This Class 12 Maths NCERT Solutions Chapter 10 Ex 10.3 page covers all 18 questions, solved step-by-step, on the scalar (dot) product — the operation \vec{a}\cdot\vec{b}=|\vec{a}||\vec{b}|\cos\theta that turns two vectors into a single number, and quietly does the heavy lifting behind angle, projection and perpendicularity questions throughout the rest of the chapter.
Questions 1–9 are the exercise's computational backbone: finding the angle between two vectors from their dot product, computing a projection, and using the identity \vec{a}\cdot\vec{a}=|\vec{a}|^2 to expand expressions like (\vec{a}+\vec{b})\cdot(\vec{a}-\vec{b}) — a technique CBSE reuses in nearly every 2019–2026 sample paper. Questions 10–14 shift to the perpendicularity condition \vec{a}\cdot\vec{b}=0, including the "converse need not be true" justification that examiners specifically like testing conceptually rather than numerically. Questions 15–17 apply the dot product to triangles — finding an angle from position vectors, proving three points collinear, and proving a right angle using the Pythagoras converse — question types that also show up, almost unchanged, in Chapter 11 (Three Dimensional Geometry). The exercise closes with an MCQ on unit vectors (18).
\cos\theta = \dfrac{\vec{a}\cdot\vec{b}}{|\vec{a}||\vec{b}|} = \dfrac{\sqrt6}{\sqrt3\cdot 2} = \dfrac{\sqrt6}{2\sqrt3} = \dfrac{\sqrt2}{2} = \dfrac{1}{\sqrt2}.
Let \vec{a}=\hat{i}-2\hat{j}+3\hat{k} and \vec{b}=3\hat{i}-2\hat{j}+\hat{k}.
\vec{a}\cdot\vec{b} = 1(3)+(-2)(-2)+3(1) = 3+4+3 = 10.
|\vec{a}| = \sqrt{1+4+9}=\sqrt{14}, |\vec{b}| = \sqrt{9+4+1}=\sqrt{14}.
\cos\theta = \dfrac{10}{\sqrt{14}\cdot\sqrt{14}} = \dfrac{10}{14} = \dfrac57.
Projection of \vec{a} on \vec{b} is \dfrac{\vec{a}\cdot\vec{b}}{|\vec{b}|}.
Here \vec{a}\cdot\vec{b} = (1)(1)+(-1)(1) = 1-1 = 0.
\vec{a}\cdot\vec{b} = 1(7)+3(-1)+7(8) = 7-3+56 = 60.
|\vec{b}| = \sqrt{49+1+64} = \sqrt{114}.
Let \vec{a}=\frac17(2\hat{i}+3\hat{j}+6\hat{k}), \vec{b}=\frac17(3\hat{i}-6\hat{j}+2\hat{k}), \vec{c}=\frac17(6\hat{i}+2\hat{j}-3\hat{k}).
|\vec{a}| = \frac17\sqrt{4+9+36}=\frac17\sqrt{49}=\frac77=1. Similarly |\vec{b}|=\frac17\sqrt{9+36+4}=1 and |\vec{c}|=\frac17\sqrt{36+4+9}=1. All three are unit vectors.
\vec{a}\cdot\vec{b} = \frac{1}{49}[2(3)+3(-6)+6(2)] = \frac{1}{49}[6-18+12] = 0.
\vec{b}\cdot\vec{c} = \frac{1}{49}[3(6)+(-6)(2)+2(-3)] = \frac{1}{49}[18-12-6] = 0.
\vec{a}\cdot\vec{c} = \frac{1}{49}[2(6)+3(2)+6(-3)] = \frac{1}{49}[12+6-18] = 0.
(\vec{a}+\vec{b})\cdot(\vec{a}-\vec{b}) = |\vec{a}|^2-|\vec{b}|^2 = 8.
Substituting |\vec{a}|=8|\vec{b}|: 64|\vec{b}|^2-|\vec{b}|^2=8 \Rightarrow 63|\vec{b}|^2=8 \Rightarrow |\vec{b}|^2=\dfrac{8}{63}.
|\vec{b}| = \sqrt{\dfrac{8}{63}} = \dfrac{2\sqrt{14}}{21}, and |\vec{a}| = 8|\vec{b}| = \dfrac{16\sqrt{14}}{21}.
Expanding using distributivity: (3\vec{a}-5\vec{b})\cdot(2\vec{a}+7\vec{b}) = 6(\vec{a}\cdot\vec{a})+21(\vec{a}\cdot\vec{b})-10(\vec{b}\cdot\vec{a})-35(\vec{b}\cdot\vec{b}).
Since \vec{a}\cdot\vec{b}=\vec{b}\cdot\vec{a}, the middle terms combine to 11(\vec{a}\cdot\vec{b}).
Let |\vec{a}|=|\vec{b}|=x. Then \vec{a}\cdot\vec{b} = x\cdot x\cdot\cos60^\circ = x^2\cdot\dfrac12 = \dfrac12.
So x^2=1 \Rightarrow x=1 (magnitude is non-negative).
(\vec{x}-\vec{a})\cdot(\vec{x}+\vec{a}) = |\vec{x}|^2-|\vec{a}|^2 = 12.
Since \vec{a} is a unit vector, |\vec{a}|^2=1, so |\vec{x}|^2 = 13.
Perpendicularity requires (\vec{a}+\lambda\vec{b})\cdot\vec{c}=0, i.e. \vec{a}\cdot\vec{c}+\lambda(\vec{b}\cdot\vec{c})=0.
\vec{a}\cdot\vec{c} = 2(3)+2(1)+3(0) = 8.
\vec{b}\cdot\vec{c} = -1(3)+2(1)+1(0) = -1.
So 8-\lambda=0.
(|\vec{a}|\vec{b}+|\vec{b}|\vec{a})\cdot(|\vec{a}|\vec{b}-|\vec{b}|\vec{a}) = |\vec{a}|^2(\vec{b}\cdot\vec{b}) - |\vec{a}||\vec{b}|(\vec{b}\cdot\vec{a}) + |\vec{a}||\vec{b}|(\vec{a}\cdot\vec{b}) - |\vec{b}|^2(\vec{a}\cdot\vec{a}).
= |\vec{a}|^2|\vec{b}|^2 - |\vec{a}|^2|\vec{b}|^2 = 0 (using \vec{a}\cdot\vec{b}=\vec{b}\cdot\vec{a}, so the two middle terms cancel and the remaining terms are equal and opposite).
\vec{a}\cdot\vec{a}=0 \Rightarrow |\vec{a}|^2=0 \Rightarrow \vec{a}=\vec{0}, the zero vector.
Since the zero vector's dot product with any vector is automatically 0, the condition \vec{a}\cdot\vec{b}=0 holds no matter what \vec{b} is.
Squaring: (\vec{a}+\vec{b}+\vec{c})\cdot(\vec{a}+\vec{b}+\vec{c}) = 0.
|\vec{a}|^2+|\vec{b}|^2+|\vec{c}|^2+2(\vec{a}\cdot\vec{b}+\vec{b}\cdot\vec{c}+\vec{c}\cdot\vec{a})=0.
Since each is a unit vector, 1+1+1+2(\vec{a}\cdot\vec{b}+\vec{b}\cdot\vec{c}+\vec{c}\cdot\vec{a})=0.
Take \vec{a}=\hat{i} and \vec{b}=\hat{j}, both nonzero vectors.
\vec{a}\cdot\vec{b} = \hat{i}\cdot\hat{j} = 0, since they are mutually perpendicular unit vectors.
\vec{BA} = (1-(-1))\hat{i}+(2-0)\hat{j}+(3-0)\hat{k} = 2\hat{i}+2\hat{j}+3\hat{k}.
\vec{BC} = (0-(-1))\hat{i}+(1-0)\hat{j}+(2-0)\hat{k} = \hat{i}+\hat{j}+2\hat{k}.
\vec{BA}\cdot\vec{BC} = 2(1)+2(1)+3(2) = 2+2+6=10.
|\vec{BA}| = \sqrt{4+4+9}=\sqrt{17}, |\vec{BC}| = \sqrt{1+1+4}=\sqrt6.
\cos(\angle ABC) = \dfrac{10}{\sqrt{17}\cdot\sqrt6} = \dfrac{10}{\sqrt{102}}.
\vec{AB} = (2-1)\hat{i}+(6-2)\hat{j}+(3-7)\hat{k} = \hat{i}+4\hat{j}-4\hat{k}, so |\vec{AB}|=\sqrt{1+16+16}=\sqrt{33}.
\vec{BC} = (3-2)\hat{i}+(10-6)\hat{j}+(-1-3)\hat{k} = \hat{i}+4\hat{j}-4\hat{k}, so |\vec{BC}|=\sqrt{33}.
\vec{AC} = (3-1)\hat{i}+(10-2)\hat{j}+(-1-7)\hat{k} = 2\hat{i}+8\hat{j}-8\hat{k}, so |\vec{AC}|=\sqrt{4+64+64}=\sqrt{132}=2\sqrt{33}.
Since |\vec{AC}| = |\vec{AB}|+|\vec{BC}| (as \sqrt{33}+\sqrt{33}=2\sqrt{33}), the three points lie on the same straight line.
Let these be the position vectors of A, B, C respectively: \vec{a}=2\hat{i}-\hat{j}+\hat{k}, \vec{b}=\hat{i}-3\hat{j}-5\hat{k}, \vec{c}=3\hat{i}-4\hat{j}-4\hat{k}.
\vec{AB}=\vec{b}-\vec{a}=-\hat{i}-2\hat{j}-6\hat{k}, so |\vec{AB}|^2=1+4+36=41.
\vec{BC}=\vec{c}-\vec{b}=2\hat{i}-\hat{j}+\hat{k}, so |\vec{BC}|^2=4+1+1=6.
\vec{CA}=\vec{a}-\vec{c}=-\hat{i}+3\hat{j}+5\hat{k}, so |\vec{CA}|^2=1+9+25=35.
Since |\vec{BC}|^2+|\vec{CA}|^2 = 6+35 = 41 = |\vec{AB}|^2, the converse of the Pythagoras theorem is satisfied, with the right angle at the vertex common to BC and CA.
\lambda\vec{a} is a unit vector when |\lambda\vec{a}|=1, i.e. |\lambda|\cdot|\vec{a}|=1, i.e. |\lambda|\cdot a=1.
This gives a=\dfrac{1}{|\lambda|}.
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