Multiple Choice Questions (MCQs) for JEE Mathematics: Vectors
Access targeted multiple-choice questions for Vectors designed to align with the latest JEE academic syllabus for JEE Mathematics. These objective practice sets help students evaluate their conceptual understanding and improve exam readiness.
Practice Vectors MCQs for JEE Mathematics
Access the complete set of multiple-choice questions for Vectors below. This focused format allows students to isolate specific topics for thorough review and uninterrupted practice alongside official JEE textbooks.
Multiple Choice Questions
(a) \( 2\sqrt{5} \)
(b) \( 2\sqrt{2} \)
(c) \( 10\sqrt{5} \)
(d) \( 5\sqrt{2} \)
Show Answer & Explanation
Answer: (d) \( 5\sqrt{2} \)
Explanation:
1. The three conditions give \( \vec{a}\cdot\vec{b} + \vec{a}\cdot\vec{c} = 0 \), \( \vec{b}\cdot\vec{c} + \vec{b}\cdot\vec{a} = 0 \) and \( \vec{c}\cdot\vec{a} + \vec{c}\cdot\vec{b} = 0 \).
2. Adding and solving, each of the three dot products is 0.
3. \( |\vec{a} + \vec{b} + \vec{c}|^2 = 9 + 16 + 25 = 50 \), so the magnitude is \( 5\sqrt{2} \).
Teacher's Note:
1. Write each perpendicularity as a dot product equal to zero.
2. The three equations force all pairwise dot products to vanish.
(a) \( k\sqrt{2 + 2\sqrt{2}} \)
(b) \( k\sqrt{3 + 2\sqrt{2}} \)
(c) \( k\sqrt{4 + 2\sqrt{2}} \)
(d) \( k\sqrt{4 - 2\sqrt{2}} \)
Show Answer & Explanation
Answer: (c) \( k\sqrt{4 + 2\sqrt{2}} \)
Explanation:
1. Write the forces as \( k\hat{i} \), \( \frac{k}{\sqrt{2}}(\hat{i} + \hat{j}) \), \( k\hat{j} \) and \( \frac{k}{\sqrt{2}}(-\hat{i} + \hat{j}) \).
2. The sum is \( k\hat{i} + (k + \sqrt{2}k)\hat{j} \).
3. Magnitude \( = k\sqrt{1 + (1 + \sqrt{2})^2} = k\sqrt{4 + 2\sqrt{2}} \).
Teacher's Note:
1. Resolve each force along the two axes and add the components.
2. Use \( (1 + \sqrt{2})^2 = 3 + 2\sqrt{2} \).
(a) \( \vec{XB} = \frac{1}{3}\vec{AB} \)
(b) \( \vec{AX} = \frac{1}{3}\vec{AB} \)
(c) \( \vec{XN} = \frac{3}{4}\vec{MN} \)
(d) \( \vec{XM} = 3\vec{XN} \)
Show Answer & Explanation
Answer: (c) \( \vec{XN} = \frac{3}{4}\vec{MN} \)
Explanation:
1. Take A as origin with \( \vec{AB} = \vec{b} \), \( \vec{AC} = \vec{c} \). Then \( M = \frac{\vec{c}}{3} \) and \( N = 2\vec{b} - \vec{c} \).
2. Points of MN: \( \frac{\vec{c}}{3} + t\left(2\vec{b} - \frac{4\vec{c}}{3}\right) \). It meets line AB when the \( \vec{c} \)-coefficient is zero: \( t = \frac{1}{4} \).
3. So \( X = \frac{\vec{b}}{2} \), and \( \vec{MX} = \frac{1}{4}\vec{MN} \), i.e. \( \vec{XN} = \frac{3}{4}\vec{MN} \).
Teacher's Note:
1. Use non-collinear vectors \( \vec{b}, \vec{c} \) as a basis.
2. Coefficients of independent vectors must match separately.
(a) 6
(b) 5
(c) 4
(d) 0
Show Answer & Explanation
Answer: (a) 6
Explanation:
1. \( \vec{a}\times(\vec{b} - 2\vec{c}) = \vec{0} \), so \( \vec{b} - 2\vec{c} = \alpha\vec{a} \).
2. Squaring: \( 16 + 4 - 4\vec{b}\cdot\vec{c} = \alpha^2 \), and \( \vec{b}\cdot\vec{c} = 4\cdot 1\cdot\frac{1}{4} = 1 \), so \( \alpha^2 = 16 \), \( \alpha = \pm 4 \).
3. Then \( \vec{b} = 2\vec{c} \pm 4\vec{a} \), so \( |\ell| + |\mu| = 2 + 4 = 6 \).
Teacher's Note:
1. Parallel vectors have zero cross product.
2. Square the relation to bring in the given angle.
(a) \( [0, \frac{\pi}{3}] \)
(b) \( [\frac{\pi}{3}, \frac{2\pi}{3}] \)
(c) \( [0, \frac{2\pi}{3}] \)
(d) \( [0, \frac{5\pi}{6}] \)
Show Answer & Explanation
Answer: (c) \( [0, \frac{2\pi}{3}] \)
Explanation:
1. \( \cos\theta = \frac{ab + bc + ca}{a^2 + b^2 + c^2} \).
2. Since \( (a - b)^2 + (b - c)^2 + (c - a)^2 \ge 0 \), \( \cos\theta \le 1 \); and \( (a + b + c)^2 \ge 0 \) gives \( \cos\theta \ge -\frac{1}{2} \).
3. So \( -\frac{1}{2} \le \cos\theta \le 1 \), i.e. \( 0 \le \theta \le \frac{2\pi}{3} \).
Teacher's Note:
1. Both bounds come from sums of squares.
2. \( \cos\theta = -\frac{1}{2} \) corresponds to \( \frac{2\pi}{3} \).
(a) \( [\vec{a}\ \vec{b}\ \vec{c}]^2 = |\vec{a}| \)
(b) \( [\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}| \)
(c) \( [\vec{a}\ \vec{b}\ \vec{c}] = 0 \)
(d) \( [\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|^2 \)
Show Answer & Explanation
Answer: (d) \( [\vec{a}\ \vec{b}\ \vec{c}] = |\vec{a}|^2 \)
Explanation:
1. \( \vec{a}\cdot\vec{b} = 0 \) gives \( x - y + 2 = 0 \); \( \vec{a}\cdot\vec{c} = 4 \) gives \( x + 2y = 4 \). So \( x = 0,\ y = 2 \).
2. \( \vec{a} = 2\hat{j} + 2\hat{k} \) and \( |\vec{a}|^2 = 8 \).
3. \( [\vec{a}\ \vec{b}\ \vec{c}] = \begin{vmatrix} 0 & 2 & 2 \\ 1 & -1 & 1 \\ 1 & 2 & 0 \end{vmatrix} = 8 = |\vec{a}|^2 \).
Teacher's Note:
1. Solve the two linear equations for \( x \) and \( y \) first.
2. Evaluate the determinant to get the scalar triple product.
(a) not coplanar
(b) coplanar but cannot form a triangle
(c) coplanar and can form a triangle
(d) coplanar and can form a right-angled triangle
Show Answer & Explanation
Answer: (b) coplanar but cannot form a triangle
Explanation:
1. \( \vec{v}_1 + \vec{v}_2 = 3\hat{i} + \hat{j} + 4\hat{k} = \vec{v}_3 \), so the vectors are linearly dependent and hence coplanar.
2. For a closed triangle we would need \( \vec{v}_1 + \vec{v}_2 + \vec{v}_3 = \vec{0} \), but the sum is \( 2\vec{v}_3 \ne \vec{0} \).
3. So they are coplanar but cannot form a triangle.
Teacher's Note:
1. Check whether one vector is the sum of the other two.
2. A triangle needs the three vectors to sum to zero.
(a) \( (1 + \cos\theta)\sqrt{\cos 2\theta} \)
(b) \( (1 + \cos\theta)\sqrt{1 - 2\cos 2\theta} \)
(c) \( (1 - \cos\theta)\sqrt{1 + 2\cos\theta} \)
(d) \( (1 - \sin\theta)\sqrt{1 + 2\cos\theta} \)
Show Answer & Explanation
Answer: (c) \( (1 - \cos\theta)\sqrt{1 + 2\cos\theta} \)
Explanation:
1. \( [\vec{a}\ \vec{b}\ \vec{c}]^2 = \begin{vmatrix} 1 & \cos\theta & \cos\theta \\ \cos\theta & 1 & \cos\theta \\ \cos\theta & \cos\theta & 1 \end{vmatrix} \).
2. With \( c = \cos\theta \) the determinant is \( 1 - 3c^2 + 2c^3 = (1 - c)^2(1 + 2c) \).
3. So \( |[\vec{a}\ \vec{b}\ \vec{c}]| = (1 - \cos\theta)\sqrt{1 + 2\cos\theta} \).
Teacher's Note:
1. The square of a scalar triple product is a Gram determinant.
2. Factorise \( 2c^3 - 3c^2 + 1 \) using the root \( c = 1 \).
(a) \( \vec{a}_1 + \vec{a}_2 + \vec{a}_3 + \vec{a}_4 = \vec{0} \)
(b) \( \vec{a}_1 + \vec{a}_3 = \vec{a}_2 + \vec{a}_4 \)
(c) \( \vec{a}_1 + \vec{a}_2 = \vec{a}_3 + \vec{a}_4 \)
(d) \( \vec{a}_1 + \vec{a}_2 - \vec{a}_3 + \vec{a}_4 = \vec{0} \)
Show Answer & Explanation
Answer: (a) \( \vec{a}_1 + \vec{a}_2 + \vec{a}_3 + \vec{a}_4 = \vec{0} \)
Explanation:
1. Take vertices A, B, C, D. The outward area vectors are \( \frac{1}{2}\vec{AC}\times\vec{AB} \), \( \frac{1}{2}\vec{DB}\times\vec{DC} \), \( \frac{1}{2}\vec{DC}\times\vec{DA} \), \( \frac{1}{2}\vec{DA}\times\vec{DB} \).
2. With D as origin these are \( \frac{1}{2}[(\vec{c}-\vec{a})\times(\vec{b}-\vec{a})] \), \( \frac{1}{2}\vec{b}\times\vec{c} \), \( \frac{1}{2}\vec{c}\times\vec{a} \), \( \frac{1}{2}\vec{a}\times\vec{b} \).
3. Expanding the first gives \( \frac{1}{2}(\vec{c}\times\vec{b} - \vec{c}\times\vec{a} - \vec{a}\times\vec{b}) \), and the four sum to zero.
Teacher's Note:
1. The vector area of a closed surface is zero.
2. Place one vertex at the origin to simplify the cross products.
(a) 2
(b) 1
(c) 0
(d) \( -1 \)
Show Answer & Explanation
Answer: (c) 0
Explanation:
1. \( \vec{r}\cdot(\vec{a} + \vec{b} + \vec{c}) = 0 \).
2. Each cross product is perpendicular to two of the vectors: \( \ell[\vec{a}\ \vec{b}\ \vec{c}] + m[\vec{a}\ \vec{b}\ \vec{c}] + n[\vec{a}\ \vec{b}\ \vec{c}] = 0 \).
3. Since the triple product is 2, not zero, \( \ell + m + n = 0 \).
Teacher's Note:
1. Expand the dot product term by term.
2. Triple products with a repeated vector vanish.
(a) \( 2[\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \)
(b) \( 3[\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \)
(c) \( [\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \)
(d) \( 4[\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \)
Show Answer & Explanation
Answer: (a) \( 2[\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \)
Explanation:
1. Write \( \vec{r} = x\vec{a} + y\vec{b} + z\vec{c} \). Then \( (\vec{a}\times\vec{b})\times(\vec{r}\times\vec{c}) = [\vec{a}\ \vec{b}\ \vec{c}]\vec{r} - [\vec{a}\ \vec{b}\ \vec{r}]\vec{c} \) and \( [\vec{a}\ \vec{b}\ \vec{r}] = z[\vec{a}\ \vec{b}\ \vec{c}] \).
2. So the first term is \( [\vec{a}\ \vec{b}\ \vec{c}](\vec{r} - z\vec{c}) \); similarly for the others.
3. The sum is \( [\vec{a}\ \vec{b}\ \vec{c}](3\vec{r} - x\vec{a} - y\vec{b} - z\vec{c}) = 2[\vec{a}\ \vec{b}\ \vec{c}]\vec{r} \).
Teacher's Note:
1. Expand each vector product with the identity for \( (\vec{p}\times\vec{q})\times(\vec{r}\times\vec{s}) \).
2. Resolve \( \vec{r} \) along the three non-coplanar vectors.
(a) \( a^2(\vec{b}\cdot\vec{c}) \)
(b) \( b^2(\vec{a}\cdot\vec{c}) \)
(c) \( c^2(\vec{a}\cdot\vec{b}) \)
(d) \( -a^2(\vec{b}\cdot\vec{c}) \)
Show Answer & Explanation
Answer: (a) \( a^2(\vec{b}\cdot\vec{c}) \)
Explanation:
1. \( (\vec{a}\times\vec{b})\cdot(\vec{a}\times\vec{c}) = (\vec{a}\cdot\vec{a})(\vec{b}\cdot\vec{c}) - (\vec{a}\cdot\vec{c})(\vec{b}\cdot\vec{a}) \).
2. Since \( \vec{a} \) is parallel to \( \vec{b}\times\vec{c} \), it is perpendicular to both \( \vec{b} \) and \( \vec{c} \), so \( \vec{a}\cdot\vec{b} = \vec{a}\cdot\vec{c} = 0 \).
3. The result is \( a^2(\vec{b}\cdot\vec{c}) \).
Teacher's Note:
1. Use the Lagrange identity for the dot product of two cross products.
2. A vector parallel to \( \vec{b}\times\vec{c} \) is perpendicular to \( \vec{b} \) and \( \vec{c} \).
(a) \( 2\hat{i} - \hat{j} + 2\hat{k} \)
(b) \( \hat{i} - \hat{j} - 2\hat{k} \)
(c) \( \hat{i} + \hat{j} - 2\hat{k} \)
(d) \( -\hat{i} + \hat{j} - 2\hat{k} \)
Show Answer & Explanation
Answer: (d) \( -\hat{i} + \hat{j} - 2\hat{k} \)
Explanation:
1. Let \( \vec{b} = (b_1, b_2, b_3) \). \( \vec{a}\times\vec{b} = (b_3 + b_2,\ -b_1,\ -b_1) \) must equal \( -\vec{c} = (-1, 1, 1) \).
2. So \( b_1 = -1 \) and \( b_2 + b_3 = -1 \). Also \( \vec{a}\cdot\vec{b} = b_2 - b_3 = 3 \).
3. Solving gives \( b_2 = 1,\ b_3 = -2 \): \( \vec{b} = -\hat{i} + \hat{j} - 2\hat{k} \).
Teacher's Note:
1. Expand the cross product component by component.
2. Use the dot-product condition to separate \( b_2 \) and \( b_3 \).
(a) \( (2, -3) \)
(b) \( (-2, 3) \)
(c) \( (3, -2) \)
(d) \( (-3, 2) \)
Show Answer & Explanation
Answer: (d) \( (-3, 2) \)
Explanation:
1. \( \vec{a}\cdot\vec{c} = \lambda - 1 + 2\mu = 0 \).
2. \( \vec{b}\cdot\vec{c} = 2\lambda + 4 + \mu = 0 \).
3. Solving the two equations: \( \lambda = -3,\ \mu = 2 \).
Teacher's Note:
1. Mutually orthogonal means every pair has zero dot product.
2. \( \vec{a}\cdot\vec{b} = 2 - 4 + 2 = 0 \) already holds.
(a) \( -5 \)
(b) \( -3 \)
(c) 5
(d) 3
Show Answer & Explanation
Answer: (a) \( -5 \)
Explanation:
1. Both are unit vectors and \( \vec{a}\cdot\vec{b} = \frac{6 - 6}{7\sqrt{10}} = 0 \).
2. \( (\vec{a}\times\vec{b})\times\vec{a} = \vec{b}(\vec{a}\cdot\vec{a}) - \vec{a}(\vec{a}\cdot\vec{b}) = \vec{b} \) and \( (\vec{a}\times\vec{b})\times\vec{b} = \vec{b}(\vec{a}\cdot\vec{b}) - \vec{a}(\vec{b}\cdot\vec{b}) = -\vec{a} \), so \( (\vec{a}\times\vec{b})\times(\vec{a} + 2\vec{b}) = \vec{b} - 2\vec{a} \).
3. So the expression is \( (2\vec{a} - \vec{b})\cdot(\vec{b} - 2\vec{a}) = -|2\vec{a} - \vec{b}|^2 = -(4 + 1) = -5 \).
Teacher's Note:
1. Check whether the vectors are unit and orthogonal first.
2. For orthonormal \( \vec{a}, \vec{b} \), \( \vec{a}\times\vec{b} \) is a third unit vector.
(a) 2
(b) 0
(c) \( -1 \)
(d) \( -2 \)
Show Answer & Explanation
Answer: (d) \( -2 \)
Explanation:
1. Coplanar means \( \begin{vmatrix} p & 1 & 1 \\ 1 & q & 1 \\ 1 & 1 & r \end{vmatrix} = 0 \).
2. Expanding: \( pqr - p - q - r + 2 = 0 \).
3. So \( pqr - (p + q + r) = -2 \).
Teacher's Note:
1. Three vectors are coplanar when their determinant is zero.
2. Expand along the first row.
(a) \( \vec{a} \)
(b) \( \vec{c} \)
(c) \( \vec{0} \)
(d) \( \vec{a} + \vec{c} \)
Show Answer & Explanation
Answer: (c) \( \vec{0} \)
Explanation:
1. Let \( \vec{a} + 3\vec{b} = \lambda\vec{c} \) and \( \vec{b} + 2\vec{c} = \mu\vec{a} \).
2. From the second, \( 3\vec{b} = 3\mu\vec{a} - 6\vec{c} \). Substitute into the first: \( (1 + 3\mu)\vec{a} = (\lambda + 6)\vec{c} \).
3. Since \( \vec{a}, \vec{c} \) are not collinear, \( \lambda = -6 \), so \( \vec{a} + 3\vec{b} + 6\vec{c} = \vec{0} \).
Teacher's Note:
1. Eliminate \( \vec{b} \) between the two relations.
2. Non-collinear vectors force both coefficients to vanish.
(a) \( \frac{\pi}{6} \)
(b) \( \frac{\pi}{2} \)
(c) \( \frac{\pi}{3} \)
(d) \( \frac{\pi}{4} \)
Show Answer & Explanation
Answer: (c) \( \frac{\pi}{3} \)
Explanation:
1. \( \vec{c}\cdot\vec{d} = (\hat{a} + 2\hat{b})\cdot(5\hat{a} - 4\hat{b}) = 0 \).
2. \( 5 - 4\hat{a}\cdot\hat{b} + 10\hat{a}\cdot\hat{b} - 8 = 0 \), so \( 6\hat{a}\cdot\hat{b} = 3 \).
3. \( \cos\theta = \frac{1}{2} \), so \( \theta = \frac{\pi}{3} \).
Teacher's Note:
1. Expand the dot product using \( \hat{a}\cdot\hat{a} = \hat{b}\cdot\hat{b} = 1 \).
2. Perpendicular vectors have zero dot product.
(a) \( 3\sqrt{6} \)
(b) \( \sqrt{6} \)
(c) \( \sqrt{\frac{3}{2}} \)
(d) \( \frac{\sqrt{3}}{2} \)
Show Answer & Explanation
Answer: (c) \( \sqrt{\frac{3}{2}} \)
Explanation:
1. A normal to the plane is \( \vec{n} = (\hat{i} + \hat{j} + \hat{k})\times(\hat{i} + 2\hat{j} + 3\hat{k}) = \hat{i} - 2\hat{j} + \hat{k} \).
2. Projection magnitude \( = \frac{|(2\hat{i} + 3\hat{j} + \hat{k})\cdot\vec{n}|}{|\vec{n}|} = \frac{|2 - 6 + 1|}{\sqrt{6}} \).
3. This equals \( \frac{3}{\sqrt{6}} = \sqrt{\frac{3}{2}} \).
Teacher's Note:
1. The cross product gives a vector perpendicular to the plane.
2. Projection of \( \vec{u} \) on \( \vec{n} \) is \( \frac{\vec{u}\cdot\vec{n}}{|\vec{n}|} \).
(a) \( \sqrt{3} \)
(b) \( -\sqrt{3} \)
(c) \( \frac{1}{\sqrt{3}} \)
(d) \( -\frac{1}{\sqrt{3}} \)
Show Answer & Explanation
Answer: (c) \( \frac{1}{\sqrt{3}} \)
Explanation:
1. \( V = \begin{vmatrix} 1 & \lambda & 1 \\ 0 & 1 & \lambda \\ \lambda & 0 & 1 \end{vmatrix} = \lambda^3 - \lambda + 1 \).
2. \( \frac{dV}{d\lambda} = 3\lambda^2 - 1 = 0 \) gives \( \lambda = \pm\frac{1}{\sqrt{3}} \).
3. \( \frac{d^2V}{d\lambda^2} = 6\lambda > 0 \) only for \( \lambda = \frac{1}{\sqrt{3}} \), which gives the minimum.
Teacher's Note:
1. Volume is the scalar triple product.
2. Use the second derivative to separate the minimum from the maximum.
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