The magnitude of \(4\hat{i} - 4\hat{j} + 7\hat{k}\) is
- (a)\(9\)
- (b)\(7\)
- (c)\(81\)
- (d)\(\sqrt{15}\)
Show answer
Why: √(16 + 16 + 49) = √81.
\(\sqrt{4^2 + (-4)^2 + 7^2} = \sqrt{81} = 9\).
15 multiple-choice questions and 2 case-based questions on the current (rationalised) syllabus, in the style of the board paper's Sections A and E. Try each one first; the answer, a one-line reason and a worked solution open on a tap.
Choose one option. Section A of the board paper has 18 MCQs of 1 mark each, spread over all chapters.
The magnitude of \(4\hat{i} - 4\hat{j} + 7\hat{k}\) is
Why: √(16 + 16 + 49) = √81.
\(\sqrt{4^2 + (-4)^2 + 7^2} = \sqrt{81} = 9\).
The unit vector in the direction of \(\hat{i} + 2\hat{j} - 2\hat{k}\) is
Why: Divide by the magnitude √(1 + 4 + 4) = 3.
\(|\vec a| = \sqrt{1 + 4 + 4} = 3\), so \(\hat a = \dfrac13\left(\hat{i} + 2\hat{j} - 2\hat{k}\right)\).
If \(\vec a = \hat{i} + 2\hat{j} + 3\hat{k}\) and \(\vec b = 2\hat{i} - \hat{j} + \hat{k}\), then \(\vec a \cdot \vec b\) is
Why: Multiply matching components and add: 2 − 2 + 3.
\(\vec a \cdot \vec b = 1(2) + 2(-1) + 3(1) = 3\).
The angle between \(\vec a = \hat{i} + \hat{j}\) and \(\vec b = \hat{j} + \hat{k}\) is
Why: cos θ = (a·b)/(|a||b|) = 1/(√2 · √2).
\(\cos\theta = \dfrac{0 + 1 + 0}{\sqrt2 \cdot \sqrt2} = \dfrac12 \Rightarrow \theta = \dfrac{\pi}{3}\).
For which value of \(\lambda\) is \(3\hat{i} + \lambda\hat{j} - 2\hat{k}\) perpendicular to \(2\hat{i} + 4\hat{j} + \hat{k}\)?
Why: Dot product zero: 6 + 4λ − 2 = 0.
\(3(2) + \lambda(4) + (-2)(1) = 4 + 4\lambda = 0 \Rightarrow \lambda = -1\).
The scalar projection of \(\vec a = \hat{i} + 2\hat{j} + 2\hat{k}\) on \(\vec b = 2\hat{i} - \hat{j} + 2\hat{k}\) is
Why: Projection = a·b/|b| = 4/3.
\(\vec a \cdot \vec b = 2 - 2 + 4 = 4\), \(|\vec b| = 3\). Projection \(= \dfrac{4}{3}\).
\(\hat{k} \times \hat{i}\) equals
Why: Cyclic order i → j → k → i: k × i = j.
In the cyclic order \(\hat i, \hat j, \hat k\): \(\hat i \times \hat j = \hat k\), \(\hat j \times \hat k = \hat i\), \(\hat k \times \hat i = \hat j\).
If \(|\vec a| = 3\), \(|\vec b| = 4\) and the angle between them is \(\dfrac{\pi}{6}\), then \(|\vec a \times \vec b|\) is
Why: |a × b| = |a||b| sin θ = 12 × 1/2.
\(|\vec a \times \vec b| = 3 \times 4 \times \sin\dfrac{\pi}{6} = 6\). (\(6\sqrt3\) would be \(\vec a \cdot \vec b\).)
\((\hat{i} + \hat{j}) \times (\hat{i} - \hat{j})\) equals
Why: Only the k-component survives: (1)(−1) − (1)(1) = −2.
\(\begin{vmatrix} \hat i & \hat j & \hat k \\ 1 & 1 & 0 \\ 1 & -1 & 0 \end{vmatrix} = \hat i(0) - \hat j(0) + \hat k(-1 - 1) = -2\hat k\).
The area of the parallelogram with adjacent sides \(\vec a = 2\hat{i} + \hat{j}\) and \(\vec b = \hat{i} + 3\hat{j}\) is
Why: Area = |a × b| = |(6 − 1)k|.
\(\vec a \times \vec b = (2 \cdot 3 - 1 \cdot 1)\hat k = 5\hat k\), so the area is \(5\) sq units.
The direction cosines of the vector \(2\hat{i} - \hat{j} + 2\hat{k}\) are
Why: Divide each component by the magnitude 3.
\(|\vec a| = \sqrt{4 + 1 + 4} = 3\): direction cosines \(\dfrac23, -\dfrac13, \dfrac23\) (check: \(\tfrac49 + \tfrac19 + \tfrac49 = 1\)).
\(A\) and \(B\) have position vectors \(\hat{i} + \hat{j}\) and \(4\hat{i} + 7\hat{j}\). The point \(P\) dividing \(AB\) internally in the ratio \(1 : 2\) has position vector
Why: Section formula: (m·b + n·a)/(m + n) with m : n = 1 : 2.
\(\vec p = \dfrac{1(4\hat{i} + 7\hat{j}) + 2(\hat{i} + \hat{j})}{3} = \dfrac{6\hat i + 9\hat j}{3} = 2\hat{i} + 3\hat{j}\).
If \(|\vec a| = 2\), \(|\vec b| = 3\) and \(\vec a \cdot \vec b = 3\), then the angle between \(\vec a\) and \(\vec b\) is
Why: cos θ = 3/(2 × 3) = 1/2.
\(\cos\theta = \dfrac{3}{2 \times 3} = \dfrac12 \Rightarrow \theta = \dfrac{\pi}{3}\).
The vectors \(2\hat{i} - \hat{j} + 3\hat{k}\) and \(-4\hat{i} + 2\hat{j} + \mu\hat{k}\) are collinear. Then \(\mu\) equals
Why: Collinear means proportional components: −4/2 = 2/(−1) = μ/3 = −2.
\(\dfrac{-4}{2} = \dfrac{2}{-1} = -2\), so \(\dfrac{\mu}{3} = -2 \Rightarrow \mu = -6\).
\(\hat a\) and \(\hat b\) are unit vectors inclined at an angle \(\theta\) (\(0 \le \theta \le \pi\)). Then \(|\hat a - \hat b|\) equals
Why: |a − b|² = 1 + 1 − 2cos θ = 4 sin²(θ/2).
\(|\hat a - \hat b|^2 = |\hat a|^2 + |\hat b|^2 - 2\hat a \cdot \hat b = 2 - 2\cos\theta = 4\sin^2\dfrac{\theta}{2}\). As \(\sin\tfrac{\theta}{2} \ge 0\), \(|\hat a - \hat b| = 2\sin\dfrac{\theta}{2}\).
Section E of the board paper has three case-based questions of 4 marks: a real-life passage, then parts of 1, 1 and 2 marks, with a choice (OR) on the 2-mark part.
In a warehouse, a trolley is pushed in a straight line from the point \(A(1, 2, 0)\) to the point \(B(5, 4, 3)\) (coordinates in metres) by a constant force \(\vec F = 2\hat{i} + 3\hat{j} + \hat{k}\) newtons. The work done is \(W = \vec F \cdot \vec d\), where \(\vec d = \overrightarrow{AB}\).
For a science project, Kavya makes a triangular sail for a model boat. In a coordinate frame (units: dm), its corners are \(A(1, 0, 1)\), \(B(3, 2, 2)\) and \(C(1, 3, 5)\).
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