How to Use This Section

Twenty-five fully worked problems covering the whole chapter, arranged in five graded batches: unit vectors and components, then resultants and the section formula, then the dot product, then the cross product, and finally mixed miscellaneous-level problems. Attempt each on paper before reading the solution — the worked version is for checking, not for first contact.

A classification habit worth building from the very first example: before computing, name the tool. Lengths and angles → dot product. Perpendiculars and areas → cross product. Points dividing segments → section formula. "Parallel to" or "collinear" → proportional components. Most errors in this chapter are not calculation slips — they are wrong-tool choices made in the first line.

Key Point: marks are lost at setup, not at arithmetic. Writing AB→=b⃗−a⃗\overrightarrow{AB} = \vec{b} - \vec{a} (terminal minus initial) correctly, choosing the dot for an angle, and remembering the 12\dfrac{1}{2} for a triangle's area account for nearly every mark in this chapter.

Batch 1 — Unit Vectors and Components (Easy)

Example 1: All unit vectors in the XY-plane

Write all the unit vectors in the XY-plane.

Solution:

  1. Parametrise by the angle: a unit vector r⃗\vec{r} in the XY-plane making angle θ\theta with the positive xx-axis has components x=cos⁡θx = \cos\theta, y=sin⁡θy = \sin\theta.
  2. Check the magnitude: ∣r⃗∣=cos⁡2θ+sin⁡2θ=1|\vec{r}| = \sqrt{\cos^2\theta + \sin^2\theta} = 1. ✓

Answer: r⃗=cos⁡θ i^+sin⁡θ j^\vec{r} = \cos\theta\,\hat{i} + \sin\theta\,\hat{j}, 0≤θ<2π0 \leq \theta < 2\pi — as θ\theta sweeps a full turn, the tip traces the unit circle and every planar direction appears exactly once.


Example 2: One specific direction

Write a unit vector in the XY-plane making an angle of 30∘30^\circ with the positive xx-axis.

Solution:

  1. Substitute into Example 1's formula: r⃗=cos⁡30∘ i^+sin⁡30∘ j^\vec{r} = \cos 30^\circ\,\hat{i} + \sin 30^\circ\,\hat{j}.

Answer: r⃗=32i^+12j^\vec{r} = \dfrac{\sqrt{3}}{2}\hat{i} + \dfrac{1}{2}\hat{j}.


Example 3: Scaling to unit length

Find the value of xx for which x(i^+j^+k^)x\left(\hat{i} + \hat{j} + \hat{k}\right) is a unit vector.

Solution:

  1. Magnitude condition: ∣x(i^+j^+k^)∣=∣x∣3=1\left|x\left(\hat{i}+\hat{j}+\hat{k}\right)\right| = |x|\sqrt{3} = 1.
  2. Solve: ∣x∣=13|x| = \dfrac{1}{\sqrt{3}}.

Answer: x=±13x = \pm\dfrac{1}{\sqrt{3}} — both signs work; the two answers point in opposite directions along the same line.


Example 4: The joining vector, in general

Find the scalar components and the magnitude of the vector joining P(x1,y1,z1)P(x_1, y_1, z_1) to Q(x2,y2,z2)Q(x_2, y_2, z_2).

Solution:

  1. Terminal minus initial: PQ→=(x2−x1)i^+(y2−y1)j^+(z2−z1)k^\overrightarrow{PQ} = (x_2 - x_1)\hat{i} + (y_2 - y_1)\hat{j} + (z_2 - z_1)\hat{k}.
  2. Magnitude: ∣PQ→∣=(x2−x1)2+(y2−y1)2+(z2−z1)2\left|\overrightarrow{PQ}\right| = \sqrt{(x_2-x_1)^2 + (y_2-y_1)^2 + (z_2-z_1)^2}.

Answer: components (x2−x1), (y2−y1), (z2−z1)(x_2 - x_1),\ (y_2 - y_1),\ (z_2 - z_1); magnitude as above — the distance formula is just the length of a joining vector.


Example 5: A two-leg walk

A girl walks 44 km towards the west, then 33 km in a direction 30∘30^\circ east of north, and stops. Find her displacement from the starting point.

Solution:

  1. Set axes: east =i^= \hat{i}, north =j^= \hat{j}. First leg: −4i^-4\hat{i}.
  2. Second leg: "30∘30^\circ east of north" tilts from north towards east: 3(sin⁡30∘ i^+cos⁡30∘ j^)=32i^+332j^3\left(\sin 30^\circ\,\hat{i} + \cos 30^\circ\,\hat{j}\right) = \dfrac{3}{2}\hat{i} + \dfrac{3\sqrt{3}}{2}\hat{j}.
  3. Add: (−4+32)i^+332j^=−52i^+332j^\left(-4 + \dfrac{3}{2}\right)\hat{i} + \dfrac{3\sqrt{3}}{2}\hat{j} = -\dfrac{5}{2}\hat{i} + \dfrac{3\sqrt{3}}{2}\hat{j}.
  4. Magnitude: 254+274=13\sqrt{\dfrac{25}{4} + \dfrac{27}{4}} = \sqrt{13} km.

Answer: −52i^+332j^-\dfrac{5}{2}\hat{i} + \dfrac{3\sqrt{3}}{2}\hat{j}, of magnitude 13\sqrt{13} km — the angle in "east of north" measures from north, which is why sine goes with i^\hat{i} here.

Batch 2 — Resultants, Collinearity, and the Section Formula (Easy-Medium)

Example 6: A vector of magnitude 5 along a resultant

Find a vector of magnitude 55 units parallel to the resultant of a⃗=2i^+3j^−k^\vec{a} = 2\hat{i} + 3\hat{j} - \hat{k} and b⃗=i^−2j^+k^\vec{b} = \hat{i} - 2\hat{j} + \hat{k}.

Solution:

  1. Resultant: a⃗+b⃗=3i^+j^\vec{a} + \vec{b} = 3\hat{i} + \hat{j}, magnitude 10\sqrt{10}.
  2. Normalise and scale: ±5⋅3i^+j^10=±102(3i^+j^)\pm 5 \cdot \dfrac{3\hat{i} + \hat{j}}{\sqrt{10}} = \pm\dfrac{\sqrt{10}}{2}\left(3\hat{i} + \hat{j}\right).

Answer: ±(3102i^+102j^)\pm\left(\dfrac{3\sqrt{10}}{2}\hat{i} + \dfrac{\sqrt{10}}{2}\hat{j}\right) — "parallel to" admits both signs.


Example 7: A unit vector parallel to a combination

If a⃗=i^+j^+k^\vec{a} = \hat{i} + \hat{j} + \hat{k}, b⃗=2i^−j^+3k^\vec{b} = 2\hat{i} - \hat{j} + 3\hat{k} and c⃗=i^−2j^+k^\vec{c} = \hat{i} - 2\hat{j} + \hat{k}, find a unit vector parallel to 2a⃗−b⃗+3c⃗2\vec{a} - \vec{b} + 3\vec{c}.

Solution:

  1. Combine componentwise: 2a⃗−b⃗+3c⃗=(2−2+3)i^+(2+1−6)j^+(2−3+3)k^=3i^−3j^+2k^2\vec{a} - \vec{b} + 3\vec{c} = (2 - 2 + 3)\hat{i} + (2 + 1 - 6)\hat{j} + (2 - 3 + 3)\hat{k} = 3\hat{i} - 3\hat{j} + 2\hat{k}.
  2. Magnitude: 9+9+4=22\sqrt{9 + 9 + 4} = \sqrt{22}.

Answer: ±122(3i^−3j^+2k^)\pm\dfrac{1}{\sqrt{22}}\left(3\hat{i} - 3\hat{j} + 2\hat{k}\right).


Example 8: Collinear points and the dividing ratio

Show that A(1,−2,−8)A(1, -2, -8), B(5,0,−2)B(5, 0, -2) and C(11,3,7)C(11, 3, 7) are collinear, and find the ratio in which BB divides ACAC.

Solution:

  1. Joining vectors: AB→=4i^+2j^+6k^\overrightarrow{AB} = 4\hat{i} + 2\hat{j} + 6\hat{k}, BC→=6i^+3j^+9k^\overrightarrow{BC} = 6\hat{i} + 3\hat{j} + 9\hat{k}.
  2. Proportionality: BC→=32AB→\overrightarrow{BC} = \dfrac{3}{2}\overrightarrow{AB} — parallel vectors sharing the point BB: collinear. ✓
  3. Ratio: AB:BC=2:3AB : BC = 2 : 3, so BB divides ACAC internally in the ratio 2:32 : 3.
  4. Check with the section formula: 2c⃗+3a⃗5=(22+3, 6−6, 14−24)5=(5,0,−2)=b⃗\dfrac{2\vec{c} + 3\vec{a}}{5} = \dfrac{(22 + 3, \ 6 - 6, \ 14 - 24)}{5} = (5, 0, -2) = \vec{b}. ✓

Answer: collinear, with BB dividing ACAC in the ratio 2:32 : 3 internally.


Example 9: External division, and a midpoint that appears for free

PP and QQ have position vectors 2a⃗+b⃗2\vec{a} + \vec{b} and a⃗−3b⃗\vec{a} - 3\vec{b}. Find the position vector of RR dividing PQPQ externally in the ratio 1:21 : 2, and show that PP is the midpoint of RQRQ.

Solution:

  1. External formula with m:n=1:2m : n = 1 : 2: r⃗=1⋅(a⃗−3b⃗)−2(2a⃗+b⃗)1−2=−3a⃗−5b⃗−1=3a⃗+5b⃗\vec{r} = \dfrac{1\cdot\left(\vec{a} - 3\vec{b}\right) - 2\left(2\vec{a} + \vec{b}\right)}{1 - 2} = \dfrac{-3\vec{a} - 5\vec{b}}{-1} = 3\vec{a} + 5\vec{b}.
  2. Midpoint of RQRQ: (3a⃗+5b⃗)+(a⃗−3b⃗)2=4a⃗+2b⃗2=2a⃗+b⃗\dfrac{\left(3\vec{a} + 5\vec{b}\right) + \left(\vec{a} - 3\vec{b}\right)}{2} = \dfrac{4\vec{a} + 2\vec{b}}{2} = 2\vec{a} + \vec{b} — precisely PP. ✓

Answer: r⃗=3a⃗+5b⃗\vec{r} = 3\vec{a} + 5\vec{b}, and PP is the midpoint of RQRQ — external division in 1:21:2 always places the original first point midway between the new point and the second.


Example 10: An angle that turns out straight

The points A,B,C,DA, B, C, D have position vectors i^+j^+k^\hat{i} + \hat{j} + \hat{k}, 2i^+5j^2\hat{i} + 5\hat{j}, 3i^+2j^−3k^3\hat{i} + 2\hat{j} - 3\hat{k} and i^−6j^−k^\hat{i} - 6\hat{j} - \hat{k}. Find the angle between AB→\overrightarrow{AB} and CD→\overrightarrow{CD}, and deduce that they are collinear.

Solution:

  1. Joining vectors: AB→=i^+4j^−k^\overrightarrow{AB} = \hat{i} + 4\hat{j} - \hat{k} (magnitude 323\sqrt{2}), CD→=−2i^−8j^+2k^\overrightarrow{CD} = -2\hat{i} - 8\hat{j} + 2\hat{k} (magnitude 626\sqrt{2}).
  2. Cosine: cos⁡θ=−2−32−2(32)(62)=−3636=−1\cos\theta = \dfrac{-2 - 32 - 2}{\left(3\sqrt{2}\right)\left(6\sqrt{2}\right)} = \dfrac{-36}{36} = -1.
  3. Read the angle: θ=π\theta = \pi.

Answer: θ=π\theta = \pi — the vectors are anti-parallel, hence collinear. Faster still: CD→=−2AB→\overrightarrow{CD} = -2\overrightarrow{AB} by inspection.

Batch 3 — Dot Product (Medium)

Example 11: Perpendicular to the sum of the others

Let a⃗,b⃗,c⃗\vec{a}, \vec{b}, \vec{c} satisfy ∣a⃗∣=3|\vec{a}| = 3, ∣b⃗∣=4|\vec{b}| = 4, ∣c⃗∣=5|\vec{c}| = 5, each perpendicular to the sum of the other two. Find ∣a⃗+b⃗+c⃗∣\left|\vec{a} + \vec{b} + \vec{c}\right|.

Solution:

  1. Write the given conditions as dots: a⃗⋅(b⃗+c⃗)=0\vec{a}\cdot\left(\vec{b}+\vec{c}\right) = 0, b⃗⋅(c⃗+a⃗)=0\vec{b}\cdot\left(\vec{c}+\vec{a}\right) = 0, c⃗⋅(a⃗+b⃗)=0\vec{c}\cdot\left(\vec{a}+\vec{b}\right) = 0.
  2. Square the sum: ∣a⃗+b⃗+c⃗∣2=∣a⃗∣2+∣b⃗∣2+∣c⃗∣2+2(a⃗⋅b⃗+b⃗⋅c⃗+c⃗⋅a⃗)\left|\vec{a}+\vec{b}+\vec{c}\right|^2 = |\vec{a}|^2 + |\vec{b}|^2 + |\vec{c}|^2 + 2\left(\vec{a}\cdot\vec{b} + \vec{b}\cdot\vec{c} + \vec{c}\cdot\vec{a}\right).
  3. The cross terms are the given conditions in disguise: adding the three conditions gives 2(a⃗⋅b⃗+b⃗⋅c⃗+c⃗⋅a⃗)=02\left(\vec{a}\cdot\vec{b} + \vec{b}\cdot\vec{c} + \vec{c}\cdot\vec{a}\right) = 0.
  4. Finish: ∣a⃗+b⃗+c⃗∣2=9+16+25=50\left|\vec{a}+\vec{b}+\vec{c}\right|^2 = 9 + 16 + 25 = 50.

Answer: ∣a⃗+b⃗+c⃗∣=52\left|\vec{a}+\vec{b}+\vec{c}\right| = 5\sqrt{2}.


Example 12: Evaluating a sum of dots

Three vectors with ∣a⃗∣=2|\vec{a}| = 2, ∣b⃗∣=3|\vec{b}| = 3, ∣c⃗∣=4|\vec{c}| = 4 satisfy a⃗+b⃗+c⃗=0⃗\vec{a} + \vec{b} + \vec{c} = \vec{0}. Evaluate μ=a⃗⋅b⃗+b⃗⋅c⃗+c⃗⋅a⃗\mu = \vec{a}\cdot\vec{b} + \vec{b}\cdot\vec{c} + \vec{c}\cdot\vec{a}.

Solution:

  1. Square the zero: 0=∣a⃗+b⃗+c⃗∣2=∣a⃗∣2+∣b⃗∣2+∣c⃗∣2+2μ0 = \left|\vec{a}+\vec{b}+\vec{c}\right|^2 = |\vec{a}|^2 + |\vec{b}|^2 + |\vec{c}|^2 + 2\mu.
  2. Substitute: 0=4+9+16+2μ=29+2μ0 = 4 + 9 + 16 + 2\mu = 29 + 2\mu.

Answer: μ=−292\mu = -\dfrac{29}{2} — the "square the sum" identity again, run backwards.


Example 13: A unit-vector condition fixes a parameter

The scalar product of i^+j^+k^\hat{i} + \hat{j} + \hat{k} with the unit vector along the sum of 2i^+4j^−5k^2\hat{i} + 4\hat{j} - 5\hat{k} and λi^+2j^+3k^\lambda\hat{i} + 2\hat{j} + 3\hat{k} equals 11. Find λ\lambda.

Solution:

  1. The sum: s⃗=(2+λ)i^+6j^−2k^\vec{s} = (2 + \lambda)\hat{i} + 6\hat{j} - 2\hat{k}, with ∣s⃗∣=(2+λ)2+40|\vec{s}| = \sqrt{(2+\lambda)^2 + 40}.
  2. The condition: (i^+j^+k^)⋅s⃗∣s⃗∣=λ+6(2+λ)2+40=1\dfrac{\left(\hat{i}+\hat{j}+\hat{k}\right)\cdot\vec{s}}{|\vec{s}|} = \dfrac{\lambda + 6}{\sqrt{(2+\lambda)^2 + 40}} = 1.
  3. Square and solve: (λ+6)2=(λ+2)2+40⇒12λ+36=4λ+44⇒8λ=8(\lambda + 6)^2 = (\lambda + 2)^2 + 40 \Rightarrow 12\lambda + 36 = 4\lambda + 44 \Rightarrow 8\lambda = 8.

Answer: λ=1\lambda = 1 (and it satisfies the unsquared equation, since λ+6=7>0\lambda + 6 = 7 > 0).


Example 14: Equally inclined to three perpendicular directions

If a⃗,b⃗,c⃗\vec{a}, \vec{b}, \vec{c} are mutually perpendicular vectors of equal magnitude, show that a⃗+b⃗+c⃗\vec{a} + \vec{b} + \vec{c} is equally inclined to each of them.

Solution:

  1. Common data: let ∣a⃗∣=∣b⃗∣=∣c⃗∣=m|\vec{a}| = |\vec{b}| = |\vec{c}| = m; all pairwise dots vanish.
  2. Length of the sum: ∣a⃗+b⃗+c⃗∣2=3m2\left|\vec{a}+\vec{b}+\vec{c}\right|^2 = 3m^2, so ∣a⃗+b⃗+c⃗∣=m3\left|\vec{a}+\vec{b}+\vec{c}\right| = m\sqrt{3}.
  3. Angle with a⃗\vec{a}: cos⁡θa=(a⃗+b⃗+c⃗)⋅a⃗m3⋅m=m23m2=13\cos\theta_a = \dfrac{\left(\vec{a}+\vec{b}+\vec{c}\right)\cdot\vec{a}}{m\sqrt{3}\cdot m} = \dfrac{m^2}{\sqrt{3}m^2} = \dfrac{1}{\sqrt{3}} — and identically for b⃗\vec{b} and c⃗\vec{c}.

Answer: each angle is cos⁡−113\cos^{-1}\dfrac{1}{\sqrt{3}} — the body-diagonal of a cube makes equal angles with its three edges.


Example 15: Equal diagonals detect a right angle

Prove that ∣a⃗+b⃗∣=∣a⃗−b⃗∣\left|\vec{a} + \vec{b}\right| = \left|\vec{a} - \vec{b}\right| if and only if a⃗\vec{a} and b⃗\vec{b} are perpendicular (both nonzero).

Solution:

  1. Square both sides: ∣a⃗∣2+2a⃗⋅b⃗+∣b⃗∣2=∣a⃗∣2−2a⃗⋅b⃗+∣b⃗∣2|\vec{a}|^2 + 2\vec{a}\cdot\vec{b} + |\vec{b}|^2 = |\vec{a}|^2 - 2\vec{a}\cdot\vec{b} + |\vec{b}|^2.
  2. Cancel: 4 a⃗⋅b⃗=0  ⟺  a⃗⋅b⃗=0  ⟺  a⃗⊥b⃗4\,\vec{a}\cdot\vec{b} = 0 \iff \vec{a}\cdot\vec{b} = 0 \iff \vec{a} \perp \vec{b}.

Answer: proved — geometrically, a parallelogram has equal diagonals exactly when it is a rectangle.

Batch 4 — Cross Product (Medium)

Example 16: Diagonal and area of a parallelogram

The adjacent sides of a parallelogram are a⃗=2i^−4j^+5k^\vec{a} = 2\hat{i} - 4\hat{j} + 5\hat{k} and b⃗=i^−2j^−3k^\vec{b} = \hat{i} - 2\hat{j} - 3\hat{k}. Find a unit vector parallel to its diagonal, and its area.

Solution:

  1. Diagonal (through the common vertex): a⃗+b⃗=3i^−6j^+2k^\vec{a} + \vec{b} = 3\hat{i} - 6\hat{j} + 2\hat{k}, magnitude 9+36+4=7\sqrt{9 + 36 + 4} = 7; unit vector 17(3i^−6j^+2k^)\dfrac{1}{7}\left(3\hat{i} - 6\hat{j} + 2\hat{k}\right).
  2. Area: a⃗×b⃗=∣i^j^k^2−451−2−3∣=(12+10)i^−(−6−5)j^+(−4+4)k^=22i^+11j^\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & -4 & 5 \\ 1 & -2 & -3 \end{vmatrix} = (12 + 10)\hat{i} - (-6 - 5)\hat{j} + (-4 + 4)\hat{k} = 22\hat{i} + 11\hat{j}.
  3. Magnitude: 484+121=115\sqrt{484 + 121} = 11\sqrt{5}.

Answer: unit diagonal 17(3i^−6j^+2k^)\dfrac{1}{7}\left(3\hat{i} - 6\hat{j} + 2\hat{k}\right); area 11511\sqrt{5} square units.


Example 17: Perpendicular to two vectors with a prescribed dot

Let a⃗=i^+4j^+2k^\vec{a} = \hat{i} + 4\hat{j} + 2\hat{k}, b⃗=3i^−2j^+7k^\vec{b} = 3\hat{i} - 2\hat{j} + 7\hat{k}, c⃗=2i^−j^+4k^\vec{c} = 2\hat{i} - \hat{j} + 4\hat{k}. Find a vector d⃗\vec{d} perpendicular to both a⃗\vec{a} and b⃗\vec{b} with c⃗⋅d⃗=15\vec{c}\cdot\vec{d} = 15.

Solution:

  1. Perpendicular to both means parallel to the cross: d⃗=λ(a⃗×b⃗)\vec{d} = \lambda\left(\vec{a} \times \vec{b}\right), and a⃗×b⃗=(28+4)i^−(7−6)j^+(−2−12)k^=32i^−j^−14k^\vec{a} \times \vec{b} = (28 + 4)\hat{i} - (7 - 6)\hat{j} + (-2 - 12)\hat{k} = 32\hat{i} - \hat{j} - 14\hat{k}.
  2. Apply the dot condition: c⃗⋅(a⃗×b⃗)=64+1−56=9\vec{c}\cdot\left(\vec{a}\times\vec{b}\right) = 64 + 1 - 56 = 9, so 9λ=159\lambda = 15 and λ=53\lambda = \dfrac{5}{3}.

Answer: d⃗=53(32i^−j^−14k^)=13(160i^−5j^−70k^)\vec{d} = \dfrac{5}{3}\left(32\hat{i} - \hat{j} - 14\hat{k}\right) = \dfrac{1}{3}\left(160\hat{i} - 5\hat{j} - 70\hat{k}\right).


Example 18: Splitting a vector along and across a direction

With α⃗=3i^−j^\vec{\alpha} = 3\hat{i} - \hat{j} and β⃗=2i^+j^−3k^\vec{\beta} = 2\hat{i} + \hat{j} - 3\hat{k}, express β⃗=β⃗1+β⃗2\vec{\beta} = \vec{\beta}_1 + \vec{\beta}_2 where β⃗1∥α⃗\vec{\beta}_1 \parallel \vec{\alpha} and β⃗2⊥α⃗\vec{\beta}_2 \perp \vec{\alpha}.

Solution:

  1. Set up: β⃗1=λα⃗=3λi^−λj^\vec{\beta}_1 = \lambda\vec{\alpha} = 3\lambda\hat{i} - \lambda\hat{j}, so β⃗2=β⃗−λα⃗=(2−3λ)i^+(1+λ)j^−3k^\vec{\beta}_2 = \vec{\beta} - \lambda\vec{\alpha} = (2 - 3\lambda)\hat{i} + (1 + \lambda)\hat{j} - 3\hat{k}.
  2. Perpendicularity: β⃗2⋅α⃗=3(2−3λ)−(1+λ)=5−10λ=0\vec{\beta}_2\cdot\vec{\alpha} = 3(2 - 3\lambda) - (1 + \lambda) = 5 - 10\lambda = 0, so λ=12\lambda = \dfrac{1}{2}.
  3. Read off both parts: β⃗1=32i^−12j^\vec{\beta}_1 = \dfrac{3}{2}\hat{i} - \dfrac{1}{2}\hat{j} and β⃗2=12i^+32j^−3k^\vec{\beta}_2 = \dfrac{1}{2}\hat{i} + \dfrac{3}{2}\hat{j} - 3\hat{k}.

Answer: β⃗=(32i^−12j^)+(12i^+32j^−3k^)\vec{\beta} = \left(\dfrac{3}{2}\hat{i} - \dfrac{1}{2}\hat{j}\right) + \left(\dfrac{1}{2}\hat{i} + \dfrac{3}{2}\hat{j} - 3\hat{k}\right) — resolution along and perpendicular to a direction, the decomposition JEE loves.


Example 19: The same angle by two roads

For a⃗=i^+j^\vec{a} = \hat{i} + \hat{j} and b⃗=j^+k^\vec{b} = \hat{j} + \hat{k}, find the angle between them using the dot product, and confirm it with the cross product.

Solution:

  1. Dot route: a⃗⋅b⃗=1\vec{a}\cdot\vec{b} = 1, ∣a⃗∣∣b⃗∣=2|\vec{a}||\vec{b}| = 2, so cos⁡θ=12\cos\theta = \dfrac{1}{2} and θ=60∘\theta = 60^\circ.
  2. Cross route: a⃗×b⃗=i^−j^+k^\vec{a} \times \vec{b} = \hat{i} - \hat{j} + \hat{k}, magnitude 3\sqrt{3}, so sin⁡θ=32\sin\theta = \dfrac{\sqrt{3}}{2} — again θ=60∘\theta = 60^\circ. ✓

Answer: 60∘60^\circ by both routes. When only sin⁡θ\sin\theta is computed, remember it cannot distinguish θ\theta from π−θ\pi - \theta — the dot product's sign settles which; here the positive dot confirms the acute choice.


Example 20: An identity worth knowing

Show that (a⃗−b⃗)×(a⃗+b⃗)=2(a⃗×b⃗)\left(\vec{a} - \vec{b}\right) \times \left(\vec{a} + \vec{b}\right) = 2\left(\vec{a} \times \vec{b}\right).

Solution:

  1. Expand by distributivity: a⃗×a⃗+a⃗×b⃗−b⃗×a⃗−b⃗×b⃗\vec{a}\times\vec{a} + \vec{a}\times\vec{b} - \vec{b}\times\vec{a} - \vec{b}\times\vec{b}.
  2. Kill the self-crosses and flip the reversed one: =0⃗+a⃗×b⃗+a⃗×b⃗−0⃗= \vec{0} + \vec{a}\times\vec{b} + \vec{a}\times\vec{b} - \vec{0}.

Answer: 2(a⃗×b⃗)2\left(\vec{a}\times\vec{b}\right) — geometrically: the parallelogram on the two diagonals has twice the area of the one on the sides.

Batch 5 — Mixed Problems (Medium-Hard)

Example 21: Length of a combination

If ∣a⃗∣=2|\vec{a}| = 2, ∣b⃗∣=5|\vec{b}| = 5 and the angle between them is 60∘60^\circ, find ∣2a⃗+b⃗∣\left|2\vec{a} + \vec{b}\right|.

Solution:

  1. Dot first: a⃗⋅b⃗=2×5×cos⁡60∘=5\vec{a}\cdot\vec{b} = 2 \times 5 \times \cos 60^\circ = 5.
  2. Expand: ∣2a⃗+b⃗∣2=4∣a⃗∣2+4 a⃗⋅b⃗+∣b⃗∣2=16+20+25=61\left|2\vec{a}+\vec{b}\right|^2 = 4|\vec{a}|^2 + 4\,\vec{a}\cdot\vec{b} + |\vec{b}|^2 = 16 + 20 + 25 = 61.

Answer: ∣2a⃗+b⃗∣=61\left|2\vec{a}+\vec{b}\right| = \sqrt{61}.


Example 22: The fourth vertex of a parallelogram

Three vertices of parallelogram ABCDABCD (in order) are A(1,1,1)A(1, 1, 1), B(2,3,4)B(2, 3, 4), C(4,5,6)C(4, 5, 6). Find DD.

Solution:

  1. Opposite sides equal: AD→=BC→\overrightarrow{AD} = \overrightarrow{BC}, so d⃗−a⃗=c⃗−b⃗\vec{d} - \vec{a} = \vec{c} - \vec{b}.
  2. Solve: d⃗=a⃗+c⃗−b⃗=(1+4−2, 1+5−3, 1+6−4)=(3,3,3)\vec{d} = \vec{a} + \vec{c} - \vec{b} = (1 + 4 - 2, \ 1 + 5 - 3, \ 1 + 6 - 4) = (3, 3, 3).

Answer: D(3,3,3)D(3, 3, 3). Equivalent check: the diagonals bisect each other — the midpoint of ACAC is (52,3,72)\left(\frac{5}{2}, 3, \frac{7}{2}\right), which is also the midpoint of BDBD. ✓


Example 23: One length forces another

Unit vectors a^\hat{a} and b^\hat{b} satisfy ∣a^+b^∣=1\left|\hat{a} + \hat{b}\right| = 1. Find ∣a^−b^∣\left|\hat{a} - \hat{b}\right|.

Solution:

  1. Square the given: 1=1+1+2a^⋅b^1 = 1 + 1 + 2\hat{a}\cdot\hat{b}, so a^⋅b^=−12\hat{a}\cdot\hat{b} = -\dfrac{1}{2} (the angle is 120∘120^\circ).
  2. Square the target: ∣a^−b^∣2=2−2a^⋅b^=2+1=3\left|\hat{a}-\hat{b}\right|^2 = 2 - 2\hat{a}\cdot\hat{b} = 2 + 1 = 3.

Answer: ∣a^−b^∣=3\left|\hat{a} - \hat{b}\right| = \sqrt{3} — the two diagonal lengths of a unit rhombus always satisfy d12+d22=4d_1^2 + d_2^2 = 4.


Example 24: Projection, and the perpendicular remainder

For a⃗=i^+2j^+k^\vec{a} = \hat{i} + 2\hat{j} + \hat{k} and b⃗=2i^+j^+2k^\vec{b} = 2\hat{i} + \hat{j} + 2\hat{k}, find the projection of a⃗\vec{a} on b⃗\vec{b}, the vector component of a⃗\vec{a} along b⃗\vec{b}, and the component perpendicular to b⃗\vec{b}.

Solution:

  1. Projection (a number): a⃗⋅b⃗∣b⃗∣=2+2+23=2\dfrac{\vec{a}\cdot\vec{b}}{|\vec{b}|} = \dfrac{2 + 2 + 2}{3} = 2.
  2. Component along b⃗\vec{b} (a vector): (a⃗⋅b⃗∣b⃗∣2)b⃗=69b⃗=23(2i^+j^+2k^)\left(\dfrac{\vec{a}\cdot\vec{b}}{|\vec{b}|^2}\right)\vec{b} = \dfrac{6}{9}\vec{b} = \dfrac{2}{3}\left(2\hat{i} + \hat{j} + 2\hat{k}\right).
  3. Perpendicular remainder: a⃗−23b⃗=−13i^+43j^−13k^\vec{a} - \dfrac{2}{3}\vec{b} = -\dfrac{1}{3}\hat{i} + \dfrac{4}{3}\hat{j} - \dfrac{1}{3}\hat{k}; check (−13,43,−13)⋅(2,1,2)=0\left(-\dfrac{1}{3}, \dfrac{4}{3}, -\dfrac{1}{3}\right)\cdot(2, 1, 2) = 0. ✓

Answer: projection 22; along-component 23b⃗\dfrac{2}{3}\vec{b}; perpendicular component 13(−i^+4j^−k^)\dfrac{1}{3}\left(-\hat{i} + 4\hat{j} - \hat{k}\right).


Example 25: Rhombus diagonals, in two lines

Prove by vectors that the diagonals of a rhombus are perpendicular.

Solution:

  1. Set up: let the sides from one vertex be a⃗\vec{a} and b⃗\vec{b} with ∣a⃗∣=∣b⃗∣|\vec{a}| = |\vec{b}| (that is what makes it a rhombus). The diagonals are a⃗+b⃗\vec{a} + \vec{b} and a⃗−b⃗\vec{a} - \vec{b}.
  2. Dot the diagonals: (a⃗+b⃗)⋅(a⃗−b⃗)=∣a⃗∣2−∣b⃗∣2=0\left(\vec{a}+\vec{b}\right)\cdot\left(\vec{a}-\vec{b}\right) = |\vec{a}|^2 - |\vec{b}|^2 = 0.

Answer: the dot product of the diagonals vanishes, so they are perpendicular — a two-line proof of a classical theorem, and the template for most vector-geometry proofs: encode the figure in a⃗,b⃗\vec{a}, \vec{b}, then compute one dot or cross.