|\sin\theta⁠, which is exactly the length of the vector product:

area=∣a⃗×b⃗∣.\text{area} = |\vec a\times\vec b|.
Given, to find, and the plan
Given
Adjacent sides a⃗=3i^+j^+4k^\vec a = 3\hat i + \hat j + 4\hat k and b⃗=i^−j^+k^\vec b = \hat i - \hat j + \hat k⁠.
To find
The area of the parallelogram.
Plan
(1) Recall area =∣a⃗×b⃗∣= |\vec a\times\vec b|⁠. (2) Compute a⃗×b⃗\vec a\times\vec b⁠. (3) Check it is perpendicular to both sides. (4) Take its length. (5) Check with ∣a⃗∣2∣b⃗∣2−(a⃗⋅b⃗)2|\vec a|^2|\vec b|^2 - (\vec a\cdot\vec b)^2⁠.

Basics you need

1Area of a parallelogram

If a⃗\vec a and b⃗\vec b are adjacent sides, the area is ∣a⃗×b⃗∣|\vec a\times\vec b| (Section 10.6.3, Observation 9, Fig 10.27). Lesson: the cross product

2The determinant form of a⃗×b⃗\vec a\times\vec b

i^,j^,k^\hat i, \hat j, \hat k on top, then the components of a⃗\vec a⁠, then those of b⃗\vec b⁠; expand along the top row with signs +,−,++, -, +⁠. Basics: a determinant measures a signed area

3Magnitude from components

∣xi^+yj^+zk^∣=x2+y2+z2|x\hat i + y\hat j + z\hat k| = \sqrt{x^2 + y^2 + z^2} (Section 10.5.1). Basics: use Pythagoras twice

4Sine from cosine

sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta⁠, and cos⁡θ=a⃗⋅b⃗∣a⃗∣∣b⃗∣\cos\theta = \frac{\vec a\cdot\vec b}{|\vec a||\vec b|} (Section 10.6.1, Observation 6). Basics: cos θ is a shadow, sin θ is a height

Solution

  1. Area as the length of a vector product

    Take a⃗\vec a as the base. The height is the distance of the opposite side from the base, ∣b⃗∣sin⁡θ|\vec b|\sin\theta⁠, so

    area=∣a⃗∣ ∣b⃗∣sin⁡θ=∣a⃗×b⃗∣.\text{area} = |\vec a|\,|\vec b|\sin\theta = |\vec a\times\vec b|.
    By definition 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, so its length is ∣a⃗∣∣b⃗∣sin⁡θ|\vec a||\vec b|\sin\theta (with sin⁡θ≥0\sin\theta \ge 0 because 0≤θ≤π0 \le \theta \le \pi⁠). That is the base times the height.
    Area of a parallelogram =∣a⃗×b⃗∣= |\vec a\times\vec b| (Section 10.6.3, Observation 9). Lesson: the cross product
  2. The vector product

    a⃗×b⃗=∣i^j^k^3141−11∣=i^(1+4)−j^(3−4)+k^(−3−1)=5i^+j^−4k^.\begin{aligned} \vec a\times\vec b &= \begin{vmatrix} \hat i & \hat j & \hat k \\ 3 & 1 & 4 \\ 1 & -1 & 1 \end{vmatrix} \\ &= \hat i(1 + 4) - \hat j(3 - 4) \\ &\quad + \hat k(-3 - 1) \\ &= 5\hat i + \hat j - 4\hat k. \end{aligned}
    The minors are (1)(1)−(4)(−1)=1+4(1)(1) - (4)(-1) = 1 + 4⁠, (3)(1)−(4)(1)=3−4(3)(1) - (4)(1) = 3 - 4 and (3)(−1)−(1)(1)=−3−1(3)(-1) - (1)(1) = -3 - 1⁠. The middle one, −1-1⁠, takes a minus sign and becomes +1+1⁠, so the j^\hat j component is +1+1⁠.
    Expansion along the top row, signs +,−,++, -, +⁠. Basics: a determinant measures a signed area
  3. Check: perpendicular to both sides

    (5i^+j^−4k^)⋅a⃗=15+1−16=0,(5i^+j^−4k^)⋅b⃗=5−1−4=0.\begin{aligned} (5\hat i + \hat j - 4\hat k)\cdot\vec a &= 15 + 1 - 16 = 0, \\ (5\hat i + \hat j - 4\hat k)\cdot\vec b &= 5 - 1 - 4 = 0. \end{aligned}
    a⃗×b⃗\vec a\times\vec b must be perpendicular to both a⃗\vec a and b⃗\vec b⁠; both scalar products are 0, so the determinant work is consistent.
    u⃗⋅v⃗=0\vec u\cdot\vec v = 0 for perpendicular vectors (Section 10.6.1, Observation 2). Lesson: the dot product
  4. The length gives the area

    ∣a⃗×b⃗∣=52+12+(−4)2=25+1+16=42.\begin{aligned} |\vec a\times\vec b| &= \sqrt{5^2 + 1^2 + (-4)^2} \\ &= \sqrt{25 + 1 + 16} = \sqrt{42}. \end{aligned}

    So the area is 42\sqrt{42} square units. Since 42=2×3×742 = 2 \times 3 \times 7 has no square factor, 42\sqrt{42} is already in simplest form.

    An area is a length squared, so it is measured in square units; the vector product's direction (along 5i^+j^−4k^5\hat i + \hat j - 4\hat k⁠) is not needed, only its length.
    ∣r⃗∣=x2+y2+z2|\vec r| = \sqrt{x^2 + y^2 + z^2} (Section 10.5.1). Basics: use Pythagoras twice
  5. A check with the scalar product only

    ∣a⃗∣2=9+1+16=26|\vec a|^2 = 9 + 1 + 16 = 26⁠, ∣b⃗∣2=1+1+1=3|\vec b|^2 = 1 + 1 + 1 = 3 and a⃗⋅b⃗=3−1+4=6\vec a\cdot\vec b = 3 - 1 + 4 = 6⁠. Since ∣a⃗×b⃗∣2=∣a⃗∣2∣b⃗∣2sin⁡2θ|\vec a\times\vec b|^2 = |\vec a|^2|\vec b|^2\sin^2\theta =∣a⃗∣2∣b⃗∣2−(a⃗⋅b⃗)2= |\vec a|^2|\vec b|^2 - (\vec a\cdot\vec b)^2⁠,

    ∣a⃗×b⃗∣2=(26)(3)−62=78−36=42.\begin{aligned} |\vec a\times\vec b|^2 &= (26)(3) - 6^2 \\ &= 78 - 36 = 42. \end{aligned}
    O a, length √26 b, length √3 area = |a × b| = √42 ≈ 6.48
    The parallelogram drawn in its own plane, true to scale: base ∣a⃗∣=26|\vec a| = \sqrt{26}⁠, side ∣b⃗∣=3|\vec b| = \sqrt3⁠, and the height ∣b⃗∣sin⁡θ=4226|\vec b|\sin\theta = \frac{\sqrt{42}}{\sqrt{26}}⁠, so base times height is 42≈6.48\sqrt{42} \approx 6.48⁠.
    This uses no determinant at all, so it is an independent check of Steps 2 and 4. It comes from sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta and a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec a\cdot\vec b = |\vec a||\vec b|\cos\theta⁠.
    cos⁡θ=a⃗⋅b⃗∣a⃗∣∣b⃗∣\cos\theta = \frac{\vec a\cdot\vec b}{|\vec a||\vec b|} (Section 10.6.1, Observation 6). Lesson: Examples 22–25
Result

The area of the parallelogram is ∣a⃗×b⃗∣=42|\vec a\times\vec b| = \sqrt{42} square units.

(Textbook answer: a⃗×b⃗=5i^+j^−4k^\vec a\times\vec b = 5\hat i + \hat j - 4\hat k⁠, ∣a⃗×b⃗∣=25+1+16=42|\vec a\times\vec b| = \sqrt{25 + 1 + 16} = \sqrt{42}⁠, "and hence, the required area is 42\sqrt{42}⁠.")

Check it with numbers

42≈6.480741\sqrt{42} \approx 6.480741⁠.

∣a⃗∣=26≈5.099020|\vec a| = \sqrt{26} \approx 5.099020⁠, ∣b⃗∣=3≈1.732051|\vec b| = \sqrt3 \approx 1.732051⁠, cos⁡θ=678≈0.679366\cos\theta = \frac{6}{\sqrt{78}} \approx 0.679366⁠, so θ≈47.21∘\theta \approx 47.21^\circ⁠. The height is 4226≈1.270978\frac{\sqrt{42}}{\sqrt{26}} \approx 1.270978⁠, and base times height is 26⋅4226=42\sqrt{26}\cdot\frac{\sqrt{42}}{\sqrt{26}} = \sqrt{42} exactly.

Common mistakes
  1. Halving. 12∣a⃗×b⃗∣\frac12|\vec a\times\vec b| is the triangle on a⃗\vec a and b⃗\vec b⁠; the parallelogram is the whole ∣a⃗×b⃗∣|\vec a\times\vec b|⁠.
  2. Treating the diagonals as sides. If a question gives the diagonals d⃗1,d⃗2\vec d_1, \vec d_2⁠, the area is 12∣d⃗1×d⃗2∣\frac12|\vec d_1\times\vec d_2|⁠; here the vectors are adjacent sides, so no 12\frac12⁠.
  3. Using ∣a⃗∣∣b⃗∣|\vec a||\vec b| as the area. That would be right only for a rectangle; the factor sin⁡θ≈0.73\sin\theta \approx 0.73 here cannot be dropped.
What to take away
  1. Parallelogram with adjacent sides a⃗\vec a⁠, b⃗\vec b⁠: area =∣a⃗×b⃗∣= |\vec a\times\vec b|⁠.
  2. Triangle with the same two sides: half of that.
  3. ∣a⃗×b⃗∣2=∣a⃗∣2∣b⃗∣2−(a⃗⋅b⃗)2|\vec a\times\vec b|^2 = |\vec a|^2|\vec b|^2 - (\vec a\cdot\vec b)^2 gives an independent check.

Every fact used, and where it comes from

FactUsed inSource
Area of a parallelogram =∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ= |\vec a\times\vec b| = |\vec a||\vec b|\sin\thetaSteps 1, 4Section 10.6.3, Definition 3 and Observation 9, Fig 10.27 (Lesson: the cross product)
a⃗×b⃗\vec a\times\vec b as a determinant in componentsStep 2Section 10.6.3 (Basics: a determinant measures a signed area)
Scalar product in components; zero for perpendicular vectorsSteps 3, 5Section 10.6.1 and its Observation 2
∣xi^+yj^+zk^∣=x2+y2+z2|x\hat i + y\hat j + z\hat k| = \sqrt{x^2 + y^2 + z^2}Steps 4, 5Section 10.5.1
cos⁡θ=a⃗⋅b⃗∣a⃗∣∣b⃗∣\cos\theta = \frac{\vec a\cdot\vec b}{|\vec a||\vec b|}⁠; sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1Step 5Section 10.6.1, Observation 6; trigonometry
Area of a triangle =12∣a⃗×b⃗∣= \frac12|\vec a\times\vec b|Common mistakesSection 10.6.3, Observation 8
The book's working and answerResultExample 25, Section 10.6.3 (Lesson: Examples 22–25)
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