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Important Questions for CBSE Class 12 Maths Chapter 10 - Vector Algebra 2024-25

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CBSE Class 12 Maths Chapter-10 Important Questions - Free PDF Download

Free PDF download of Important Questions with solutions for CBSE Class 12 Maths Chapter 10 - Vector Algebra prepared by expert Maths teachers from latest edition of CBSE(NCERT) books. Register online for Maths tuition on Vedantu.com to score more marks in CBSE board examination.


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Also, check CBSE Class 12 Maths Important Questions for other chapters:

CBSE Class 12 Maths Important Questions

Sl.No

Chapter No

Chapter Name

1

Chapter 1

Relations and Functions

2

Chapter 2

Inverse Trigonometric Functions

3

Chapter 3

Matrices

4

Chapter 4

Determinants

5

Chapter 5

Continuity and Differentiability

6

Chapter 6

Application of Derivatives

7

Chapter 7

Integrals

8

Chapter 8

Application of Integrals

9

Chapter 9

Differential Equations

10

Chapter 10

Vector Algebra

11

Chapter 11

Three Dimensional Geometry

12

Chapter 12

Linear Programming

13

Chapter 13

Probability

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Study Important Questions for Class 12 Maths Chapter 10 - Vector Algebra

Very Short Answer Questions (1 Mark)

1. What are the horizontal and vertical components of a vector \[\overrightarrow a \] of magnitude \[5\] making an angle of \[{150^ \circ }\] with the direction of x-axis?

Ans: The vector \[\overrightarrow a \] has a magnitude \[|\overrightarrow a | = 5\] units and makes an angle \[\theta  = {150^ \circ }\] in the direction of the x-axis. Its horizontal and vertical components can be calculated as follows:

Horizontal component \[x = |\overrightarrow a | \cdot \cos \theta \]

\[ \Rightarrow x = 5 \cdot (\cos {150^ \circ })\]

\[ \Rightarrow x = 5 \cdot ( - \cos {30^ \circ })\]

\[ \Rightarrow x = 5 \cdot ( - \frac{{\sqrt 3 }}{2})\]

\[ \Rightarrow x =  - \frac{{5\sqrt 3 }}{2}\]

Vertical component \[y = |\overrightarrow a | \cdot \sin \theta \]

\[ \Rightarrow y = 5 \cdot (\sin {150^ \circ })\]

\[ \Rightarrow y = 5 \cdot (\sin {30^ \circ })\]

\[ \Rightarrow y = 5 \cdot (\frac{1}{2})\]

\[ \Rightarrow y = \frac{5}{2}\]


2. What is \[a \in R\] such that \[|a\overrightarrow x | = 1\] , where \[\overrightarrow x  = \hat i - 2\hat j + 2\hat k\] ?

Ans: We know that \[\overrightarrow x  = \hat i - 2\hat j + 2\hat k\] , so we can calculate \[|\overrightarrow x |\] as:

\[|\overrightarrow x | = \sqrt {{1^2} + {{( - 2)}^2} + {2^2}} \]

\[|\overrightarrow x | = \sqrt {1 + 4 + 4} \]

\[|\overrightarrow x | = \sqrt 9 \]

\[|\overrightarrow x | = 3\] units

Now we have \[|a\overrightarrow x | = 1\] and \[|\overrightarrow x | = 3\].

\[ \Rightarrow |a(3)| = 1\]

\[ \Rightarrow |a| = \frac{1}{3}\]

\[ \Rightarrow a =  \pm \frac{1}{3}\]


3. When is \[\mathbf{|\overrightarrow x  + \overrightarrow y | = |\overrightarrow x | + |\overrightarrow y |}\] ?

Ans: The magnitude of sum of two vectors can be equal to sum of their individual magnitude if and only if the two vectors are parallel.


4. What is the area of a parallelogram whose sides are given by \[\mathbf{2\hat i - \hat j}\] and \[\mathbf{\hat i + 5\hat k}\] ?

Ans: Let a parallelogram with adjacent sides \[\overrightarrow a  = 2\hat i - \hat j\] and \[\overrightarrow b  = \hat i + 5\hat k\] have an area of \[\overrightarrow a  \times \overrightarrow b \] . We calculate the value of \[\overrightarrow a  \times \overrightarrow b \] as follows:

\[\overrightarrow a  \times \overrightarrow b  = \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ 2&{ - 1}&0\\ 1&0&5 \end{array}} \right)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = \hat i( - 5) - \hat j(10) + \hat k(1)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  =  - 5\hat i - 10\hat j + \hat k\]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {{{( - 5)}^2} + {{( - 10)}^2} + {1^2}} \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {25 + 100 + 1} \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {126} \] units


5. What is the angle between \[\mathbf{\overrightarrow a} \] and \[\mathbf{\overrightarrow b} \] if \[\mathbf{\overrightarrow a  \cdot \overrightarrow b  = 3}\] and \[\mathbf{|\overrightarrow a  \times \overrightarrow b | = 3\sqrt 3} \] ?

Ans: We know that \[\overrightarrow a  \cdot \overrightarrow b  = |\overrightarrow a ||\overrightarrow b |\cos \theta \] and \[\overrightarrow a  \cdot \overrightarrow b  = 3\] is given.

So, \[|\overrightarrow a ||\overrightarrow b |\cos \theta  = 3\] .

\[ \Rightarrow \cos \theta  = \frac{3}{{|\overrightarrow a ||\overrightarrow b |}}\] ……(1)

Further, \[\overrightarrow a  \times \overrightarrow b  = |\overrightarrow a ||\overrightarrow b |\sin \theta \] and \[\overrightarrow a  \times \overrightarrow b  = 3\sqrt 3 \] . 

So, \[|\overrightarrow a ||\overrightarrow b |\sin \theta  = 3\sqrt 3 \]

\[ \Rightarrow \frac{{\sin \theta }}{{\sqrt 3 }} = \frac{3}{{|\overrightarrow a ||\overrightarrow b |}}\] ……(2)

From (1) and (2) we get:

\[\frac{{\sin \theta }}{{\sqrt 3 }} = \cos \theta \]

\[ \Rightarrow \frac{{\sin \theta }}{{\cos \theta }} = \sqrt 3 \]

\[ \Rightarrow \tan \theta  = \sqrt 3 \]

\[ \Rightarrow \theta  = \frac{\pi }{3}\]


6. Write a unit vector which makes an angle of \[\frac{\pi }{4}\] with x-axis and \[\frac{\pi }{3}\] with z-axis and an acute angle with y-axis.

Ans: It is given that \[\alpha  = \frac{\pi }{4}\] is the angle that the vector makes with x-axis, \[\gamma  = \frac{\pi }{3}\] with z-axis and an acute angle \[\beta \] with y-axis.

We know that \[{\cos ^2}\alpha  + {\cos ^2}\beta  + {\cos ^2}\gamma  = 1\]

So, \[{\cos ^2}\frac{\pi }{4} + {\cos ^2}\beta  + {\cos ^2}\frac{\pi }{3} = 1\]

\[ \Rightarrow {\left( {\frac{1}{{\sqrt 2 }}} \right)^2} + {\cos ^2}\beta  + {(\frac{1}{2})^2} = 1\]

\[ \Rightarrow \frac{1}{2} + {\cos ^2}\beta  + \frac{1}{4} = 1\]

\[ \Rightarrow {\cos ^2}\beta  = \frac{1}{4}\]

\[ \Rightarrow \cos \beta  =  \pm \frac{1}{2}\]

\[ \Rightarrow \beta  = \frac{\pi }{3} since \beta is acute angle \] 

We can find the unit vector making the above angles with the axes as follows:

\[\hat a = \cos \alpha  \cdot \hat i + \cos \beta  \cdot \hat j + \cos \gamma  \cdot \hat k\]

\[ \Rightarrow \hat a = \frac{1}{2}\hat i + \frac{1}{2}\hat j + \frac{1}{2}\hat k\]


7. If A is the point (4,5) and vector \[\mathbf{\overrightarrow {AB} }\] has components \[2\] and \[6\] along x-axis and y-axis respectively then write point B.

Ans: Since point A is \[(4,5)\] , we can write \[\overrightarrow {OA}  = 4\hat i + 5\hat j\] . Further, it is given that \[\overrightarrow {AB}  = 2\hat i + 6\hat j\] .

Let \[\overrightarrow {OB}  = x\hat i + y\hat j\] .

Now, \[\overrightarrow {AB}  = \overrightarrow {OB}  - \overrightarrow {OA} \] .

\[ \Rightarrow (2\hat i + 6\hat j) = (x\hat i + y\hat j) - (4\hat i + 5\hat j)\]

\[ \Rightarrow (x\hat i + y\hat j) = (2\hat i + 6\hat j) + (4\hat i + 5\hat j)\]

\[ \Rightarrow x\hat i + y\hat j = 6\hat i + 11\hat j\]

Hence, point B is \[(6,11)\] .


8. What is the point of trisection of PQ nearer to P if positions of P and Q are \[ \mathbf{3\hat i + 3\hat j - 4\hat k}\] and \[\mathbf{9\hat i + 8\hat j - 10\hat k}\] respectively?

Ans:  It is given that \[\overrightarrow {OP}  = 3\hat i + 3\hat j - 4\hat k\] and \[\overrightarrow {OQ}  = 9\hat i + 8\hat j - 10\hat k\] .

Now, \[\overrightarrow {PQ}  = \overrightarrow {OQ}  - \overrightarrow {OP} \] .

\[ \Rightarrow \overrightarrow {PQ}  = (9\hat i + 8\hat j - 10\hat k) - (3\hat i + 3\hat j - 4\hat k)\]

\[ \Rightarrow \overrightarrow {PQ}  = 6\hat i + 5\hat j - 6\hat k\]

Let the point of trisection nearer to P be A. 

So, \[3\overrightarrow {PA}  = \overrightarrow {PQ} \]

\[ \Rightarrow \overrightarrow {PA}  = \frac{{\overrightarrow {PQ} }}{3}\]

\[ \Rightarrow \overrightarrow {PA}  = \frac{{6\hat i + 5\hat j - 6\hat k}}{3}\]

\[ \Rightarrow \overrightarrow {PA}  = 2\hat i + \frac{5}{2}\hat j - 2\hat k\]

Hence, the point of trisection of \[\overrightarrow {PQ} \] nearer to P is \[(2,\frac{5}{2}, - 2)\] .


9. Write the vector in the direction of \[\mathbf{2\hat i + 3\hat j + 2\sqrt 3 \hat k}\] , whose magnitude is \[\mathbf{10}\] units.

Ans: Let the vector \[\overrightarrow a \] be \[2\hat i + 3\hat j + 2\sqrt 3 \hat k\] .

The unit vector in its direction will hence be-

\[\hat a = \frac{{2\hat i + 3\hat j + 2\sqrt 3 \hat k}}{{\sqrt {{2^2} + {3^2} + {{(2\sqrt 3 )}^2}} }}\]

\[ \Rightarrow \hat a = \frac{{2\hat i + 3\hat j + 2\sqrt 3 \hat k}}{{\sqrt {4 + 9 + 12} }}\]

\[\hat a = \frac{{2\hat i + 3\hat j + 2\sqrt 3 \hat k}}{{\sqrt {25} }}\]

\[\hat a = \frac{{2\hat i + 3\hat j + 2\sqrt 3 \hat k}}{5}\]

A vector \[\overrightarrow x \] in the direction of \[\overrightarrow a \] and with a magnitude \[10\] units will be-

\[\overrightarrow x  = \frac{{2\hat i + 3\hat j + 2\sqrt 3 \hat k}}{5} \times 10\]

\[ \Rightarrow \overrightarrow x  = 2(2\hat i + 3\hat j + 2\sqrt 3 \hat k)\]

\[ \Rightarrow \overrightarrow x  = 4\hat i + 6\hat j + 4\sqrt 3 \hat k\]


10. What are the direction cosines of a vector equiangular with coordinate

axes?

Ans: Let all the direction cosines of the vector be equal to \[\alpha \] .

Therefore, \[l = m = n = \cos \alpha \] .

We know that \[{l^2} + {m^2} + {n^2} = 1\] .

\[ \Rightarrow {\cos ^2}\alpha  + {\cos ^2}\alpha  + {\cos ^2}\alpha  = 1\]

\[ \Rightarrow 3{\cos ^2}\alpha  = 1\]

\[ \Rightarrow {\cos ^2}\alpha  = \frac{1}{3}\]

\[ \Rightarrow \cos \alpha  =  \pm \frac{1}{{\sqrt 3 }}\]

Thus, direction cosines of the vector which is equiangular to all three coordinate axes are \[ \pm \frac{1}{{\sqrt 3 }}\] , \[ \pm \frac{1}{{\sqrt 3 }}\] and \[ \pm \frac{1}{{\sqrt 3 }}\] .


11. What is the angle which the vector \[\mathbf{3\hat i - 6\hat j + 2\hat k}\] makes with the x-axis?

Ans: We have the vector \[\overrightarrow v  = 3\hat i - 6\hat j + 2\hat k\] .

To determine the angle it makes with the x-axis, we calculate the direction cosine with the required axis. So, we need to find \[l = \frac{a}{{|\overrightarrow v |}}\] , where \[l\] is the direction cosine with x-axis and \[a\] is the component corresponding to it.

Now, \[l = \frac{a}{{|\overrightarrow v |}}\]

\[ \Rightarrow l = \frac{3}{{\sqrt {{3^2} + {{( - 6)}^2} + {2^2}} }}\]

\[ \Rightarrow l = \frac{3}{{\sqrt {9 + 36 + 4} }}\]

\[ \Rightarrow l = \frac{3}{{\sqrt {49} }}\]

\[ \Rightarrow l = \frac{3}{7}\]

Further, \[l = \cos \alpha \] , where \[\alpha \] is the angle the vector makes with the x-axis.

Thus, \[\cos \alpha  = \frac{3}{7}\]

\[ \Rightarrow \alpha  = {\cos ^{ - 1}}(\frac{3}{7})\]

The vector \[\overrightarrow v  = 3\hat i - 6\hat j + 2\hat k\] makes an angle of \[{\cos ^{ - 1}}(\frac{3}{7})\] with the x-axis.


12. Write a unit vector perpendicular to both the vectors \[\mathbf{3\hat i - 2\hat j + \hat k}\] and \[ \mathbf{- 2\hat i + \hat j - 2\hat k}\] .

Ans: Given vectors \[\overrightarrow a  = 3\hat i - 2\hat j + \hat k\] and \[\overrightarrow b  =  - 2\hat i + \hat j - 2\hat k\] .

Firstly, we find the cross product of the two vectors:

\[\overrightarrow a  \times \overrightarrow b  = \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ 3&{ - 2}&1\\ { - 2}&1&{ - 2} \end{array}} \right)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = \hat i(3) - \hat j( - 4) + \hat k( - 1)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = 3\hat i + 4\hat j - \hat k\]

Now, the required unit vector which is perpendicular to both the given vectors can be calculated as \[\frac{{\overrightarrow a  \times \overrightarrow b }}{{|\overrightarrow a  \times \overrightarrow b |}}\] 

\[ \Rightarrow \frac{{\overrightarrow a  \times \overrightarrow b }}{{|\overrightarrow a  \times \overrightarrow b |}} = \frac{{3\hat i + 4\hat j - \hat k}}{{\sqrt {{3^2} + {4^2} + {{( - 1)}^2}} }}\]

\[ \Rightarrow \frac{{\overrightarrow a  \times \overrightarrow b }}{{|\overrightarrow a  \times \overrightarrow b |}} = \frac{{3\hat i + 4\hat j - \hat k}}{{\sqrt {9 + 16 + 1} }}\]

\[ \Rightarrow \frac{{\overrightarrow a  \times \overrightarrow b }}{{|\overrightarrow a  \times \overrightarrow b |}} = \frac{{3\hat i + 4\hat j - \hat k}}{{\sqrt {26} }}\]

\[ \Rightarrow \frac{{\overrightarrow a  \times \overrightarrow b }}{{|\overrightarrow a  \times \overrightarrow b |}} = \frac{{3\hat i + 4\hat j - \hat k}}{{\sqrt {26} }}\]

Hence, the required vector is \[\frac{{3\hat i + 4\hat j - \hat k}}{{\sqrt {26} }}\] .


13. What is the projection of the vector \[\mathbf{\hat i - \hat j}\] on the vector \[\mathbf{\hat i + \hat j}\] ?

Ans: Let \[\overrightarrow a  = \hat i - \hat j\] and \[\overrightarrow b  = \hat i + \hat j\] .

Projection of vector \[\overrightarrow a \] on \[\overrightarrow b \] \[ = \frac{{\overrightarrow a  \cdot \overrightarrow b }}{{|\overrightarrow b |}}\]

\[ \Rightarrow \frac{{\overrightarrow a  \cdot \overrightarrow b }}{{|\overrightarrow b |}} = \frac{{(1)(1) + ( - 1)(1) + (0)(0)}}{{\sqrt {{1^2} + {1^2}} }}\]

\[ \Rightarrow \frac{{\overrightarrow a  \cdot \overrightarrow b }}{{|\overrightarrow b |}} = \frac{{1 - 1}}{{\sqrt 2 }}\]

\[ \Rightarrow \frac{{\overrightarrow a  \cdot \overrightarrow b }}{{|\overrightarrow b |}} = 0\]

The projection of vector \[\overrightarrow a \] on \[\overrightarrow b \] is \[0\] .


14. If \[\mathbf{|\overrightarrow a | = 2}\] , \[\mathbf{|\overrightarrow b | = 2\sqrt 3} \] and \[\mathbf{\overrightarrow a  \bot \overrightarrow b }\] , what is the value of \[\mathbf{|\overrightarrow a  + \overrightarrow b |}\] ?

Ans: Taking the square of \[|\overrightarrow a  + \overrightarrow b |\] :

\[|\overrightarrow a  + \overrightarrow b {|^2} = |\overrightarrow a  + \overrightarrow b | \cdot |\overrightarrow a  + \overrightarrow b |\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = \overrightarrow a  \cdot \overrightarrow a  + \overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow a  + \overrightarrow b  \cdot \overrightarrow b \]

Since \[\overrightarrow a \] and \[\overrightarrow b \] are perpendicular, their dot product is equal to zero.

Further, we know that the dot product of a vector with itself is equal to the square of its magnitude.

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = |\overrightarrow a {|^2} + |\overrightarrow b {|^2}\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = {2^2} + {(2\sqrt 3 )^2}\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = 4 + 12\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = 16\]

Hence, \[|\overrightarrow a  + \overrightarrow b | = 4\] .


15. For what value of \[\mathbf{\lambda }\] is \[\mathbf{\overrightarrow a  = \lambda \hat i + \hat j + 4\hat k}\] perpendicular to \[\mathbf{\overrightarrow b  = 2\hat i + 6\hat j + 3\hat k}\] ?

Ans: For \[\overrightarrow a \] to be perpendicular to \[\overrightarrow b \] , their dot product should be zero.

So, \[\overrightarrow a  \cdot \overrightarrow b  = {a_1}{a_2} + {b_1}{b_2} + {c_1}{c_2}\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = \lambda (2) + (1)(6) + (4)(3)\] 

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = 2\lambda  + 6 + 12\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = 2\lambda  + 18\]

Now, \[\overrightarrow a  \cdot \overrightarrow b  = 0\]

Hence, \[2\lambda  + 18 = 0\]

\[ \Rightarrow \lambda  =  - \frac{{18}}{2}\]

\[ \Rightarrow \lambda  =  - 9\]


16. What is \[\mathbf{|\overrightarrow a |}\] , if \[\mathbf{(\overrightarrow a  + \overrightarrow b ) \cdot (\overrightarrow a  - \overrightarrow b ) = 3}\] and \[\mathbf{2|\overrightarrow b | = |\overrightarrow a |}\] ?

Ans: It is given that \[(\overrightarrow a  + \overrightarrow b ) \cdot (\overrightarrow a  - \overrightarrow b ) = 3\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow a  - \overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow a  + \overrightarrow b  \cdot \overrightarrow b  = 3\]

We know that the dot product of a vector with itself is equal to the square of its magnitude.

\[ \Rightarrow |\overrightarrow a {|^2} + |\overrightarrow b {|^2} = 3\]

\[ \Rightarrow |\overrightarrow a {|^2} + {\left( {\frac{{|\overrightarrow a |}}{2}} \right)^2} = 3\]  (Since \[2|\overrightarrow b | = |\overrightarrow a |\] )

\[ \Rightarrow |\overrightarrow a {|^2} + \frac{{|\overrightarrow a {|^2}}}{4} = 3\]

\[ \Rightarrow \frac{{5|\overrightarrow a {|^2}}}{4} = 3\]

\[ \Rightarrow |\overrightarrow a {|^2} = \frac{{12}}{5}\]

\[ \Rightarrow |\overrightarrow a | =  \pm \sqrt {\frac{{12}}{5}} \]


17. What is the angle between \[\mathbf{\overrightarrow a }\] and \[\mathbf{\overrightarrow b }\] , if \[\mathbf{|\overrightarrow a  - \overrightarrow b | = |\overrightarrow a  + \overrightarrow b |}\] ?

Ans: We have \[|\overrightarrow a  - \overrightarrow b | = |\overrightarrow a  + \overrightarrow b |\]

Squaring both sides,

\[ \Rightarrow |\overrightarrow a  - \overrightarrow b {|^2} = |\overrightarrow a  + \overrightarrow b {|^2}\]

\[ \Rightarrow |\overrightarrow a {|^2} + |\overrightarrow b {|^2} - 2\overrightarrow a  \cdot \overrightarrow b  = |\overrightarrow a {|^2} + |\overrightarrow b {|^2} + 2\overrightarrow a  \cdot \overrightarrow b \]

\[ \Rightarrow  - 2\overrightarrow a  \cdot \overrightarrow b  = 2\overrightarrow a  \cdot \overrightarrow b \]

\[ \Rightarrow 4\overrightarrow a  \cdot \overrightarrow b  = 0\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = 0\]

Since the dot product of the two vectors is equal to zero, the given vectors are perpendicular. Hence, the angle between them is \[{90^ \circ }\] .


18. In a parallelogram ABCD, \[\mathbf{\overrightarrow {AB}  = 2\hat i - \hat j + 4\hat k}\] and \[\mathbf{\overrightarrow {AC}  = \hat i + \hat j + 4\hat k}\] . What is the length of the side BC?

Ans: We have \[\overrightarrow {AB}  = 2\hat i - \hat j + 4\hat k\] and \[\overrightarrow {AC}  = \hat i + \hat j + 4\hat k\] .

We calculate \[|\overrightarrow {AB} | = \sqrt {{2^2} + {{( - 1)}^2} + {4^2}} \]

\[ \Rightarrow |\overrightarrow {AB} | = \sqrt {21} \]

Similarly, \[|\overrightarrow {AC} | = \sqrt {{1^2} + {1^2} + {4^2}} \]

\[ \Rightarrow |\overrightarrow {AC} | = \sqrt {18} \]

In a parallelogram, AC would represent a diagonal and AB and BC would be adjacent sides.

So, \[|\overrightarrow {BC} | = |\overrightarrow {AC}  - \overrightarrow {AB} |\]

Squaring both sides:

\[ \Rightarrow |\overrightarrow {BC} {|^2} = |\overrightarrow {AC}  - \overrightarrow {AB} {|^2}\]

\[ \Rightarrow |\overrightarrow {BC} {|^2} = |\overrightarrow {AC} {|^2} + |\overrightarrow {AB} {|^2} - 2\overrightarrow {AC}  \cdot \overrightarrow {AB} \]

\[ \Rightarrow |\overrightarrow {BC} {|^2} = 18 + 21 - 2[(2)(1) + ( - 1)(1) + (4)(4)]\]

\[ \Rightarrow |\overrightarrow {BC} {|^2} = 39 - 2(17)\]

\[ \Rightarrow |\overrightarrow {BC} {|^2} = 39 - 34\]

\[ \Rightarrow |\overrightarrow {BC} {|^2} = 5\]

\[ \Rightarrow |\overrightarrow {BC} | = \sqrt 5 \]


19. What is the area of a parallelogram whose diagonals are given by vectors \[\mathbf{2\hat i + \hat j - 2\hat k}\] and \[ \mathbf{- \hat i + 2\hat k}\] ?

Ans: The two diagonals of a parallelogram are given by \[\overrightarrow a  = 2\hat i + \hat j - 2\hat k\] and \[\overrightarrow b  =  - \hat i + 2\hat k\] .

We find their cross product as follows:

\[\overrightarrow a  \times \overrightarrow b  = \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ 2&1&{ - 2}\\ { - 1}&0&2 \end{array}} \right)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = \hat i(2) - \hat j(2) + \hat k(1)\]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = 2\hat i - 2\hat j + \hat k\]

Next, we find its magnitude:

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {{2^2} + {{( - 2)}^2} + {1^2}} \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {4 + 4 + 1} \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt 9 \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = 3\]

The area of the parallelogram A can be calculated as:

\[A = \frac{1}{2} \cdot |\overrightarrow a  \times \overrightarrow b |\]

\[ \Rightarrow A = \frac{3}{2}\] square units

The area of the parallelogram with diagonals \[\overrightarrow a  = 2\hat i + \hat j - 2\hat k\] and \[\overrightarrow b  =  - \hat i + 2\hat k\] is \[\frac{3}{2}\] square units.


20. Find \[\mathbf{|\overrightarrow x |}\] if for a unit vector \[\mathbf{\hat a}\] , \[\mathbf{(\overrightarrow x  - \hat a) \cdot (\overrightarrow x  + \hat a) = 12}\] .

Ans: It is given that \[(\overrightarrow x  - \hat a) \cdot (\overrightarrow x  + \hat a) = 12\]

\[ \Rightarrow \overrightarrow x  \cdot \overrightarrow x  - \overrightarrow x  \cdot \hat a + \hat a \cdot \overrightarrow x  - \hat a \cdot \hat a = 12\]

We know that the dot product of a vector with itself is equal to the square of its magnitude.

\[ \Rightarrow |\overrightarrow x {|^2} - |\hat a{|^2} = 12\]

\[ \Rightarrow |\overrightarrow x {|^2} - {1^2} = 12\] (Since, magnitude of a unit vector is equal to one unit)

\[ \Rightarrow |\overrightarrow x {|^2} = 13\]

\[ \Rightarrow |\overrightarrow x | = \sqrt {13} \] units


21. If \[\overrightarrow a \] and \[\overrightarrow b \] are two unit vectors and \[\overrightarrow a  + \overrightarrow b \] is also a unit vector, then what is the angle between \[\overrightarrow a \] and \[\overrightarrow b \] ?

Ans: We know that \[\overrightarrow a  + \overrightarrow b \] , \[\overrightarrow a \] and \[\overrightarrow b \] are unit vectors.

Taking the square of \[\overrightarrow a  + \overrightarrow b \] :

\[|\overrightarrow a  + \overrightarrow b {|^2} = \overrightarrow a  \cdot \overrightarrow a  + 2\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow b \]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} = |\overrightarrow a {|^2} + 2\overrightarrow a  \cdot \overrightarrow b  + |\overrightarrow b {|^2}\]

\[ \Rightarrow {1^2} = {1^2} + 2\overrightarrow a  \cdot \overrightarrow b  + {1^2}\] (Since magnitude of unit vectors is equal to one unit)

\[ \Rightarrow 2\overrightarrow a  \cdot \overrightarrow b  =  - 1\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  =  - \frac{1}{2}\]

Further, \[\overrightarrow a  \cdot \overrightarrow b  = |\overrightarrow a ||\overrightarrow b |\cos \theta \]

\[ \Rightarrow |\overrightarrow a ||\overrightarrow b |\cos \theta  =  - \frac{1}{2}\]

\[ \Rightarrow (1)(1)\cos \theta  =  - \frac{1}{2}\]

\[ \Rightarrow \cos \theta  =  - \frac{1}{2}\]

\[ \Rightarrow \theta  = \frac{{2\pi }}{3}\]


22. If \[\mathbf{\hat i,\hat j,\hat k}\] are the usual three mutually perpendicular unit vectors then what is the value of \[\mathbf{\hat i \cdot (\hat j \times \hat k) + \hat j \cdot (\hat i \times \hat k) + \hat k \cdot (\hat j \times \hat i)}\] ? 

Ans: We have \[\hat i \cdot (\hat j \times \hat k) + \hat j \cdot (\hat i \times \hat k) + \hat k \cdot (\hat j \times \hat i)\] .

It is known that \[\hat j \times \hat k = \hat i\] , \[\hat k \times \hat i = \hat j\] and \[\hat i \times \hat j = \hat k\] .

Therefore, \[\hat i \cdot (\hat j \times \hat k) + \hat j \cdot (\hat i \times \hat k) + \hat k \cdot (\hat j \times \hat i)\] can be rewritten as:

\[ = \hat i \cdot \hat i + \hat j \cdot ( - \hat j) + \hat k \cdot ( - \hat k)\]

\[= \hat i \cdot \hat i - \hat j \cdot \hat j - \hat k \cdot \hat k\]

\[ = 1 - 1 - 1\] (Since \[\hat i \cdot \hat i = \hat j \cdot \hat j = \hat k \cdot \hat k = 1\] )

\[ =  - 1\]


23. What is the angle between \[\mathbf{\overrightarrow x} \] and \[\mathbf{\overrightarrow y }\] if \[\mathbf{\overrightarrow x  \cdot \overrightarrow y  = |\overrightarrow x  \times \overrightarrow y |}\] ?

Ans: The dot product and cross product of the given vectors \[\overrightarrow x \] and \[\overrightarrow y \] are equal. This implies:

\[\overrightarrow x  \cdot \overrightarrow y  = |\overrightarrow x  \times \overrightarrow y |\]

\[ \Rightarrow |\overrightarrow x ||\overrightarrow y |\cos \theta  = |\overrightarrow x ||\overrightarrow y |\sin \theta \]

\[ \Rightarrow \cos \theta  = \sin \theta \]

This is only possible if \[\theta  = \frac{\pi }{4}\] .

Hence, the angle between vectors \[\overrightarrow x \] and \[\overrightarrow y \] is \[\frac{\pi }{4}\] .


24. Write a unit vector in XY-plane, making an angle of \[{30^ \circ }\] with the positive direction of x–axis.

Ans: Let \[\overrightarrow r \] be a unit vector in the XY-plane, making an angle of \[{30^ \circ }\] with the positive direction of the x-axis. It will be represented as:

\[\overrightarrow r  = \cos \theta \hat i + \sin \theta \hat j\]

Substituting \[\theta  = {30^ \circ }\] :

\[ \Rightarrow \overrightarrow r  = \cos ({30^ \circ })\hat i + \sin ({30^ \circ })\hat j\]

\[ \Rightarrow \overrightarrow r  = \frac{{\sqrt 3 }}{2}\hat i + \frac{1}{2}\hat j\]

The required vector is \[\frac{{\sqrt 3 }}{2}\hat i + \frac{1}{2}\hat j\] .

 

25. If \[\mathbf{\overrightarrow a }\] , \[\mathbf{\overrightarrow b }\] and \[\mathbf{\overrightarrow c }\] are unit vectors with \[\mathbf{\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0}\] , then what is the value of \[\mathbf{\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow c  \cdot \overrightarrow a }\] ?

Ans: Since \[\overrightarrow a \] , \[\overrightarrow b \] and \[\overrightarrow c \] are unit vectors, it means that \[|\overrightarrow a | = |\overrightarrow b | = |\overrightarrow c | = 1\] .

Further it is given that \[\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0\] .

Squaring both sides:

\[ \Rightarrow {(\overrightarrow a  + \overrightarrow b  + \overrightarrow c )^2} = 0\]

\[ \Rightarrow |\overrightarrow a {|^2} + |\overrightarrow b {|^2} + |\overrightarrow c {|^2} + 2(\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow c  \cdot \overrightarrow a ) = 0\]

\[ \Rightarrow 1 + 1 + 1 + 2(\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow c  \cdot \overrightarrow a ) = 0\]

\[ \Rightarrow 2(\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow c  \cdot \overrightarrow a ) =  - 3\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow c  \cdot \overrightarrow a  =  - \frac{3}{2}\]


26. If \[\mathbf{\overrightarrow a }\] and \[\mathbf{\overrightarrow b }\] are unit vectors such that \[\mathbf{\overrightarrow a  + 2\overrightarrow b} \] is perpendicular to \[\mathbf{5\overrightarrow a  - 4\overrightarrow b }\] , then what is the angle between \[\mathbf{\overrightarrow a }\] and \[\mathbf{\overrightarrow b }\] ?

Ans: It is given that \[\overrightarrow a \] and \[\overrightarrow b \] are unit vectors, and the vectors \[\overrightarrow a  + 2\overrightarrow b \] and \[5\overrightarrow a  - 4\overrightarrow b \] are perpendicular, that is, their dot product will be zero.

\[(\overrightarrow a  + 2\overrightarrow b ) \cdot (5\overrightarrow a  - 4\overrightarrow b ) = 0\]

\[ \Rightarrow 5|\overrightarrow a {|^2} + 6\overrightarrow a  \cdot \overrightarrow b  - 8|\overrightarrow b {|^2} = 0\]

\[ \Rightarrow 5{(1)^2} + 6\overrightarrow a  \cdot \overrightarrow b  - 8{(1)^2} = 0\] (Since \[\overrightarrow a \] and \[\overrightarrow b \] are unit vectors)

\[ \Rightarrow 6\overrightarrow a  \cdot \overrightarrow b  = 3\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = \frac{1}{2}\]

Now, \[\overrightarrow a  \cdot \overrightarrow b  = |\overrightarrow a ||\overrightarrow b |\cos \theta \]

\[ \Rightarrow \frac{1}{2} = (1)(1)\cos \theta \]

\[ \Rightarrow \frac{1}{2} = \cos \theta \]

\[ \Rightarrow \theta  = \frac{\pi }{3}\]


Short Answer Questions (4 Mark)

27. If ABCDEF is a regular hexagon then using triangle law of addition prove that \[\mathbf{\overrightarrow {AB}  + \overrightarrow {AC}  + \overrightarrow {AD}  + \overrightarrow {AE}  + \overrightarrow {AF}  = 3\overrightarrow {AD}  = 6\overrightarrow {AO}} \] , O being the centre of hexagon.

Ans: ABCDEF is a regular polygon:


ABCDEF is a Regular Polygon:


Hence, \[\overrightarrow {AB} ,\overrightarrow {BC} ,\overrightarrow {CD} ,\overrightarrow {ED} ,\overrightarrow {EF} ,\overrightarrow {AF} \] are all equal.

Further, using the triangle law of addition:

\[\overrightarrow {AC}  + \overrightarrow {CD}  = \overrightarrow {AD} \] ......(1)

And, \[\overrightarrow {AE}  + \overrightarrow {ED}  = \overrightarrow {AD} \] ......(2)

Now, taking (1)+(2) :

\[\overrightarrow {AC}  + \overrightarrow {CD}  + \overrightarrow {AE}  + \overrightarrow {ED}  = \overrightarrow {AD}  + \overrightarrow {AD} \]

Adding \[\overrightarrow {AD} \] both sides:

\[ \Rightarrow \overrightarrow {AC}  + \overrightarrow {CD}  + \overrightarrow {AE}  + \overrightarrow {ED}  + \overrightarrow {AD}  = 3\overrightarrow {AD} \]

\[ \Rightarrow \overrightarrow {AC}  + \overrightarrow {AF}  + \overrightarrow {AE}  + \overrightarrow {AB}  + \overrightarrow {AD}  = 3\overrightarrow {AD} \] (Since \[\overrightarrow {CD}  = \overrightarrow {AF} \] and \[\overrightarrow {AE}  = \overrightarrow {AB} \] )

Also, O is the midpoint of \[\overrightarrow {AD} \] , therefore, \[\overrightarrow {AD}  = 2\overrightarrow {AO} \] .

Hence, \[\overrightarrow {AC}  + \overrightarrow {AF}  + \overrightarrow {AE}  + \overrightarrow {AB}  + \overrightarrow {AD}  = 3\overrightarrow {AD}  = 6\overrightarrow {AO} \] is proved.


28. Points L, M, N divide the sides BC, CA, AB of a ABC in the ratios 1:4,3:2,3:7 respectively. Prove that \[\mathbf{\overrightarrow {AL}  + \overrightarrow {BM}  + \overrightarrow {CN} }\] is a vector parallel to \[\mathbf{\overrightarrow {CK} }\] where K divides AB in ratio 1:3 .

Ans: Let \[\overrightarrow a \] , \[\overrightarrow b \] and \[\overrightarrow c \] be the position vectors of points A, B and C respectively.

We find the position vectors of points L, M, N and K:

\[\overrightarrow {OL}  = \frac{{(1)\overrightarrow c  + (4)\vec b}}{{1 + 4}}\] (Since L divides BC in the ratio \[1:4\] )

\[ \Rightarrow \overrightarrow {OL}  = \frac{{\vec c + 4\vec b}}{5}\]

\[\overrightarrow {OM}  = \frac{{(3)\overrightarrow a  + (2)c}}{{3 + 2}}\] (Since M divides CA in the ratio \[3:2\] )

\[ \Rightarrow \overrightarrow {OM}  = \frac{{3\overrightarrow a  + 2\overrightarrow c }}{5}\]

\[\overrightarrow {ON}  = \frac{{(3)\overrightarrow b  + (7)\overrightarrow a }}{{3 + 7}}\] (Since N divides AB in the ratio \[3:7\] )

\[ \Rightarrow \overrightarrow {ON}  = \frac{{3\vec b + 7\vec a}}{{10}}\]

\[\overrightarrow {OK}  = \frac{{(1)\overrightarrow b  + (3)\overrightarrow a }}{{1 + 3}}\] (Since K divides AB in the ratio \[1:3\] )

\[ \Rightarrow \overrightarrow {OK}  = \frac{{\vec b + 3\vec a}}{4}\]

Taking \[\overrightarrow {AL}  + \overrightarrow {BM}  + \overrightarrow {CN} \] :

\[ = (\overrightarrow {OL}  - \overrightarrow {OA} ) + (\overrightarrow {BM}  - \overrightarrow {OB} ) + (\overrightarrow {CN}  - \overrightarrow {OC} )\]

\[ = (\overrightarrow {OL}  - \overrightarrow a ) + (\overrightarrow {OM}  - \overrightarrow b ) + (\overrightarrow {ON}  - \overrightarrow c )\]

\[ = (\frac{{\overrightarrow c  + 4\vec b}}{5} - \overrightarrow a ) + (\frac{{3\overrightarrow a  + 2\overrightarrow c }}{5} - \overrightarrow b ) + (\frac{{3\vec b + 7\overrightarrow a }}{{10}} - \overrightarrow c )\]

\[ = \frac{{2\overrightarrow c  + 8\vec b - 10\overrightarrow a  + 6\overrightarrow a  + 4\overrightarrow c  - 10\overrightarrow b  + 3\vec b + 7\overrightarrow a  - 10\overrightarrow c }}{{10}}\]

\[ = \frac{{3\overrightarrow a  + \overrightarrow b  - 4\overrightarrow c }}{{10}}\]

Now, \[\overrightarrow {CK}  = \overrightarrow {OK}  - \overrightarrow {OC} \]

\[ \Rightarrow \overrightarrow {CK}  = \frac{{\vec b + 3\vec a}}{4} - \overrightarrow c \]

\[ \Rightarrow \overrightarrow {CK}  = \frac{{\vec b + 3\vec a - 4\overrightarrow c }}{4}\] 

We notice that \[\overrightarrow {CK}  = \frac{5}{2} \times (\overrightarrow {AL}  + \overrightarrow {BM}  + \overrightarrow {CN} )\] .

Hence, we prove that \[\overrightarrow {AL}  + \overrightarrow {BM}  + \overrightarrow {CN} \] is parallel to \[\overrightarrow {CK} \] .


29. The scalar product of vector \[\mathbf{\hat i + \hat j + \hat k}\] with a unit vector along the sum of the vectors \[\mathbf{2\hat i + 4\hat j - 5\hat k}\] and \[\mathbf{\lambda \hat i + 2\hat j + 3\hat k}\] is equal to 1 . Find the value of \[\lambda \] .

Ans: The sum of vectors \[2\hat i + 4\hat j - 5\hat k\] and \[\lambda \hat i + 2\hat j + 3\hat k\] is:

\[(2\hat i + 4\hat j - 5\hat k) + (\lambda \hat i + 2\hat j + 3\hat k)\]

\[ = \hat i(2 + \lambda ) + \hat j(4 + 2) + \hat k( - 5 + 3)\]

\[ = (2 + \lambda )\hat i + 6\hat j - 2\hat k\]

The unit vector along the sum of \[2\hat i + 4\hat j - 5\hat k\] and \[\lambda \hat i + 2\hat j + 3\hat k\] vectors is:

\[\frac{{(2 + \lambda )\hat i + 6\hat j - 2\hat k}}{{|(2 + \lambda )\hat i + 6\hat j - 2\hat k|}}\]

\[ = \frac{{(2 + \lambda )\hat i + 6\hat j - 2\hat k}}{{\sqrt {{\lambda ^2} + 4\lambda  + 4 + 36 + 4} }}\]

\[ = \frac{{(2 + \lambda )\hat i + 6\hat j - 2\hat k}}{{\sqrt {{\lambda ^2} + 4\lambda  + 44} }}\]

The scalar product of \[\frac{{(2 + \lambda )\hat i + 6\hat j - 2\hat k}}{{\sqrt {{\lambda ^2} + 4\lambda  + 44} }}\] and \[\hat i + \hat j + \hat k\] is \[1\] .

Thus, \[(\frac{{(2 + \lambda )\hat i + 6\hat j - 2\hat k}}{{\sqrt {{\lambda ^2} + 4\lambda  + 44} }}) \cdot (\hat i + \hat j + \hat k) = 1\]

\[ \Rightarrow \frac{{(2 + \lambda ) + 6 - 2}}{{\sqrt {{\lambda ^2} + 4\lambda  + 44} }} = 1 \]

\[ \Rightarrow \lambda  + 6 = \sqrt {{\lambda ^2} + 4\lambda  + 44} \]

Squaring both sides:

\[ \Rightarrow {(\lambda  + 6)^2} = {\lambda ^2} + 4\lambda  + 44\]

\[ \Rightarrow {\lambda ^2} + 12\lambda  + 36 = {\lambda ^2} + 4\lambda  + 44\]

\[ \Rightarrow {\lambda ^2} + 12\lambda  + 36 = {\lambda ^2} + 4\lambda  + 44\]

\[ \Rightarrow 8\lambda  = 8\]

\[ \Rightarrow \lambda  = 1\]


30. \[\mathbf{\overrightarrow a} \] , \[\mathbf{\overrightarrow b }\] and \[\mathbf{\overrightarrow c }\] are three mutually perpendicular vectors of equal magnitude. Show that \[\mathbf{\overrightarrow a  + \overrightarrow b  + \overrightarrow c }\] makes equal angles with \[\mathbf{\overrightarrow a} \] , \[\mathbf{\overrightarrow b }\] and \[\mathbf{\overrightarrow c }\] with each angle as \[\mathbf{{\cos ^{ - 1}}\left( {\frac{1}{{\sqrt 3 }}} \right)}\] .

Ans: Let \[|\overrightarrow a | = |\overrightarrow b | = |\overrightarrow c | = \lambda \] and since they are mutually perpendicular, \[\overrightarrow a  \cdot \overrightarrow b  = \overrightarrow b  \cdot \overrightarrow c  = \overrightarrow a  \cdot \overrightarrow c  = 0\] .

Consider \[|\overrightarrow a  + \overrightarrow b  + \overrightarrow c {|^2}\] :

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b  + \overrightarrow c {|^2} = |\overrightarrow a {|^2} + |\overrightarrow b {|^2} + |\overrightarrow c {|^2} + 2(\overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow c  + \overrightarrow a  \cdot \overrightarrow c )\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b  + \overrightarrow c {|^2} = {\lambda ^2} + {\lambda ^2} + {\lambda ^2} + 2(0 + 0 + 0)\] 

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b  + \overrightarrow c {|^2} = 3{\lambda ^2}\]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b  + \overrightarrow c | = \sqrt 3 \lambda \]

Suppose \[\overrightarrow a ,\overrightarrow b ,\overrightarrow c \] make angles \[{\theta _1},{\theta _2},{\theta _3}\] with \[\overrightarrow a  + \overrightarrow b  + \overrightarrow c \] respectively.

Then, \[\cos {\theta _1} = \frac{{\overrightarrow a  \cdot (\overrightarrow a  + \overrightarrow b  + \overrightarrow c )}}{{|\overrightarrow a ||\overrightarrow a  + \overrightarrow b  + \overrightarrow c |}}\]

\[ \Rightarrow \cos {\theta _1} = \frac{{\overrightarrow a  \cdot \overrightarrow a  + \overrightarrow a  \cdot \overrightarrow b  + \overrightarrow a  \cdot \overrightarrow c }}{{|\overrightarrow a | \cdot \sqrt 3 \lambda }}\]

\[ \Rightarrow \cos {\theta _1} = \frac{{|\overrightarrow a {|^2}}}{{|\overrightarrow a | \cdot \sqrt 3 \lambda }}\]

\[ \Rightarrow \cos {\theta _1} = \frac{\lambda }{{\sqrt 3 \lambda }}\]

\[ \Rightarrow \cos {\theta _1} = \frac{1}{{\sqrt 3 }}\]

Similarly, \[\cos {\theta _2} = \cos {\theta _3} = \frac{1}{{\sqrt 3 }}\] .

Therefore, \[{\theta _1} = {\theta _2} = {\theta _3}\] .


31. If \[\mathbf{\overrightarrow \alpha   = 3\hat i - \hat j}\] and \[\mathbf{\overrightarrow \beta   = 2\hat i + \hat j + 3\hat k}\] then express \[\mathbf{\overrightarrow \beta } \] in the form of \[\mathbf{\overrightarrow \beta   = \overrightarrow {{\beta _1}}  + \overrightarrow {{\beta _2}} }\] , where \[\mathbf{\overrightarrow {{\beta _1}} }\] is parallel to \[\mathbf{\overrightarrow \alpha  }\] and \[\mathbf{\overrightarrow {{\beta _2}} }\] is perpendicular to \[\mathbf{\overrightarrow \alpha } \] .

Ans: It is given that \[\overrightarrow \alpha   = 3\hat i - \hat j\] and \[\overrightarrow \beta   = 2\hat i + \hat j + 3\hat k\] .

Since \[\vec \alpha \] is parallel to \[\overrightarrow {{\beta _1}} \] , that implies \[\overrightarrow {{\beta _1}}  = \lambda \overrightarrow \alpha  \] .

\[ \Rightarrow \overrightarrow {{\beta _1}}  = \lambda (3\hat i - \hat j)\]

Further, \[\overrightarrow \beta   = \overrightarrow {{\beta _1}}  + \overrightarrow {{\beta _2}} \]

\[ \Rightarrow 2\hat i + \hat j + 3\hat k = [\lambda (3\hat i - \hat j)] + \overrightarrow {{\beta _2}} \]

\[ \Rightarrow \overrightarrow {{\beta _2}}  = (2 - 3\lambda )\hat i + (1 + \lambda )\hat j + 3\hat k\]

Now, \[\overrightarrow {{\beta _2}} \] is perpendicular to \[\vec \alpha \] , hence their dot product will be equal to zero.

\[ \Rightarrow \overrightarrow \alpha   \cdot \overrightarrow {{\beta _2}}  = 0\]

\[ \Rightarrow (3\hat i - \hat j) \cdot [(2 - 3\lambda )\hat i + (1 + \lambda )\hat j + 3\hat k] = 0\]

\[ \Rightarrow 3(2 - 3\lambda ) + ( - 1 - \lambda ) = 0\]

\[ \Rightarrow 6 - 9\lambda  - 1 - \lambda  = 0\]

\[ \Rightarrow 5 - 10\lambda  = 0\]

\[ \Rightarrow \lambda  = \frac{1}{2}\]

We calculate the value of \[\overrightarrow {{\beta _1}} \] and \[\overrightarrow {{\beta _2}} \] :

\[\overrightarrow {{\beta _1}}  = \lambda (3\hat i - \hat j)\]

\[ \Rightarrow \overrightarrow {{\beta _1}}  = \frac{1}{2}(3\hat i - \hat j)\]

\[ \Rightarrow \overrightarrow {{\beta _1}}  = \frac{3}{2}\hat i - \frac{1}{2}\hat j\]

Also, \[\overrightarrow {{\beta _2}}  = (2 - 3\lambda )\hat i + (1 + \lambda )\hat j + 3\hat k\]

\[ \Rightarrow \overrightarrow {{\beta _2}}  = [2 - 3(\frac{1}{2})]\hat i + (1 + \frac{1}{2})\hat j + 3\hat k\]

\[ \Rightarrow \overrightarrow {{\beta _2}}  = \frac{1}{2}\hat i + \frac{3}{2}\hat j + 3\hat k\]

Hence, we can say \[\overrightarrow \beta   = \left( {\frac{3}{2}\hat i - \frac{1}{2}\hat j} \right) + \left( {\frac{1}{2}\hat i + \frac{3}{2}\hat j + 3\hat k} \right)\] .


32. If \[\mathbf{\overrightarrow a }\] , \[\mathbf{\overrightarrow b }\] , \[\mathbf{\overrightarrow c }\] are three vectors such that \[\mathbf{\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0}\] then prove that \[\mathbf{\overrightarrow a  \times \overrightarrow b  = \overrightarrow b  \times \overrightarrow c  = \overrightarrow c  \times \overrightarrow a} \] .

Ans: We know that \[\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0\] .

Cross multiplying both sides by \[\overrightarrow a \] :

\[\overrightarrow a  \times (\overrightarrow a  + \overrightarrow b  + \overrightarrow c ) = \overrightarrow a  \times \overrightarrow 0 \]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b  + \overrightarrow a  \times \overrightarrow c  = 0\]

\[ \Rightarrow 0 + \overrightarrow a  \times \overrightarrow b  - \overrightarrow c  \times \overrightarrow a  = 0\] (Since \[\overrightarrow a  \times \overrightarrow a  = 0\] and \[\overrightarrow a  \times \overrightarrow c  =  - \overrightarrow c  \times \overrightarrow a \] )

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = \overrightarrow c  \times \overrightarrow a \] ......(1)

Similarly, if we cross multiplying both sides of \[\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = \overrightarrow 0 \] by \[\overrightarrow b \] :

\[\overrightarrow b  \times (\overrightarrow a  + \overrightarrow b  + \overrightarrow c ) = \overrightarrow b  \times \overrightarrow 0 \]

\[ \Rightarrow \overrightarrow b  \times \overrightarrow a  + \overrightarrow b  \times \overrightarrow b  + \overrightarrow b  \times \overrightarrow c  = 0\]

\[ \Rightarrow  - \overrightarrow a  \times \overrightarrow b  + \overrightarrow b  \times \overrightarrow c  = 0\] (Since \[\overrightarrow b  \times \overrightarrow b  = 0\] and \[\overrightarrow b  \times \overrightarrow a  =  - \overrightarrow a  \times \overrightarrow b \] )

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  = \overrightarrow b  \times \overrightarrow c \] ......(2)

From (1) and (2) , we conclude that \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow b  \times \overrightarrow c  = \overrightarrow c  \times \overrightarrow a \] .


33. If \[\mathbf{|\overrightarrow a | = 3}\] , \[\mathbf{|\overrightarrow b | = 5}\] , \[\mathbf{|\overrightarrow c | = 7}\] and \[\mathbf{\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0}\] , find the angle between \[\mathbf{\overrightarrow a} \] and \[\mathbf{\overrightarrow b} \] .

Ans: We know that \[\overrightarrow a  + \overrightarrow b  + \overrightarrow c  = 0\] .

\[ \Rightarrow \overrightarrow a  + \overrightarrow b  =  - \overrightarrow c \]

Squaring both sides:

\[ \Rightarrow {(\overrightarrow a  + \overrightarrow b )^2} = {( - \overrightarrow c )^2}\]

\[ \Rightarrow |\overrightarrow a {|^2} + |\overrightarrow b {|^2} + 2\overrightarrow a  \cdot \overrightarrow b  = | - \overrightarrow c {|^2}\]

\[ \Rightarrow {3^2} + {5^2} + 2\overrightarrow a  \cdot \overrightarrow b  = {( - 7)^2}\] (Since \[|\overrightarrow a | = 3\] , \[|\overrightarrow b | = 5\] , \[|\overrightarrow c | = 7\] )

\[ \Rightarrow 9 + 25 + 2\overrightarrow a  \cdot \overrightarrow b  = 49\]

\[ \Rightarrow 2\overrightarrow a  \cdot \overrightarrow b  = 15\]

\[ \Rightarrow 2(|\overrightarrow a ||\overrightarrow b |\cos \theta ) = 15\]

\[ \Rightarrow 2(3 \cdot 5 \cdot \cos \theta ) = 15\]

\[ \Rightarrow \cos \theta  = \frac{1}{2}\]

The angle between \[\overrightarrow a \] and \[\overrightarrow b \] is \[\frac{\pi }{3}\] .


34. Let \[\mathbf{\overrightarrow a  = \hat i - \hat j}\] , \[\mathbf{\overrightarrow b  = 3\hat j - \hat k}\] and \[\mathbf{\overrightarrow c  = 7\hat i - \hat k}\] , find a vector \[\mathbf{\overrightarrow d }\] which is perpendicular to \[\mathbf{\overrightarrow a} \] and \[\mathbf{\overrightarrow b }\] and \[\mathbf{\overrightarrow c  \cdot \overrightarrow d  = 1}\] .

Ans: It is given that \[\overrightarrow d \] is perpendicular to both \[\overrightarrow a \] and \[\overrightarrow b \] .

That implies \[\overrightarrow d  = \lambda (\overrightarrow a  \times \overrightarrow b )\] .

\[\overrightarrow d  = \lambda \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ 1&{ - 1}&0\\ 0&3&{ - 1} \end{array}} \right)\]

\[ \Rightarrow \overrightarrow d  = \lambda [\hat i(1) - \hat j( - 1) + \hat k(3)]\]

\[ \Rightarrow \overrightarrow d  = \lambda (\hat i + \hat j + 3\hat k)\]

Also, \[\overrightarrow c  \cdot \overrightarrow d  = 1\] .

\[ \Rightarrow (7\hat i - \hat k) \cdot [\lambda (\hat i + \hat j + 3\hat k)] = 1\]

\[ \Rightarrow 7\lambda  + 0 - 3\lambda  = 1\]

\[ \Rightarrow 4\lambda  = 1\]

\[ \Rightarrow \lambda  = \frac{1}{4}\]

Hence, \[\overrightarrow d  = \frac{1}{4}(\hat i + \hat j + 3\hat k)\]


35. If \[\mathbf{\overrightarrow a  = \hat i + \hat j + \hat k}\] , \[\mathbf{\overrightarrow c  = \hat j - \hat k}\] are the given vectors then find a vector \[\mathbf{\overrightarrow b }\] satisfying the equation \[\mathbf{\overrightarrow a  \times \overrightarrow b  = \overrightarrow c }\] , \[\mathbf{\overrightarrow a  \cdot \overrightarrow b  = 3}\] .

Ans: Assume \[\overrightarrow b  = x\hat i + y\hat j + z\hat k\] .

Since \[\overrightarrow a  \cdot \overrightarrow b  = 3\] :

\[(\hat i + \hat j + \hat k) \cdot (x\hat i + y\hat j + z\hat k) = 3\]

\[ \Rightarrow x + y + z = 3\] ......(1)

Now, we have \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow c \] :

\[ \Rightarrow (\hat i + \hat j + \hat k) \times (x\hat i + y\hat j + z\hat k) = \hat j - \hat k\]

\[ \Rightarrow \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ 1&1&1\\ x&y&z \end{array}} \right) = \hat j - \hat k\]

\[ \Rightarrow \hat i(z - y) - \hat j(z - x) + \hat k(y - x) = \hat j - \hat k\]

On comparing, we find that \[z - y = 0\] , that is, \[y = z\] .

Further, \[ - z + x = 1\] , that is, \[x = 1 + z\] .

From (1) , we have:

\[x + y + z = 3\]

\[ \Rightarrow 1 + z + z + z = 3\] (Since \[y = z\] and \[x = 1 + z\] )

\[ \Rightarrow 3z = 2\]

\[ \Rightarrow z = \frac{2}{3}\]

\[ \Rightarrow y = \frac{2}{3}\]

\[ \Rightarrow x = \frac{5}{3}\]

Hence, \[\overrightarrow b  = \frac{{5\hat i + 2\hat j + 2\hat k}}{3}\] .


36. Find a unit vector perpendicular to plane ABC, when position vectors of A, B, C are \[\mathbf{3\hat i - \hat j + 2\hat k}\] , \[\mathbf{\hat i - \hat j - 3\hat k}\] and \[\mathbf{4\hat i - 3\hat j + \hat k}\] respectively.

Ans: We know that given any two vectors, their cross product will result in a vector that is perpendicular to the plane that the two vectors lie in.

Accordingly, we need to find a unit vector in the direction of \[\overrightarrow {AB}  \times \overrightarrow {AC} \] .

First, we find \[\overrightarrow {AB}  = \overrightarrow {OB}  - \overrightarrow {OA} \] :

\[\overrightarrow {AB}  = (\hat i - \hat j - 3\hat k) - (3\hat i - \hat j + 2\hat k)\]

\[ \Rightarrow \overrightarrow {AB}  =  - 2\hat i - 5\hat k\]

Next, \[\overrightarrow {AC}  = \overrightarrow {OC}  - \overrightarrow {OA} \] :

\[\overrightarrow {AC}  = (4\hat i - 3\hat j + \hat k) - (3\hat i - \hat j + 2\hat k)\]

\[ \Rightarrow \overrightarrow {AC}  = \hat i - 2\hat j - \hat k\]

Further, \[\overrightarrow {AB}  \times \overrightarrow {AC}  = \left( {\begin{array}{*{20}{c}} {\hat i}&{\hat j}&{\hat k}\\ { - 2}&0&{ - 5}\\ 1&{ - 2}&{ - 1} \end{array}} \right)\]

\[\overrightarrow {AB}  \times \overrightarrow {AC}  =  - 10\hat i - 7\hat j - 4\hat k\]

\[|\overrightarrow {AB}  \times \overrightarrow {AC} | = \sqrt {{{( - 10)}^2} + {{( - 7)}^2} + {{( - 4)}^2}} \]

\[|\overrightarrow {AB}  \times \overrightarrow {AC} | = \sqrt {100 + 49 + 16} \]

\[|\overrightarrow {AB}  \times \overrightarrow {AC} | = \sqrt {165} \]

Hence, required unit vector is \[\frac{{\overrightarrow {AB}  \times \overrightarrow {AC} }}{{|\overrightarrow {AB}  \times \overrightarrow {AC} |}} = \frac{{ - 10\hat i - 7\hat j - 4\hat k}}{{\sqrt {165} }}\] .


37. For any two vectors, show that \[\mathbf{|\overrightarrow a  + \overrightarrow b | \le |\overrightarrow a | + |\overrightarrow b |}\] .

Ans: We take the square of \[\overrightarrow a  + \overrightarrow b \] :

\[{\left( {\overrightarrow a  + \overrightarrow b } \right)^2} = \overrightarrow a  \cdot \overrightarrow a  + \overrightarrow b  \cdot \overrightarrow a  + \overrightarrow a  \cdot \overrightarrow b  + \overrightarrow b  \cdot \overrightarrow b \]

\[ \Rightarrow {\left( {\overrightarrow a  + \overrightarrow b } \right)^2} = |\overrightarrow a {|^2} + 2\overrightarrow a  \cdot \overrightarrow b  + |\overrightarrow b {|^2}\]

\[ \Rightarrow {\left( {\overrightarrow a  + \overrightarrow b } \right)^2} = |\overrightarrow a {|^2} + 2\overrightarrow a  \cdot \overrightarrow b \cos \theta  + |\overrightarrow b {|^2}\]  ......(1)

We know that \[\cos \theta  \le 1\] .

Multiplying \[2\overrightarrow a  \cdot \overrightarrow b \] both sides:

\[2\overrightarrow a  \cdot \overrightarrow b \cos \theta  \le 2\overrightarrow a  \cdot \overrightarrow b \]

Adding \[|\overrightarrow a {|^2} + |\overrightarrow b {|^2}\] both sides:

\[|\overrightarrow a {|^2} + |\overrightarrow b {|^2} + 2\overrightarrow a  \cdot \overrightarrow b \cos \theta  \le |\overrightarrow a {|^2} + |\overrightarrow b {|^2} + 2\overrightarrow a  \cdot \overrightarrow b \]

\[ \Rightarrow |\overrightarrow a  + \overrightarrow b {|^2} \le {\left( {|\overrightarrow a | + |\overrightarrow b |} \right)^2}\] (From (1)) 

Hence proved, \[|\overrightarrow a  + \overrightarrow b {|^2} \le {\left( {|\overrightarrow a | + |\overrightarrow b |} \right)^2}\] .


38. Evaluate \[\mathbf{{\left( {\overrightarrow a  \times \hat i} \right)^2} + {\left( {\overrightarrow a  \times \hat j} \right)^2} + {\left( {\overrightarrow a  \times \hat k} \right)^2}}\] .

Ans: Let \[\overrightarrow a  = x\hat i + y\hat j + z\hat k\] .

So, \[\overrightarrow a  \times \hat i =  - y\hat k + z\hat j\]

\[\overrightarrow a  \times \hat j = x\hat k - z\hat i\]

\[\overrightarrow a  \times \hat k =  - x\hat j + y\hat i\]

Now, \[{\left( {\overrightarrow a  \times \hat i} \right)^2} + {\left( {\overrightarrow a  \times \hat j} \right)^2} + {\left( {\overrightarrow a  \times \hat k} \right)^2}\]

\[ \Rightarrow {y^2} + {z^2} + {x^2} + {z^2} + {x^2} + {y^2}\]

\[ \Rightarrow 2({x^2} + {y^2} + {z^2})\]

\[ \Rightarrow 2|\overrightarrow a {|^2}\]

Hence, \[{\left( {\overrightarrow a  \times \hat i} \right)^2} + {\left( {\overrightarrow a  \times \hat j} \right)^2} + {\left( {\overrightarrow a  \times \hat k} \right)^2} = 2|\overrightarrow a {|^2}\] .


39. If \[\mathbf{\hat a}\] and \[\mathbf{\hat b}\] are unit vectors inclined at an angle \[\mathbf{\theta} \] then prove that:

i. \[\mathbf{\sin \frac{\theta }{2} = \frac{1}{2}\left| {\hat a - \hat b} \right|}\]

Ans: Taking \[|\hat a - \hat b{|^2} = \hat a \cdot \hat a + \hat b \cdot \hat b - 2\hat a \cdot \hat b\] :

\[ \Rightarrow |\hat a - \hat b{|^2} = |\hat a{|^2} + |\hat b{|^2} - 2|\hat a||\hat b|\cos \theta \]

\[ \Rightarrow |\hat a - \hat b{|^2} = 1 + 1 - 2(1)(1)\cos \theta \] (Since they are unit vectors, their magnitude is equal to one)

\[ \Rightarrow |\hat a - \hat b{|^2} = 2(1 - \cos \theta )\]

\[ \Rightarrow \frac{{|\hat a - \hat b{|^2}}}{2} = 1 - \cos \theta \]

\[ \Rightarrow \frac{{|\hat a - \hat b{|^2}}}{2} = 2{\sin ^2}\frac{\theta }{2}\]

\[ \Rightarrow \frac{{|\hat a - \hat b{|^2}}}{4} = {\sin ^2}\frac{\theta }{2}\]

\[ \Rightarrow \frac{{|\hat a - \hat b|}}{2} = \sin \frac{\theta }{2}\] ......(1)

Hence proved.

ii. \[\mathbf{\tan \frac{\theta }{2} = \left| {\frac{{\hat a - \hat b}}{{\hat a + \hat b}}} \right|}\]

Ans: Taking \[|\hat a + \hat b{|^2} = \hat a \cdot \hat a + \hat b \cdot \hat b + 2\hat a \cdot \hat b\] :

\[ \Rightarrow |\hat a + \hat b{|^2} = |\hat a{|^2} + |\hat b{|^2} + 2|\hat a||\hat b|\cos \theta \]

\[ \Rightarrow |\hat a + \hat b{|^2} = 1 + 1 + 2(1)(1)\cos \theta \] (Since they are unit vectors, their magnitude is equal to one)

\[ \Rightarrow |\hat a + \hat b{|^2} = 2(1 + \cos \theta )\]

\[ \Rightarrow \frac{{|\hat a + \hat b{|^2}}}{2} = 1 + \cos \theta \]

\[ \Rightarrow \frac{{|\hat a + \hat b{|^2}}}{2} = 2{\cos ^2}\frac{\theta }{2}\]

\[ \Rightarrow \frac{{|\hat a + \hat b{|^2}}}{4} = {\cos ^2}\frac{\theta }{2}\]

\[ \Rightarrow \frac{{|\hat a + \hat b|}}{2} = \cos \frac{\theta }{2}\] ......(2)

We know that \[\tan \frac{\theta }{2} = \frac{{\sin \frac{\theta }{2}}}{{\cos \frac{\theta }{2}}}\]

From (1) and (2) :

\[\tan \frac{\theta }{2} = \frac{{\frac{{|\hat a - \hat b|}}{2}}}{{\frac{{|\hat a + \hat b|}}{2}}}\]

\[\tan \frac{\theta }{2} = \left| {\frac{{\hat a - \hat b}}{{\hat a + \hat b}}} \right|\]

Hence proved. 


40. For any two vectors, show that \[\mathbf{|\overrightarrow a  \times \overrightarrow b | = \sqrt {{a^2}{b^2} - {{(\overrightarrow a  \cdot \overrightarrow b )}^2}} }\] .

Ans: Taking \[|\overrightarrow a  \times \overrightarrow b {|^2}\] :

\[|\overrightarrow a  \times \overrightarrow b {|^2} = {\left( {|\overrightarrow a ||\overrightarrow b |\sin \theta } \right)^2}\]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b {|^2} = |\overrightarrow a {|^2}|\overrightarrow b {|^2}{\sin ^2}\theta \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b {|^2} = |\overrightarrow a {|^2}|\overrightarrow b {|^2}(1 - {\cos ^2}\theta )\]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b {|^2} = |\overrightarrow a {|^2}|\overrightarrow b {|^2} - |\overrightarrow a {|^2}|\overrightarrow b {|^2}{\cos ^2}\theta \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b {|^2} = |\overrightarrow a {|^2}|\overrightarrow b {|^2} - {(\overrightarrow a  \cdot \overrightarrow b )^2}\]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {|\overrightarrow a {|^2}|\overrightarrow b {|^2} - {{(\overrightarrow a  \cdot \overrightarrow b )}^2}} \]

Hence proved.


41. \[\mathbf{\overrightarrow a  = \hat i + \hat j + \hat k}\] , \[\mathbf{\overrightarrow b  = \hat i - \hat j + 2\hat k}\] and \[\mathbf{\overrightarrow c  = x\hat i + (x - 2)\hat j - \hat k}\] . If \[\mathbf{\overrightarrow c }\] lies in the plane of \[\mathbf{\overrightarrow a }\] and \[\mathbf{\overrightarrow b }\] , then find the value of x .

Ans: We have \[\overrightarrow a  = \hat i + \hat j + \hat k\] , \[\overrightarrow b  = \hat i - \hat j + 2\hat k\] and \[\overrightarrow c  = x\hat i + (x - 2)\hat j - \hat k\] .

Since vectors \[\overrightarrow a ,\overrightarrow b ,\overrightarrow c \] are co-planar, that is, lying on the same plane, hence their scalar product will be equal to zero. 

\[ \Rightarrow [\overrightarrow a  \cdot \overrightarrow b  \cdot \overrightarrow c ] = 0\]

\[ \Rightarrow \left| {\begin{array}{*{20}{c}} 1&1&1\\ 1&{ - 1}&2\\ x&{x - 2}&{ - 1} \end{array}} \right| = 0\]

\[ \Rightarrow 1(1 - 2x + 4) - 1( - 1 - 2x) + 1(x - 2 + x) = 0\]

\[ \Rightarrow 5 - 2x + 1 + 2x - 2 + 2x = 0\]

\[ \Rightarrow 4 + 2x = 0\]

\[ \Rightarrow x =  - 2\]


42. Prove that the angle between any two diagonals of a cube is \[\mathbf{{\cos ^{ - 1}}\left( {\frac{1}{3}} \right)}\] .

Ans: Let us first graphically represent a cube to prove the required:

 

Graphical Representation of a Cube


Let a be the edge of the cube with its centre \[O\] at the origin. The diagonals of this cube are AD, OG, BE and CF. 

Let us consider the diagonals AD and OG. 

\[\overrightarrow {OG}  = a\hat i + a\hat j + a\hat k\]

\[\overrightarrow {AD}  = \overrightarrow {OD}  - \overrightarrow {OA} \]

\[ \Rightarrow \overrightarrow {AD}  = (0 - a)\hat i + (a - 0)\hat j + (a - 0)\hat k\]

\[ \Rightarrow \overrightarrow {AD}  =  - a\hat i + a\hat j + a\hat k\]

Now, let the angle between them be \[\theta \] :

\[\cos \theta  = \frac{{\overrightarrow {AD}  \cdot \overrightarrow {OG} }}{{|\overrightarrow {AD} ||\overrightarrow {OG} |}}\]

\[ \Rightarrow \cos \theta  = \frac{{a( - a) + a(a) + a(a)}}{{\sqrt {{a^2} + {a^2} + {a^2}} \sqrt {{{( - a)}^2} + {a^2} + {a^2}} }}\]

\[ \Rightarrow \cos \theta  = \frac{{ - {a^2} + {a^2} + {a^2}}}{{\sqrt {3{a^2}} \sqrt {3{a^2}} }}\]

\[ \Rightarrow \cos \theta  = \frac{{{a^2}}}{{3{a^2}}}\]

\[ \Rightarrow \cos \theta  = \frac{1}{3}\]

\[ \Rightarrow \theta  = {\cos ^{ - 1}}\left( {\frac{1}{3}} \right)\]

Similarly, the angle between BE and CF will also be \[{\cos ^{ - 1}}\left( {\frac{1}{3}} \right)\] .

Hence proved.


43. Let \[\mathbf{\hat a,\hat b,\hat c}\] are unit vectors such that \[\mathbf{\hat a \cdot \hat b{\rm{ = }}\hat a \cdot \hat c = 0}\]and the angle between \[\mathbf{\hat b}\] and \[\mathbf{\hat c}\] is \[\mathbf{\frac{\pi }{6}}\] , then prove that \[\mathbf{\hat a =  \pm 2(\hat b \times \hat c)}\] .

Ans: Since \[\hat a \cdot \hat b{\rm{ = }}\hat a \cdot \hat c = 0\] , it means that \[\hat a\] is perpendicular to both \[\hat b\] and \[\hat c\] .

This further implies that \[\hat a\] is perpendicular to the plane in which \[\hat b\] and \[\hat c\] lie.

Also, \[\hat b \times \hat c = |\hat b||\hat c|\sin \theta \hat n\]  , where \[\theta \] is the angle between \[\hat b\] and \[\hat c\] , and \[\hat n\] is a unit vector perpendicular to the plane in which \[\hat b\] and \[\hat c\] lie.

\[ \Rightarrow \hat b \times \hat c = (1)(1)\sin \frac{\pi }{6}\hat a\]

(Since \[\hat b\] and \[\hat c\] are unit vectors, the angle between them is given to be \[\frac{\pi }{6}\] , and \[\hat a\] satisfies the conditions for \[\hat n\] )

\[ \Rightarrow \hat b \times \hat c = \sin \frac{\pi }{6}\hat a\]

\[ \Rightarrow \hat b \times \hat c = \frac{1}{2}\hat a\]

\[ \Rightarrow \hat a =  \pm 2(\hat b \times \hat c)\]

Hence proved.


44. Prove that the normal vector to the plane containing three points with

position vectors \[\overrightarrow a \] , \[\overrightarrow b \] and \[\overrightarrow c \] lies in the direction of vector \[\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b \] .

Ans: In a plane containing the vectors \[\overrightarrow a \] , \[\overrightarrow b \] and \[\overrightarrow c \] , let \[\overrightarrow n \] be its normal vector.

Therefore, \[\overrightarrow n  = \lambda (\overrightarrow {AB}  \times \overrightarrow {AC} )\] .

\[ \Rightarrow \overrightarrow n  = \lambda [(\overrightarrow b  - \overrightarrow a ) \times (\overrightarrow c  - \overrightarrow a )]\]

\[ \Rightarrow \overrightarrow n  = \lambda [(\overrightarrow b  - \overrightarrow a ) \times \overrightarrow c  - (\overrightarrow b  - \overrightarrow a ) \times \overrightarrow a ]\] (By distributive property)

\[ \Rightarrow \overrightarrow n  = \lambda (\overrightarrow b  \times \overrightarrow c  - \overrightarrow a  \times \overrightarrow c  - \overrightarrow b  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow a )\]

\[ \Rightarrow \overrightarrow n  = \lambda (\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b  + 0)\] (Since \[\overrightarrow a  \times \overrightarrow a  = 0\] , \[\overrightarrow a  \times \overrightarrow c  =  - \overrightarrow c  \times \overrightarrow a \] , \[\overrightarrow b  \times \overrightarrow a  =  - \overrightarrow a  \times \overrightarrow b \] )

\[ \Rightarrow \overrightarrow n  = \lambda (\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b )\]

Hence, we can say that \[\overrightarrow n \] lies in the direction of \[\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b \] .


45. If \[\mathbf{\overrightarrow a }\] , \[\mathbf{\overrightarrow b }\] and \[\mathbf{\overrightarrow c }\] are position vectors of the vertices A, B and C of a triangle ABC, then show that the area of ABC is \[\mathbf{\frac{1}{2}\left| {\overrightarrow a  \times \overrightarrow b  + \overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a } \right|}\] .

Ans: Let us consider a parallelogram ABCD:


A Parallelogram ABCD:


Area of ABCD will be \[\overrightarrow {AB}  \times \overrightarrow {AC} \] , that is, the product of two adjacent vectors.

Hence, area of \[ABC\] will be \[\frac{1}{2}\left( {\overrightarrow {AB}  \times \overrightarrow {AC} } \right)\] .

\[ \Rightarrow \frac{1}{2}\left( {(\overrightarrow b  - \overrightarrow a ) \times (\overrightarrow c  - \overrightarrow a )} \right)\]

\[ \Rightarrow \frac{1}{2}\left( {(\overrightarrow b  - \overrightarrow a ) \times \overrightarrow c  - (\overrightarrow b  - \overrightarrow a ) \times \overrightarrow a } \right)\]

\[ \Rightarrow \frac{1}{2}\left( {\overrightarrow b  \times \overrightarrow c  - \overrightarrow a  \times \overrightarrow c  - \overrightarrow b  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow a } \right)\]

\[ \Rightarrow \frac{1}{2}\left( {\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b  + 0} \right)\] (Since \[\overrightarrow a  \times \overrightarrow a  = 0\] , \[\overrightarrow a  \times \overrightarrow c  =  - \overrightarrow c  \times \overrightarrow a \] , \[\overrightarrow b  \times \overrightarrow a  =  - \overrightarrow a  \times \overrightarrow b \] )

\[ \Rightarrow \frac{1}{2}\left( {\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow a  + \overrightarrow a  \times \overrightarrow b } \right)\]

Hence proved.


46. If \[\mathbf{\overrightarrow a  \times \overrightarrow b  = \overrightarrow c  \times \overrightarrow d }\] and \[\mathbf{\overrightarrow a  \times \overrightarrow c  = \overrightarrow b  \times \overrightarrow d} \] , then prove that \[\mathbf{\overrightarrow a  - \overrightarrow d} \] is parallel to \[\mathbf{\overrightarrow b  - \overrightarrow c} \] provided \[\mathbf{\overrightarrow a  \ne \overrightarrow d }\] and \[\mathbf{\overrightarrow b  \ne \overrightarrow c }\] .

Ans: For vectors \[\overrightarrow a  - \overrightarrow d \] and \[\overrightarrow b  - \overrightarrow c \] to be parallel, their cross product must be equal to zero.

\[ \Rightarrow \left( {\overrightarrow a  - \overrightarrow d } \right) \times \left( {\overrightarrow b  - \overrightarrow c } \right) \]

\[ \Rightarrow (\overrightarrow a  - \overrightarrow d ) \times \overrightarrow b  - (\overrightarrow a  - \overrightarrow d ) \times \overrightarrow c \]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  - \overrightarrow d  \times \overrightarrow b  - \overrightarrow a  \times \overrightarrow c  + \overrightarrow d  \times \overrightarrow c \]

\[ \Rightarrow \overrightarrow a  \times \overrightarrow b  + \overrightarrow b  \times \overrightarrow d  - \overrightarrow a  \times \overrightarrow c  - \overrightarrow c  \times \overrightarrow d \] (Since \[ - \overrightarrow d  \times \overrightarrow b  = \overrightarrow b  \times \overrightarrow d \] and \[\overrightarrow d  \times \overrightarrow c  =  - \overrightarrow c  \times \overrightarrow d \] )

\[ \Rightarrow 0\] (Since \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow c  \times \overrightarrow d \] and \[\overrightarrow a  \times \overrightarrow c  = \overrightarrow b  \times \overrightarrow d \] )

Hence proved.


47. Dot product of a vector with vectors \[\mathbf{\hat i + \hat j - 3\hat k}\] , \[\mathbf{\hat i + 3\hat j - 2\hat k}\] and \[\mathbf{2\hat i + \hat j + 4\hat k}\] is 0 , 5 and 8 respectively. Find the vector.

Ans: Let the required vector be \[\overrightarrow h  = x\hat i + y\hat j + z\hat k\] . We have given \[\overrightarrow a  = \hat i + \hat j - 3\hat k\] , \[\overrightarrow b  = \hat i + 3\hat j - 2\hat k\] , \[\overrightarrow c  = 2\hat i + \hat j + 4\hat k\] and \[\overrightarrow a  \cdot \overrightarrow h  = 0\] , \[\overrightarrow b  \cdot \overrightarrow h  = 5\] , \[\overrightarrow c  \cdot \overrightarrow h  = 8\] .

Since \[\overrightarrow a  \cdot \overrightarrow h  = 0\] :

\[(\hat i + \hat j - 3\hat k) \cdot (x\hat i + y\hat j + z\hat k) = 0\]

\[ \Rightarrow x + y - 3z = 0\] ......(1)

Since \[\overrightarrow b  \cdot \overrightarrow h  = 5\] :

\[(\hat i + 3\hat j - 2\hat k) \cdot (x\hat i + y\hat j + z\hat k) = 5\]

\[ \Rightarrow x + 3y - 2z = 5\] ......(2)

Since \[\overrightarrow c  \cdot \overrightarrow h  = 8\] :

\[(2\hat i + \hat j + 4\hat k) \cdot (x\hat i + y\hat j + z\hat k) = 8\]

\[ \Rightarrow 2x + y + 4z = 8\] ......(3)

Subtract equation (1) from (2) :

\[\left( {x + 3y - 2z} \right) - \left( {x + y - 3z} \right) = 5\]

\[ \Rightarrow 2y + z = 5\]

\[ \Rightarrow y = \frac{{5 - z}}{2}\]

Subtract equation (1) from (3) :

\[\left( {2x + y + 4z} \right) - \left( {x + y - 3z} \right) = 8\]

\[ \Rightarrow x + 7z = 8\]

\[ \Rightarrow x = 8 - 7z\]

Substituting in (1) :

\[x + y - 3z = 0\]

\[ \Rightarrow 8 - 7z + \frac{{5 - z}}{2} - 3z = 0\]

\[ \Rightarrow 8 - 10z + \frac{{5 - z}}{2} = 0\]

\[ \Rightarrow \frac{{16 - 20z + 5 - z}}{2} = 0\]

\[ \Rightarrow \frac{{21 - 21z}}{2} = 0\]

\[ \Rightarrow 21 - 21z = 0\]

\[ \Rightarrow z = 1\]

Now, \[x = 8 - 7(1)\]

\[ \Rightarrow x = 1\]

Also, \[y = \frac{{5 - 1}}{2}\]

\[ \Rightarrow y = 2\]

Hence, we have \[\overrightarrow h  = \hat i + 2\hat j + \hat k\] .


48. If \[\mathbf{\overrightarrow a  = 5\hat i - \hat j + 7\hat k}\] , \[\mathbf{\hat b = \hat i - \hat j - \lambda \hat k}\] , find \[\mathbf{\lambda} \] such that \[\mathbf{\overrightarrow a  + \overrightarrow b} \] and \[\mathbf{\overrightarrow a  - \overrightarrow b }\] are orthogonal. 

Ans: If \[\overrightarrow a  + \overrightarrow b \] and \[\overrightarrow a  - \overrightarrow b \] are orthogonal, it implies that their dot product is zero.

We find \[\overrightarrow a  + \overrightarrow b \] :

\[\overrightarrow a  + \overrightarrow b  = (5\hat i - \hat j + 7\hat k) + (\hat i - \hat j - \lambda \hat k)\]

\[ \Rightarrow \overrightarrow a  + \overrightarrow b  = 6\hat i - 2\hat j + (7 - \lambda )\hat k\]

Similarly, we find \[\overrightarrow a  - \overrightarrow b \] :

\[\overrightarrow a  - \overrightarrow b  = (5\hat i - \hat j + 7\hat k) - (\hat i - \hat j - \lambda \hat k)\]

\[ \Rightarrow \overrightarrow a  - \overrightarrow b  = 4\hat i + (7 + \lambda )\hat k\]

Now, \[(\overrightarrow a  + \overrightarrow b ) \cdot (\overrightarrow a  - \overrightarrow b ) = 0\] :

\[ \Rightarrow [6\hat i - 2\hat j + (7 - \lambda )\hat k] \cdot [4\hat i + (7 + \lambda )\hat k] = 0\]

\[ \Rightarrow 24 + 0 + 49 - {\lambda ^2} = 0\]

\[ \Rightarrow {\lambda ^2} = 73\]

\[ \Rightarrow \lambda  = \sqrt {73} \]


49. Let \[\mathbf{\overrightarrow a }\] and \[\mathbf{\overrightarrow b }\] be vectors such that \[\mathbf{|\overrightarrow a | = |\overrightarrow b | = |\overrightarrow a  - \overrightarrow b | = 1}\] , then find \[\mathbf{|\overrightarrow a  + \overrightarrow b |}\] .

Ans: Let us take \[|\overrightarrow a  - \overrightarrow b | = 1\] and square both sides:

\[ \Rightarrow |\overrightarrow a  - \overrightarrow b {|^2} = {1^2}\]

\[ \Rightarrow |\overrightarrow a {|^2} + |\overrightarrow b {|^2} - 2\overrightarrow a  \cdot \overrightarrow b  = 1\]

\[ \Rightarrow 1 + 1 - 2(|\overrightarrow a ||\overrightarrow b |\cos \theta ) = 1\] (Since \[|\overrightarrow a | = |\overrightarrow b | = 1\] )

\[ \Rightarrow 2 - 2\cos \theta  = 1\]

\[ \Rightarrow 2\cos \theta  = 1\]

\[ \Rightarrow \cos \theta  = \frac{1}{2}\]

Now, let us take \[|\overrightarrow a  + \overrightarrow b |\]:

\[ \Rightarrow \sqrt {|\overrightarrow a {|^2} + |\overrightarrow b {|^2} + 2\overrightarrow a  \cdot \overrightarrow b } \]

\[ \Rightarrow \sqrt {1 + 1 + 2(|\overrightarrow a ||\overrightarrow b |\cos \theta )} \] (Since \[|\overrightarrow a | = |\overrightarrow b | = 1\] )

\[ \Rightarrow \sqrt {2 + 2(\frac{1}{2})} \]

\[ \Rightarrow \sqrt {2 + 1} \]

\[ \Rightarrow \sqrt 3 \]


50. If \[\mathbf{|\overrightarrow a | = 2}\] , \[\mathbf{|\overrightarrow b | = 5}\] and \[\mathbf{\overrightarrow a  \times \overrightarrow b  = 2\hat i + \hat j - 2\hat k}\] , find the value of \[\mathbf{\overrightarrow a  \cdot \overrightarrow b} \] .

Ans: Let us find \[|\overrightarrow a  \times \overrightarrow b |\] , given that \[\overrightarrow a  \times \overrightarrow b  = 2\hat i + \hat j - 2\hat k\] : 

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt {{2^2} + {1^2} + {{( - 2)}^2}} \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = \sqrt 9 \]

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = 3\]

Now, \[|\overrightarrow a  \times \overrightarrow b | = |\overrightarrow a ||\overrightarrow b |\sin \theta \]

\[ \Rightarrow 3 = (2)(5)\sin \theta \]

\[ \Rightarrow \sin \theta  = \frac{3}{{10}}\]

Now, \[\overrightarrow a  \cdot \overrightarrow b  = |\overrightarrow a ||\overrightarrow b |\cos \theta \] :

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = (2)(5)\cos ({\sin ^{ - 1}}\frac{3}{{10}})\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = (2)(5)\cos ({\sin ^{ - 1}}\frac{3}{{10}})\]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = 10\cos ({\cos ^{ - 1}}\sqrt {1 - {{\left( {\frac{3}{{10}}} \right)}^2}} )\] (Since \[{\sin ^{ - 1}}x = {\cos ^{ - 1}}\sqrt {1 - {x^2}} \] )

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = 10\sqrt {\frac{{91}}{{100}}} \]

\[ \Rightarrow \overrightarrow a  \cdot \overrightarrow b  = \sqrt {91} \]


51. \[\mathbf{\overrightarrow a ,\overrightarrow b ,\overrightarrow c }\] are three vectors such that \[\mathbf{\overrightarrow b  \times \overrightarrow c  = \overrightarrow a }\] and \[\mathbf{\overrightarrow a  \times \overrightarrow b  = \overrightarrow c} \] . Prove that \[\mathbf{\overrightarrow a ,\overrightarrow b ,\overrightarrow c }\] are mutually perpendicular to each other and \[\mathbf{|\overrightarrow b | = 1}\] , \[\mathbf{|\overrightarrow c | = |\overrightarrow a |}\] .

Ans: We know that \[\overrightarrow b  \times \overrightarrow c  = \overrightarrow a \] and \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow c \] .

Since \[\overrightarrow b  \times \overrightarrow c  = \overrightarrow a \] , we can say that \[\overrightarrow b  \bot \overrightarrow a \] and \[\overrightarrow c  \bot \overrightarrow a \] .

Similarly, since \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow c \] , we conclude that \[\overrightarrow a  \bot \overrightarrow c \] and \[\overrightarrow b  \bot \overrightarrow c \] .

From above statements, we can observe that \[\overrightarrow a  \bot \overrightarrow b \] , \[\overrightarrow b  \bot \overrightarrow c \] , \[\overrightarrow a  \bot \overrightarrow c \] , that is, all three vectors are mutually perpendicular.

Now, we have \[\overrightarrow a  \times \overrightarrow b  = \overrightarrow c \] .

\[ \Rightarrow |\overrightarrow a  \times \overrightarrow b | = |\overrightarrow c |\]

\[ \Rightarrow |\overrightarrow a ||\overrightarrow b |\sin \theta  = |\overrightarrow c |\]

\[ \Rightarrow |\overrightarrow a ||\overrightarrow b |\sin \frac{\pi }{2} = |\overrightarrow c |\] (Since vectors are mutually perpendicular, they are at a right angle with each other)

\[ \Rightarrow |\overrightarrow a ||\overrightarrow b | = |\overrightarrow c |\] (Since \[\sin \frac{\pi }{2} = 1\] ) ......(1)

Similarly, we have \[\overrightarrow b  \times \overrightarrow c  = \overrightarrow a \] .

\[ \Rightarrow |\overrightarrow b  \times \overrightarrow c | = |\overrightarrow a |\]

\[ \Rightarrow |\overrightarrow b ||\overrightarrow c |\sin \theta  = |\overrightarrow a |\]

\[ \Rightarrow |\overrightarrow b ||\overrightarrow c |\sin \frac{\pi }{2} = |\overrightarrow a |\] (Since vectors are mutually perpendicular, they are at a right angle with each other)

\[ \Rightarrow |\overrightarrow b ||\overrightarrow c | = |\overrightarrow a |\] (Since \[\sin \frac{\pi }{2} = 1\] ) ......(2)

Divide (2) by (1) :

\[ \Rightarrow \frac{{|\overrightarrow a ||\overrightarrow b |}}{{|\overrightarrow b ||\overrightarrow c |}} = \frac{{|\overrightarrow c |}}{{|\overrightarrow a |}}\]

\[ \Rightarrow \frac{{|\overrightarrow a |}}{{|\overrightarrow c |}} = \frac{{|\overrightarrow c |}}{{|\overrightarrow a |}}\]

\[ \Rightarrow |\overrightarrow a {|^2} = |\overrightarrow c {|^2}\]

\[ \Rightarrow |\overrightarrow a | = |\overrightarrow c |\] ......(3)

Substituting (3) in (2) :

\[|\overrightarrow b ||\overrightarrow a | = |\overrightarrow a |\]

\[ \Rightarrow |\overrightarrow b | = 1\]

Hence proved.


52. If \[\mathbf{\overrightarrow a  = 2\hat i - 3\hat j}\] , \[\mathbf{\overrightarrow b  = \hat i + \hat j - \hat k}\] and \[\mathbf{\overrightarrow c  = 3\hat i - \hat k}\] , find \[\mathbf{[\overrightarrow a \overrightarrow b \overrightarrow c ]}\] .

Ans: It is given that \[\overrightarrow a  = 2\hat i - 3\hat j\] , \[\overrightarrow b  = \hat i + \hat j - \hat k\] and \[\overrightarrow c  = 3\hat i - \hat k\] .

We know that \[[\overrightarrow a \overrightarrow b \overrightarrow c ] = \left( {\begin{array}{*{20}{c}} {{a_1}}&{{a_2}}&{{a_3}}\\ {{b_1}}&{{b_2}}&{{b_3}}\\ {{c_1}}&{{c_2}}&{{c_3}} \end{array}} \right)\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = \left( {\begin{array}{*{20}{c}} 2&{ - 3}&0\\ 1&1&{ - 1}\\ 3&0&{ - 1} \end{array}} \right)\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = 2( - 1) + 3( - 1 + 3) + 0\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] =  - 2 + 6\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = 4\]


53. Find volume of parallelepiped whose coterminous edges are given by vectors \[\mathbf{\overrightarrow a  = 2\hat i + 3\hat j + 4\hat k}\] , \[\mathbf{\overrightarrow b  = \hat i + 2\hat j - \hat k}\] and \[\mathbf{\overrightarrow c  = 3\hat i - \hat j + 2\hat k}\] .

Ans: To find the volume of parallelepiped whose coterminous edges are given by vectors \[\overrightarrow a  = 2\hat i + 3\hat j + 4\hat k\] , \[\overrightarrow b  = \hat i + 2\hat j - \hat k\] and \[\overrightarrow c  = 3\hat i - \hat j + 2\hat k\] , we simply take the scalar triple product of them:

\[[\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| {\begin{array}{*{20}{c}} {{a_1}}&{{a_2}}&{{a_3}}\\ {{b_1}}&{{b_2}}&{{b_3}}\\ {{c_1}}&{{c_2}}&{{c_3}} \end{array}} \right|\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| {\begin{array}{*{20}{c}} 2&3&4\\ 1&2&{ - 1}\\ 3&{ - 1}&2 \end{array}} \right|\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| {2(3) - 3(5) + 4( - 7)} \right|\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| {6 - 15 - 28} \right|\]

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| { - 37} \right|\]

Hence, the volume of parallelepiped is \[37\] cubic units.


54. Find the value of \[\lambda \] such that \[\mathbf{\overrightarrow a  = \hat i - \hat j + \hat k}\] , \[\mathbf{\overrightarrow b  = 2\hat i + \hat j - \hat k}\] and \[\mathbf{\overrightarrow c  = \lambda \hat i - \hat j + \lambda \hat k}\] are coplanar.

Ans: When three vectors are coplanar, their scalar triple product is zero.

We have \[\overrightarrow a  = \hat i - \hat j + \hat k\] , \[\overrightarrow b  = 2\hat i + \hat j - \hat k\] and \[\overrightarrow c  = \lambda \hat i - \hat j + \lambda \hat k\] .

\[[\overrightarrow a \overrightarrow b \overrightarrow c ] = \left| {\begin{array}{*{20}{c}} {{a_1}}&{{a_2}}&{{a_3}}\\ {{b_1}}&{{b_2}}&{{b_3}}\\ {{c_1}}&{{c_2}}&{{c_3}} \end{array}} \right|\]

\[ \Rightarrow \left| {\begin{array}{*{20}{c}} 1&{ - 1}&1\\ 2&1&{ - 1}\\ \lambda &{ - 1}&\lambda \end{array}} \right| = 0\]

\[ \Rightarrow \left| {(\lambda  - 1) + (2\lambda  + \lambda ) + ( - 2 - \lambda )} \right| = 0\]

\[ \Rightarrow \left| {(3\lambda  - 3)} \right| = 0\]

\[ \Rightarrow \lambda  = 1\]


55. Show that the four points \[\mathbf{\left( {--1,{\rm{ }}4,{\rm{ }}--3} \right)}\] , \[\mathbf{\left( {3,{\rm{ }}2,{\rm{ }}--5} \right)}\] , \[\mathbf{\left( {--3,{\rm{ }}8,{\rm{ }}--5} \right)}\] , \[\mathbf{\left( {--3,{\rm{ }}2,{\rm{ }}1} \right)}\] are coplanar.

Ans: Given the four points A \[\left( {--1,{\rm{ }}4,{\rm{ }}--3} \right)\] , B \[\left( {3,{\rm{ }}2,{\rm{ }}--5} \right)\] , C \[\left( {3,{\rm{ }}2,{\rm{ }}--5} \right)\] , D \[\left( {--3,{\rm{ }}2,{\rm{ }}1} \right)\] :

Now, \[\overrightarrow {AB}  = \overrightarrow b  - \overrightarrow a \]

\[ \Rightarrow \overrightarrow {AB}  = 4\hat i - 2\hat j - 2\hat k\]

\[\overrightarrow {AC}  = \overrightarrow c  - \overrightarrow a \]

\[ \Rightarrow \overrightarrow {AC}  =  - 2\hat i + 4\hat j - 2\hat k\]

\[\overrightarrow {AD}  = \overrightarrow d  - \overrightarrow a \]

\[ \Rightarrow \overrightarrow {AD}  =  - 2\hat i - 2\hat j + 4\hat k\]

For the points A, B, C and D to be coplanar, we need to show that vectors \[\overrightarrow {AB} ,\overrightarrow {AC} \overrightarrow {,AD} \] are coplanar, that is, their triple product should be equal to zero. 

\[[\overrightarrow {AB} \overrightarrow {AC} \overrightarrow {AD} ] = \left| {\begin{array}{*{20}{c}} {{a_1}}&{{a_2}}&{{a_3}}\\ {{b_1}}&{{b_2}}&{{b_3}}\\ {{c_1}}&{{c_2}}&{{c_3}} \end{array}} \right|\]

\[ \Rightarrow [\overrightarrow {AB} \overrightarrow {AC} \overrightarrow {AD} ] = \left| {\begin{array}{*{20}{c}} 4&{ - 2}&{ - 2}\\ { - 2}&4&{ - 2}\\ { - 2}&{ - 2}&4 \end{array}} \right|\]

\[ \Rightarrow [\overrightarrow {AB} \overrightarrow {AC} \overrightarrow {AD} ] = \left| {4(12) + 2( - 12) - 2(12)} \right|\]

\[ \Rightarrow [\overrightarrow {AB} \overrightarrow {AC} \overrightarrow {AD} ] = \left| {48 - 24 - 24} \right|\]

\[ \Rightarrow [\overrightarrow {AB} \overrightarrow {AC} \overrightarrow {AD} ] = 0\]

Hence proved.


56. For any three vectors \[\mathbf{\overrightarrow a ,\overrightarrow b ,\overrightarrow c} \] prove that \[\mathbf{[\overrightarrow a  + \overrightarrow b  \cdot \overrightarrow b  + \overrightarrow c  \cdot \overrightarrow c  + \overrightarrow a ] = 2[\overrightarrow a  \cdot \overrightarrow b  \cdot \overrightarrow c ]}\] .

Ans: Let us consider \[[\overrightarrow a  + \overrightarrow b  \cdot \overrightarrow b  + \overrightarrow c  \cdot \overrightarrow c  + \overrightarrow a ]\] :

\[ \Rightarrow (\overrightarrow a  + \overrightarrow b ) \cdot [(\overrightarrow b  + \overrightarrow c ) \times (\overrightarrow c  + \overrightarrow a )]\]

\[ \Rightarrow (\overrightarrow a  + \overrightarrow b ) \cdot (\overrightarrow b  \times \overrightarrow c  + \overrightarrow c  \times \overrightarrow c  + \overrightarrow b  \times \overrightarrow a  + \overrightarrow c  \times \overrightarrow a )\]

\[ \Rightarrow (\overrightarrow a  + \overrightarrow b ) \cdot (\overrightarrow b  \times \overrightarrow c  + \overrightarrow b  \times \overrightarrow a  + \overrightarrow c  \times \overrightarrow a )\] (Since \[\overrightarrow c  \times \overrightarrow c  = 0\] )

\[ \Rightarrow \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c ) + \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow c ) + \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow a ) + \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow a ) + \overrightarrow a  \cdot (\overrightarrow c  \times \overrightarrow a ) + \overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a )\]

\[ \Rightarrow \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c ) + \overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a )\] (Since \[\overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow c ) = \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow a ) = \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow a ) = \overrightarrow a  \cdot (\overrightarrow c  \times \overrightarrow a ) = 0\] )

\[ \Rightarrow \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c ) + \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c )\] (Since \[\overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a ) = \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c )\] )

\[ \Rightarrow 2[\overrightarrow a \overrightarrow b \overrightarrow c ]\]

Hence proved. 


57. For any three vectors \[\mathbf{\overrightarrow a ,\overrightarrow b ,\overrightarrow c }\] prove that \[\mathbf{\overrightarrow a  - \overrightarrow b ,\overrightarrow b  - \overrightarrow c ,\overrightarrow c  - \overrightarrow a }\] are coplanar.

Ans: For \[\overrightarrow a  - \overrightarrow b ,\overrightarrow b  - \overrightarrow c ,\overrightarrow c  - \overrightarrow a \] to be coplanar, their scalar product should be equal to zero.

\[ \Rightarrow [\overrightarrow a  - \overrightarrow b  \cdot \overrightarrow b  - \overrightarrow c  \cdot \overrightarrow c  - \overrightarrow a ]\]

\[ \Rightarrow (\overrightarrow a  - \overrightarrow b ) \cdot [(\overrightarrow b  - \overrightarrow c ) \times (\overrightarrow c  - \overrightarrow a )]\]

\[ \Rightarrow (\overrightarrow a  - \overrightarrow b ) \cdot (\overrightarrow b  \times \overrightarrow c  - \overrightarrow c  \times \overrightarrow c  - \overrightarrow b  \times \overrightarrow a  + \overrightarrow c  \times \overrightarrow a )\]

\[ \Rightarrow (\overrightarrow a  - \overrightarrow b ) \cdot (\overrightarrow b  \times \overrightarrow c  - \overrightarrow b  \times \overrightarrow a  + \overrightarrow c  \times \overrightarrow a )\] (Since \[\overrightarrow c  \times \overrightarrow c  = 0\] )

\[ \Rightarrow \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c ) - \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow c ) - \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow a ) + \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow a ) + \overrightarrow a  \cdot (\overrightarrow c  \times \overrightarrow a ) - \overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a )\]

\[ \Rightarrow \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c ) - \overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a )\] (Since \[\overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow c ) = \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow a ) = \overrightarrow b  \cdot (\overrightarrow b  \times \overrightarrow a ) = \overrightarrow a  \cdot (\overrightarrow c  \times \overrightarrow a ) = 0\] )

\[ \Rightarrow [\overrightarrow a \overrightarrow b \overrightarrow c ] - [\overrightarrow a \overrightarrow b \overrightarrow c ]\] (Since \[\overrightarrow b  \cdot (\overrightarrow c  \times \overrightarrow a ) = \overrightarrow a  \cdot (\overrightarrow b  \times \overrightarrow c )\] )

\[ \Rightarrow 0\]

Hence proved.


Important Related Links for CBSE Class 12 Maths 

FAQs on Important Questions for CBSE Class 12 Maths Chapter 10 - Vector Algebra 2024-25

1. How can I download Vedantu’s Important Questions for Class 12 Mathematics Chapter 10 “Vector Algebra?”

Vedantu’s Important Questions for Chapter 10 “Vector Algebra” of Class 12 Mathematics can be downloaded in the following simple steps:

  • Visit the page of ‘NCERT Solutions for Chapter 10 Class 12 Maths’ on the official website of Vedantu (vedantu).

  • Find the exercise for which you want a solution and click on the ‘Download PDF’ link.

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These pdf files do not require high-speed internet for downloading and they are available absolutely free of cost.

2. How can Vedantu’s Important Questions for Chapter 10 benefit me?

If you are a student who is looking to score perfect marks in Class 12 Mathematics board exams or even preparing for competitive exams, Vedantu's Important Questions can be of great benefit to you.


These questions are handpicked by expert Mathematics teachers specifically for exam preparation.


They allow you to access all the important questions from each chapter in one place. This allows you to efficiently practice them. You can practice questions of different marking schemes with these.

3. What are the topics taught in Chapter 10 “Vector Algebra?”

Vector Algebra contains many important topics which can be asked in the board examination. These are the main topics taught in Chapter 10 "Vector Algebra":

  • Types of Vectors

  • Addition of Vectors 

  • Multiplication of  a vector by a scalar

  • Components of a vector

  • Vector joining two points

  • Section formula

  • Product of two vectors

Important Questions covering all the above-mentioned topics can be accessed and downloaded for free from Vedantu.

4. What type of questions are provided in Vedantu’s Important Questions for “Vector Algebra?”

Vedantu’s Important Questions for “Vector Algebra” contain questions of different marking schemes that can appear in board examinations. Vedantu provides important questions of 1 mark and 4 marks from this chapter. Usually, only such questions are asked in board exams from "Vector Algebra."


You can find a total of 57 important questions covering the entire chapter of "Vector Algebra" here. These questions provide you with perfect and thorough practice from this chapter. These are also useful for revision purposes.

5. Why should we study Vector Algebra?

Vector Algebra is not only an important chapter from the board and competitive examinations perspective but also has many real-time applications.


Vector Algebra finds several applications in our lives. These are especially used in situations involving force and velocity. They are also useful in computations of angles and distances, construction of network pipes, measuring distances between aircraft, etc. Vector Algebra is used widely in Civil Engineering. 


Hence students must practice this chapter well to strengthen its concepts.