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Class 12Geometry10:14Published 25 Nov 2024

Vectors: Cross Product (Exercise 10.4, Part 1)

Worked solutions to Class XII vector cross product problems from Exercise 10.4, covering magnitudes, perpendicular unit vectors, direction cosines, and the angle between two vectors.

This lesson walks through five questions on the vector cross product for Class XII. It shows how to set up and expand the determinant for a cross product, find the magnitude of the result, and use it to build a unit vector perpendicular to two given vectors. It also uses direction cosines to find an unknown angle, solves for unknown components that make a cross product zero, and recovers the angle between two vectors from the magnitude of their cross product.

What you'll learn

  • Computing a cross product by expanding the determinant along its first row
  • Finding a unit vector perpendicular to the sum and the difference of two vectors
  • Using direction cosines to find an unknown angle a vector makes with an axis
  • Recovering the angle between two vectors from the magnitude of their cross product

Lesson chapters

0:00Magnitude of a cross product
2:05Unit vector perpendicular to two vectors
5:30Finding an angle from direction cosines
7:21Solving for unknowns that make a cross product zero
9:01Angle between two vectors from their cross product

Lesson notes

This lesson works through five cross product questions from Exercise 10.4 for Class XII. Each one expands a determinant, takes a magnitude, or uses those results to find a perpendicular vector or an angle.

Magnitude of a cross product

Given a=i7j+7k\vec{a} = \mathbf{i} - 7\mathbf{j} + 7\mathbf{k} and b=3i2j+2k\vec{b} = 3\mathbf{i} - 2\mathbf{j} + 2\mathbf{k}, find a×b|\vec{a} \times \vec{b}|.

Set up the determinant with the unit vectors in the first row and the components of a\vec{a} and b\vec{b} below:

a×b=ijk177322\vec{a} \times \vec{b} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 1 & -7 & 7 \\ 3 & -2 & 2 \end{vmatrix}

Expanding along the first row:

a×b=i((7)(2)(7)(2))j((1)(2)(7)(3))+k((1)(2)(7)(3))\vec{a} \times \vec{b} = \mathbf{i}\big((-7)(2) - (7)(-2)\big) - \mathbf{j}\big((1)(2) - (7)(3)\big) + \mathbf{k}\big((1)(-2) - (-7)(3)\big)

=i(0)j(19)+k(19)=19j+19k= \mathbf{i}(0) - \mathbf{j}(-19) + \mathbf{k}(19) = 19\mathbf{j} + 19\mathbf{k}

The magnitude is the square root of the sum of the squares of the components:

a×b=192+192=192|\vec{a} \times \vec{b}| = \sqrt{19^2 + 19^2} = 19\sqrt{2}

Unit vector perpendicular to two vectors

Find a unit vector perpendicular to both a+b\vec{a} + \vec{b} and ab\vec{a} - \vec{b}, where a=3i+2j+2k\vec{a} = 3\mathbf{i} + 2\mathbf{j} + 2\mathbf{k} and b=i+2j2k\vec{b} = \mathbf{i} + 2\mathbf{j} - 2\mathbf{k}.

Set up the two vectors. Let

c=a+b=4i+4j+0k,d=ab=2i+0j+4k\vec{c} = \vec{a} + \vec{b} = 4\mathbf{i} + 4\mathbf{j} + 0\mathbf{k}, \qquad \vec{d} = \vec{a} - \vec{b} = 2\mathbf{i} + 0\mathbf{j} + 4\mathbf{k}

Cross product. A vector perpendicular to both is c×d\vec{c} \times \vec{d}:

c×d=ijk440204=i(160)j(160)+k(08)=16i16j8k\vec{c} \times \vec{d} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 4 & 4 & 0 \\ 2 & 0 & 4 \end{vmatrix} = \mathbf{i}(16 - 0) - \mathbf{j}(16 - 0) + \mathbf{k}(0 - 8) = 16\mathbf{i} - 16\mathbf{j} - 8\mathbf{k}

Magnitude and unit vector.

c×d=162+(16)2+(8)2=576=24|\vec{c} \times \vec{d}| = \sqrt{16^2 + (-16)^2 + (-8)^2} = \sqrt{576} = 24

Taking out a factor of 88 from the numerator and dividing by 2424:

n^=±16i16j8k24=±2i2jk3\hat{n} = \pm \frac{16\mathbf{i} - 16\mathbf{j} - 8\mathbf{k}}{24} = \pm \frac{2\mathbf{i} - 2\mathbf{j} - \mathbf{k}}{3}

The two perpendicular unit vectors are 13(2i2jk)\tfrac{1}{3}(2\mathbf{i} - 2\mathbf{j} - \mathbf{k}) and 13(2i+2j+k)\tfrac{1}{3}(-2\mathbf{i} + 2\mathbf{j} + \mathbf{k}).

Finding an angle from direction cosines

A unit vector makes an angle π3\tfrac{\pi}{3} with i\mathbf{i}, π4\tfrac{\pi}{4} with j\mathbf{j}, and an acute angle θ\theta with k\mathbf{k}. Find θ\theta and the components of a\vec{a}.

The direction cosines are l=cosπ3l = \cos\tfrac{\pi}{3}, m=cosπ4m = \cos\tfrac{\pi}{4}, n=cosθn = \cos\theta, so

a=12i+12j+cosθk\vec{a} = \tfrac{1}{2}\mathbf{i} + \tfrac{1}{\sqrt{2}}\mathbf{j} + \cos\theta\,\mathbf{k}

Since a\vec{a} is a unit vector, a=1|\vec{a}| = 1, and squaring gives

(12)2+(12)2+cos2θ=1\left(\tfrac{1}{2}\right)^2 + \left(\tfrac{1}{\sqrt{2}}\right)^2 + \cos^2\theta = 1

14+12+cos2θ=1    cos2θ=134=14\tfrac{1}{4} + \tfrac{1}{2} + \cos^2\theta = 1 \implies \cos^2\theta = 1 - \tfrac{3}{4} = \tfrac{1}{4}

So cosθ=±12\cos\theta = \pm\tfrac{1}{2}. As θ\theta is acute, cosθ=12\cos\theta = \tfrac{1}{2} and θ=π3\theta = \tfrac{\pi}{3}. The components of a\vec{a} are 12\tfrac{1}{2}, 12\tfrac{1}{\sqrt{2}}, and 12\tfrac{1}{2}.

Solving for unknowns that make a cross product zero

Find λ\lambda and μ\mu if (2i+6j+27k)×(i+λj+μk)=0(2\mathbf{i} + 6\mathbf{j} + 27\mathbf{k}) \times (\mathbf{i} + \lambda\mathbf{j} + \mu\mathbf{k}) = \vec{0}.

The cross product is zero, so expand the determinant and set each component to zero:

ijk26271λμ=i(6μ27λ)j(2μ27)+k(2λ6)=0\begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 2 & 6 & 27 \\ 1 & \lambda & \mu \end{vmatrix} = \mathbf{i}(6\mu - 27\lambda) - \mathbf{j}(2\mu - 27) + \mathbf{k}(2\lambda - 6) = \vec{0}

This gives three equations:

6μ27λ=0(1),2μ27=0(2),2λ6=0(3)6\mu - 27\lambda = 0 \quad (1), \qquad 2\mu - 27 = 0 \quad (2), \qquad 2\lambda - 6 = 0 \quad (3)

From (2)(2), μ=272\mu = \tfrac{27}{2}. From (3)(3), λ=3\lambda = 3.

Check in (1). 6272273=8181=06 \cdot \tfrac{27}{2} - 27 \cdot 3 = 81 - 81 = 0, so the values satisfy the first equation. Hence λ=3\lambda = 3 and μ=272\mu = \tfrac{27}{2}.

Angle between two vectors from their cross product

Let a\vec{a} and b\vec{b} satisfy a=3|\vec{a}| = 3 and b=23|\vec{b}| = \tfrac{\sqrt{2}}{3}, and let a×b\vec{a} \times \vec{b} be a unit vector. Find the angle between them.

From a×b=absinθ|\vec{a} \times \vec{b}| = |\vec{a}|\,|\vec{b}|\sin\theta,

sinθ=a×bab=1323=12\sin\theta = \frac{|\vec{a} \times \vec{b}|}{|\vec{a}|\,|\vec{b}|} = \frac{1}{3 \cdot \tfrac{\sqrt{2}}{3}} = \frac{1}{\sqrt{2}}

So θ=π4\theta = \tfrac{\pi}{4}.

Key takeaways

  • A cross product is found by expanding the determinant with the unit vectors in the top row, and its magnitude is the root of the sum of the squares of the components.
  • c×d\vec{c} \times \vec{d} is perpendicular to both c\vec{c} and d\vec{d}; dividing it by its magnitude gives the two perpendicular unit vectors ±n^\pm\hat{n}.
  • For a unit vector, the squares of its direction cosines add to 11, which lets you solve for an unknown angle.
  • If a cross product is the zero vector the vectors are parallel; if it is a unit vector, sinθ=1ab\sin\theta = \dfrac{1}{|\vec{a}|\,|\vec{b}|} gives the angle between them.