Vector Product Solutions: S.N. Dey Class 12 (Ex-2A)
Definition:
The scalar product (or dot product) of two vectors $\vec{a}$ and $\vec{b}$ is denoted by $\vec{a} \cdot \vec{b}$. It is a scalar and is defined as:
$$\vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos\theta$$
where $\theta$ is the angle between vectors $\vec{a}$ and $\vec{b}$, and $|\vec{a}|, |\vec{b}|$ are the moduli of vectors $\vec{a}$ and $\vec{b}$ respectively.
Since $\cos\theta > 0$ when $\theta$ is acute and $\cos\theta < 0$ when $\theta$ is obtuse, the scalar product $\vec{a} \cdot \vec{b}$ is positive when $\theta$ is acute and negative when $\theta$ is obtuse.
Proof 1: Scalar product is commutative
We know that:
$$\vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos\theta$$
$$\vec{b} \cdot \vec{a} = |\vec{b}| |\vec{a}| \cos\theta$$
Since $|\vec{a}| |\vec{b}| = |\vec{b}| |\vec{a}|$, it follows that:
$$\vec{a} \cdot \vec{b} = \vec{b} \cdot \vec{a}$$
Proof 2: Scalar product is distributive with respect to vector addition
Let $\vec{OA} = \vec{a}$, $\vec{OB} = \vec{b}$, and $\vec{BC} = \vec{c}$, where $|\vec{a}| = \overline{OA}$, $|\vec{b}| = \overline{OB}$, and $|\vec{c}| = \overline{BC}$.
From points $B$ and $C$, draw perpendiculars $BM$ and $CN$ onto $OA$. By the triangle law of addition:
$$\vec{b} + \vec{c} = \vec{OB} + \vec{BC} = \vec{OC}$$
Therefore:
$$\vec{a} \cdot (\vec{b} + \vec{c}) = |\vec{a}| \times (\text{scalar component of } (\vec{b} + \vec{c}) \text{ along } \vec{a})$$
$$= |\vec{a}| \overline{ON} = |\vec{a}| (\overline{OM} + \overline{MN})$$
$$= |\vec{a}| \overline{OM} + |\vec{a}| \overline{MN}$$
$$= |\vec{a}|(\text{scalar component of } \vec{b} \text{ along } \vec{a}) + |\vec{a}|(\text{scalar component of } \vec{c} \text{ along } \vec{a})$$
$$= \vec{a} \cdot \vec{b} + \vec{a} \cdot \vec{c}$$
Solution:
$$(\hat{i} + \hat{j}) \cdot (\hat{j} + \hat{k}) = \hat{i}\cdot\hat{j} + \hat{i}\cdot\hat{k} + \hat{j}\cdot\hat{j} + \hat{j}\cdot\hat{k} = 0 + 0 + 1 + 0 = 1 \quad \text{--- (1)}$$
If $\theta$ is the angle between the vectors:
$$\cos\theta = \frac{(\hat{i} + \hat{j}) \cdot (\hat{j} + \hat{k})}{|\hat{i} + \hat{j}| |\hat{j} + \hat{k}|} = \frac{1}{\sqrt{1^2 + 1^2} \sqrt{1^2 + 1^2}} = \frac{1}{\sqrt{2}\sqrt{2}} = \frac{1}{2}$$
$$\implies \theta = \frac{\pi}{3}$$
Solution:
$$(2\hat{i} - \hat{j} + 2\hat{k}) \cdot (\hat{i} + \hat{j} + \hat{k}) = 2(1) + (-1)(1) + 2(1) = 3 \quad \text{--- (1)}$$
If $\theta$ is the angle between the vectors:
$$\cos\theta = \frac{3}{\sqrt{2^2 + (-1)^2 + 2^2} \sqrt{1^2 + 1^2 + 1^2}} = \frac{3}{\sqrt{9}\sqrt{3}} = \frac{3}{3\sqrt{3}} = \frac{1}{\sqrt{3}}$$
$$\implies \theta = \cos^{-1}\left(\frac{1}{\sqrt{3}}\right)$$
Solution:
$$\vec{a} \cdot \vec{b} = 2(1) + 3(2) + (-4)(1) = 2 + 6 - 4 = 4 \quad \text{--- (1)}$$
Magnitudes:
$$|\vec{a}| = \sqrt{2^2 + 3^2 + (-4)^2} = \sqrt{29}$$
$$|\vec{b}| = \sqrt{1^2 + 2^2 + 1^2} = \sqrt{6}$$
Angle calculation:
$$\cos\theta = \frac{\vec{a} \cdot \vec{b}}{|\vec{a}||\vec{b}|} = \frac{4}{\sqrt{29}\sqrt{6}} = \frac{4}{\sqrt{174}}$$
Solution:
$$\vec{a} \cdot \vec{b} = 2(1) + (-5)(-2) + 3(-4) = 2 + 10 - 12 = 0$$
$$\cos\theta = \frac{0}{|\vec{a}||\vec{b}|} = 0 \implies \theta = \frac{\pi}{2}$$
Solution:
Vectors are perpendicular if $\vec{a} \cdot \vec{b} = 0$.
$$\vec{a} \cdot \vec{b} = (2\hat{i} + \hat{j} - \hat{k}) \cdot (\hat{i} + \hat{j} + 3\hat{k}) = 2(1) + 1(1) + (-1)(3) = 2 + 1 - 3 = 0$$
Solution:
Writing in component form: $\vec{a} = 3\hat{i} + 2\hat{j} - \hat{k}$, $\vec{b} = -2\hat{i} - 6\hat{k}$
$$\vec{a} \cdot \vec{b} = 3(-2) + 2(0) + (-1)(-6) = -6 + 0 + 6 = 0$$
Solution:
$$\vec{\alpha} \cdot \vec{\beta} = (-3)(-2) + (-2)(1) + 1(-4) = 6 - 2 - 4 = 0$$
Solution:
$$\vec{a} \cdot \vec{b} = 1(1) + 2(1) + 1(-3) = 1 + 2 - 3 = 0$$
$$\vec{b} \cdot \vec{c} = 1(7) + 1(-4) + (-3)(1) = 7 - 4 - 3 = 0$$
$$\vec{c} \cdot \vec{a} = 7(1) + (-4)(2) + 1(1) = 7 - 8 + 1 = 0$$
Solution:
$$\vec{a} \cdot \vec{b} = 2(3) + 3(-6) + 6(2) = 6 - 18 + 12 = 0$$
$$\vec{b} \cdot \vec{c} = 3(6) + (-6)(2) + 2(-3) = 18 - 12 - 6 = 0$$
$$\vec{c} \cdot \vec{a} = 6(2) + 2(3) + (-3)(6) = 12 + 6 - 18 = 0$$
Solution:
Set dot product to zero:
$$(m\hat{i} - 2\hat{j} + \hat{k}) \cdot (3\hat{i} - 2\hat{j} - 7\hat{k}) = 0$$
$$\implies 3m + (-2)(-2) + 1(-7) = 0 \implies 3m + 4 - 7 = 0$$
$$\implies 3m = 3 \implies m = 1$$
Solution:
$$\vec{a} \cdot \vec{b} = 0 \implies 0(-3) + 2(-m) + (-5)(4) = 0$$
$$\implies -2m - 20 = 0 \implies -2m = 20 \implies m = -10$$
Solution:
$$\vec{a} \cdot \vec{b} = 0 \implies 1(4) + 1(m) + m(-3) = 0$$
$$\implies 4 + m - 3m = 0 \implies 4 - 2m = 0 \implies m = 2$$
Solution:
$$\vec{a} + \vec{b} = (\hat{i} + 2\hat{j} - 3\hat{k}) + (3\hat{i} - \hat{j} + 2\hat{k}) = 4\hat{i} + \hat{j} - \hat{k} \quad \text{--- (1)}$$
$$\vec{a} - \vec{b} = (\hat{i} + 2\hat{j} - 3\hat{k}) - (3\hat{i} - \hat{j} + 2\hat{k}) = -2\hat{i} + 3\hat{j} - 5\hat{k} \quad \text{--- (2)}$$
Taking scalar product:
$$(\vec{a} + \vec{b}) \cdot (\vec{a} - \vec{b}) = 4(-2) + 1(3) + (-1)(-5) = -8 + 3 + 5 = 0$$
Solution:
$$\vec{a} + \vec{b} = 4\hat{i} + (2 + \lambda)\hat{j} + 12\hat{k}$$
$$\vec{a} - \vec{b} = 2\hat{i} + (2 - \lambda)\hat{j} + 6\hat{k}$$
Since $(\vec{a} + \vec{b}) \cdot (\vec{a} - \vec{b}) = 0$:
$$4(2) + (2 + \lambda)(2 - \lambda) + 12(6) = 0$$
$$8 + (4 - \lambda^2) + 72 = 0 \implies 84 - \lambda^2 = 0$$
$$\lambda^2 = 84 \implies \lambda = \pm\sqrt{84} = \pm 2\sqrt{21}$$
Solution:
$$\vec{a} + \vec{b} = 5\hat{i} + 0\hat{j} + \hat{k} \implies |\vec{a} + \vec{b}| = \sqrt{5^2 + 1^2} = \sqrt{26}$$
$$\vec{a} - \vec{b} = -\hat{i} - 2\hat{j} + 5\hat{k} \implies |\vec{a} - \vec{b}| = \sqrt{(-1)^2 + (-2)^2 + 5^2} = \sqrt{30}$$
Dot product:
$$(\vec{a} + \vec{b}) \cdot (\vec{a} - \vec{b}) = 5(-1) + 0(-2) + 1(5) = -5 + 0 + 5 = 0$$
$$\cos\theta = \frac{0}{\sqrt{26}\sqrt{30}} = 0 \implies \theta = \frac{\pi}{2}$$
Solution:
$$\vec{a} \cdot \vec{b} = 0(0) + 1(1) + 1(1) = 1, \quad |\vec{b}| = \sqrt{1^2 + 1^2} = \sqrt{2}$$
Scalar component of $\vec{a}$ along $\vec{b}$:
$$\frac{\vec{a} \cdot \vec{b}}{|\vec{b}|} = \frac{1}{\sqrt{2}}$$
Vector component of $\vec{a}$ along $\vec{b}$:
$$\left(\frac{\vec{a} \cdot \vec{b}}{|\vec{b}|^2}\right)\vec{b} = \frac{1}{(\sqrt{2})^2}(\hat{j} + \hat{k}) = \frac{1}{2}(\hat{j} + \hat{k})$$
Solution:
$$\vec{a} \cdot \vec{b} = 3(1) + 1(-1) + 3(-1) = 3 - 1 - 3 = -1$$
$$|\vec{b}| = \sqrt{1^2 + (-1)^2 + (-1)^2} = \sqrt{3}$$
Scalar component of $\vec{a}$ along $\vec{b}$:
$$\frac{\vec{a} \cdot \vec{b}}{|\vec{b}|} = \frac{-1}{\sqrt{3}}$$
Vector component of $\vec{a}$ along $\vec{b}$:
$$\left(\frac{\vec{a} \cdot \vec{b}}{|\vec{b}|^2}\right)\vec{b} = \frac{-1}{3}(\hat{i} - \hat{j} - \hat{k}) = -\frac{1}{3}(\hat{i} - \hat{j} - \hat{k})$$
Solution:
$$\vec{a} \cdot \vec{b} = 1(0) + 2(1) + 2(2) = 0 + 2 + 4 = 6$$
$$|\vec{a}| = \sqrt{1^2 + 2^2 + 2^2} = \sqrt{9} = 3$$
Scalar projection of $\vec{b}$ on $\vec{a}$:
$$\frac{\vec{a} \cdot \vec{b}}{|\vec{a}|} = \frac{6}{3} = 2$$
Vector projection of $\vec{b}$ on $\vec{a}$:
$$\left(\frac{\vec{a} \cdot \vec{b}}{|\vec{a}|^2}\right)\vec{a} = \frac{6}{3^2}(\hat{i} + 2\hat{j} + 2\hat{k}) = \frac{2}{3}(\hat{i} + 2\hat{j} + 2\hat{k})$$

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