Chapter 6: Applications of Vector Algebra

“Mathematics is the science of the connection of magnitudes. Magnitude is anything that can be put equal or unequal to another thing. Two things are equal when in every assertion each may be replaced by the other.”

Hermann Gunther Grassmann

6.1 Introduction

We are familiar with the concept of vectors, (vectors in Latin means “to carry”) from our XI standard text book. Further the modern version of Theory of Vectors arises from the ideas of Wessel(1745- 1818) and Argand (1768- 1822) when they attempt to describe the complex numbers geometrically as a directed line segment in a coordinate plane. We have seen that a vector has magnitude and direction and two vectors with same magnitude and direction regardless of positions of their initial points are always equal.

We also have studied addition of two vectors, scalar multiplication of vectors, dot product, and cross product by denoting an arbitrary vector by the notation \vec{a} or a*{i}\hat{i} +a*{j}\hat{j} +a_{k}\hat{k}. To understand the direction and magnitude of a given vector and all other concepts with a little more rigor, we shall recall the geometric introduction of vectors, which will be useful to discuss the equations of straight lines and planes. Great mathematicians Grassmann, Hamilton, Clifford and Gibbs were pioneers to introduce the dot and cross products of vectors.

The vector algebra has a few direct applications in physics and it has a lot of applications along with vector calculus in physics, engineering, and medicine. Some of them are mentioned below.

To calculate the volume of a parallelepiped, the scalar triple product is used. To find the work done and torque in mechanics, the dot and cross products are respectively used. To introduce curl and divergence of vectors, vector algebra is used along with calculus. Curl and divergence are very much used in the study of electromagnetism, hydrodynamics, blood flow, rocket launching, and the path of a satellite. To calculate the distance between two aircrafts in the space and the angle between their paths, the dot and cross products are used. To install the solar panels by carefully considering the tilt of the roof, and the direction of the Sun so that it generates more solar power, a simple application of dot product of vectors is used. One can calculate the amount of solar power generated by a solar panel by using vector algebra. To measure angles and distance between the panels in the satellites, in the construction of networks of pipes in various industries, and, in calculating angles and distance between beams and structures in civil engineering, vector algebra is used.

6.2 Geometric introduction to vectors

A vector \bar{\nu} is represented as a directed straight line segment in a 3- dimensional space \mathbb{R}^3, with an initial point A = (a*{1},a*{2},a*{3})\in \mathbb{R}^{3} and an end point B = (b*{1},b*{2},b*{3})\in \mathbb{R}^{3}, and it is denoted by \overline{AB}. The length of the line segment AB is the magnitude of the vector \bar{\nu} and the direction from A to B is the direction of the vector \bar{\nu}. Hereafter, a vector will be interchangeably denoted by \bar{\nu} or \overline{AB}. Two vectors \overline{AB} and \overline{CD} in \mathbb{R}^3 are said to be equal if and only if the length AB is equal to the length CD and the direction from A to B is parallel to the direction from C to D. If \overline{AB} and \overline{CD} are equal, we write \overline{AB} = \overline{CD}, and \overline{CD} is called a translate of \overline{AB}.

It is easy to observe that every vector \overline{AB} can be translated to anywhere in \mathbb{R}^3, equal to a vector with initial point U\in \mathbb{R}^3 and end point V\in \mathbb{R}^3 such that \overline{AB} = \overline{UV}. In particular, if O is the origin of \mathbb{R}^3, then a point P\in \mathbb{R}^3 can be found such that \overline{AB} = \overline{OP}. The vector \overline{OP} is called the position vector of the point P. Moreover, we observe that given any vector \bar{\nu}, there exists a unique point P\in \mathbb{R}^3 such that the position vector \overline{OP} of P is equal to \bar{\nu}. A vector \overline{AB} is said to be the zero vector if the initial point A is the same as the end point B. We use the standard notations \hat{i},\hat{j},\hat{k} and \bar{0} to denote the position vectors of the points (1,0,0),(0,1,0),(0,0,1), and (0,0,0), respectively. For a given point (a*{1},a*{2},a*{3})\in \mathbb{R}^{3}, a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k} is called the position vector of the point (a*{1},a*{2},a*{3}), which is the directed straight line segment with initial point (0,0,0) and end point (a*{1},a*{2},a*{3}). All real numbers are called scalars.

XII - Mathematics

Given a vector \overline{AB}, the length of the vector is calculated by

\sqrt{(b*{1} - a*{1})^{2} + (b*{2} - a*{2})^{2} + (b*{3} - a*{3})^{2}},

where A is (a*{1},a*{2},a*{3}) and B is (b*{1},b*{2},b*{3}). In particular, if a vector is the position vector \vec{b} of (b*{1},b*{2},b*{3}), then its length is \sqrt{b*{1}^{2} + b*{2}^{2} + b*{3}^{2}}. A vector having length 1 is called a unit vector. We use the notation \hat{a}, for a unit vector. Note that \hat{i},\hat{j}, and \hat{k} are unit vectors and \vec{0} is the unique vector with length 0. The direction of \vec{0} is specified according to the context.

The addition and scalar multiplication on vectors in 3- dimensional space are defined by

\vec{a} +\vec{b} = (a*{1} + b*{1})\hat{i} +(a*{2} + b*{2})\hat{j} +(a*{3} + b*{3})\hat{k}.

\alpha \vec{a} = (\alpha a*{1})\hat{i} +(\alpha a*{2})\hat{j} +(\alpha a_{3})\hat{k};

where

\vec{a} = a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k},\vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k}\in \mathbb{R}^{3}\mathrm{and}\alpha \in \mathbb{R}.

To see the geometric interpretation of \vec{a} +\vec{b}, let \vec{a} and \vec{b}, denote the position vectors of A = (a*{1},a*{2},a*{3}) and B = (b*{1},b*{2},b*{3}), respectively. Translate the position vector \vec{b} to the vector with initial point as A and end point as C = (c*{1},c*{2},c*{3}), for a suitable (c*{1},c*{2},c*{3})\in \mathbb{R}^{3}. See the Fig (6.2). Then, the position vector \vec{c} of the point (c*{1},c*{2},c_{3}) is equal to \vec{a} +\vec{b}.

The vector \alpha \vec{a} is another vector parallel to \vec{a} and its length is magnified (if \alpha >1 ) or contracted (if 0< \alpha < 1). If \alpha < 0, then \alpha \vec{a} is a vector whose magnitude is |\alpha | times that of \vec{a} and direction opposite to that of \vec{a}. In particular, if \alpha = - 1, then \alpha \vec{a} = -\vec{a} is the vector with same length and direction opposite to that of \vec{a}. See Fig. 6.3

6.3 Scalar Product and Vector Product

Next we recall the scalar product and vector product of two vectors as follows.

Definition 6.1

Given two vectors \vec{a} = a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k} and \vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k} the scalar product (or dot product) is denoted by \vec{a}\cdot \vec{b} and is calculated by

\vec{a}\cdot \vec{b} = a*{1}b*{1} + a*{2}b*{2} + a*{3}b*{3},

and the vector product (or cross product) is denoted by \vec{a}\times \vec{b}, and is calculated by

\vec{a}\times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix}

Note

\vec{a}\cdot \vec{b} is a scalar, and \vec{a}\times \vec{b} is a vector.

6.3.1 Geometrical interpretation

Geometrically, if \vec{a} is an arbitrary vector and \hat{n} is a unit vector, then \vec{a}\cdot \hat{n} is the projection of the vector \vec{a} on the straight line on which \hat{n} lies. The quantity \vec{a}\cdot \hat{n} is positive if the angle between \vec{a} and \hat{n} is acute, see Fig. 6.4 and negative if the angle between \vec{a} and \hat{n} is obtuse see Fig. 6.5.

If \vec{a} and \vec{b} are arbitrary non- zero vectors, then |\vec{a}\cdot \vec{b}| = \left|\vec{b}\mid \vec{a}\cdot \left(\frac{\vec{b}}{|\vec{b}|}\right)\right| = \left|\vec{a}\mid \vec{b}\cdot \left(\frac{\vec{a}}{|\vec{a}|}\right)\right| and so |\vec{a}\cdot \vec{b}| means either the length of the straight line segment obtained by projecting the vector |\vec{b}\mid \vec{a} along the direction of \vec{b} or the length of the line segment obtained by projecting the vector |\vec{a}\mid \vec{b} along the direction of \vec{a}. We recall that \vec{a}\cdot \vec{b} = |\vec{a} |\mid \vec{b} |\cos \theta, where \theta is the angle between the two vectors \vec{a} and \vec{b}. We recall that the angle between \vec{a} and \vec{b} is defined as the measure from \vec{a} to \vec{b} in the counter clockwise direction.

The vector \vec{a}\times \vec{b} is either \vec{0} or a vector perpendicular to the plane parallel to both \vec{a} and \vec{b} having magnitude as the area of the parallelogram formed by coterminus vectors parallel to \vec{a} and \vec{b}. If \vec{a} and \vec{b} are non- zero vectors, then the magnitude of \vec{a}\times \vec{b} can be calculated by the formula

|\vec{a}\times \vec{b}| = |\vec{a} |\mid \vec{b} |\mid \sin \theta |, \text{where} \theta \text{is the angle between} \vec{a} \text{and} \vec{b}.

Two vectors are said to be coterminus if they have same initial point.

(1) An angle between two non-zero vectors \vec{a} and \vec{b} is found by the following formula

\theta = \cos^{-1} \left( \frac{\vec{a}\cdot\vec{b}}{|\vec{a}||\vec{b}|} \right)

(2) \vec{a} and \vec{b} are said to be parallel if the angle between them is 0 or \pi.

(3) \vec{a} and \vec{b} are said to be perpendicular if the angle between them is \frac{\pi}{2} or \frac{3\pi}{2}.

Property

(1) Let \vec{a} and \vec{b} be any two nonzero vectors. Then

\vec{a}\cdot \vec{b} = 0 if and only if \vec{a} and \vec{b} are perpendicular to each other.

\vec{a}\times \vec{b} = \vec{0} if and only if \vec{a} and \vec{b} are parallel to each other.

(2) If \vec{a},\vec{b}, and \vec{c} are any three vectors and \alpha is a scalar, then

\vec{a}\cdot \vec{b} = \vec{b}\cdot \vec{a},(\vec{a} +\vec{b})\cdot \vec{c} = \vec{a}\cdot \vec{c} +\vec{b}\cdot \vec{c},(\alpha \vec{a})\cdot \vec{b} = \alpha (\vec{a}\cdot \vec{b}) = \vec{a}\cdot (\alpha \vec{b});

\vec{a}\times \vec{b} = -(\vec{b}\times \vec{a}),(\vec{a} +\vec{b})\times \vec{c} = \vec{a}\times \vec{c} +\vec{b}\times \vec{c},(\alpha \vec{a})\times \vec{b} = \alpha (\vec{a}\times \vec{b}) = \vec{a}\times (\alpha \vec{b}).

6.3.2 Application of dot and cross products in plane Trigonometry

We apply the concepts of dot and cross products of two vectors to derive a few formulae in plane trigonometry.

Example 6.1 (Cosine formulae)

With usual notations, in any triangle ABC, prove the following by vector method.

a^{2} = b^{2} + c^{2} - 2bc\cos A

c^{2} = a^{2} + b^{2} - 2ab\cos C

Solution

With usual notations in triangle ABC, we have \overline{BC} = \vec{a},\overline{CA} = \vec{b} and \overline{AB} = \vec{c}. Then |\overline{BC} | = a,|\overline{CA} | = b, |\overline{AB} | = c and \overline{BC} +\overline{CA} +\overline{AB} = \vec{0}.

\mathrm{So},\overline{BC} = -\overline{CA} -\overline{AB}.

Then applying dot product, we get

\overline{BC}\cdot \overline{BC} = (-\overline{CA} -\overline{AB})\cdot (-\overline{CA} -\overline{AB})

\Rightarrow |\overline{BC}|^{2} = |\overline{CA}|^{2} + |\overline{AB}|^{2} + 2\overline{CA}\cdot \overline{AB}

\Rightarrow a^{2} = b^{2} + c^{2} + 2bc\cos (\pi -A)

\Rightarrow a^{2} = b^{2} + c^{2} - 2bc\cos A.

The results in (ii) and (iii) are proved in a similar way.

Example 6.2

With usual notations, in any triangle ABC, prove the following by vector method.

a = b\cos C + c\cos B

c = a\cos B + b\cos A

Solution

With usual notations in triangle A B C, we have \overrightarrow{B C} = \vec{a} \overrightarrow{C A} = \vec{b}, and \overrightarrow{A B} = \vec{c}. Then

|\overrightarrow{B C}| = a, |\overrightarrow{C A}| = b, |\overrightarrow{A B}| = c \text{ and } \overrightarrow{B C} +\overrightarrow{C A} +\overrightarrow{A B} = \vec{0}

So, \overrightarrow{B C} = -\overrightarrow{C A} -\overrightarrow{A B}

Applying dot product, we get

\overrightarrow{B C}\cdot \overrightarrow{B C} = -\overrightarrow{B C}\cdot \overrightarrow{C A} -\overrightarrow{B C}\cdot \overrightarrow{A B}

\Rightarrow |\overrightarrow{B C}|^{2} = -|\overrightarrow{B C} |\overrightarrow{C A} |\cos (\pi -C) - |\overrightarrow{B C} |\overrightarrow{A B} |\cos (\pi -B)

\Rightarrow a^{2} = a b\cos C + a c\cos B

Therefore a = b\cos C + c\cos B. The results in (ii) and (iii) are proved in a similar way.

Example 6.3

By vector method, prove that \cos (\alpha +\beta) = \cos \alpha \cos \beta - \sin \alpha \sin \beta.

Solution

Let \hat{a} = \overrightarrow{O A} and \hat{b} = \overrightarrow{O B} be the unit vectors and which make angles \alpha and \beta, respectively, with positive x - axis, where A and B are as in the Fig. 6.8. Draw A L and B M perpendicular to the x - axis. Then |\overrightarrow{O L}| = |\overrightarrow{O A} |\cos \alpha = \cos \alpha, |\overrightarrow{L A}| = |\overrightarrow{O A} |\sin \alpha = \sin \alpha.

\overrightarrow{O L} = |\overrightarrow{O L} |\hat{i} = \cos \alpha \hat{i},\overrightarrow{L A} = \sin \alpha (-\hat{j}).

Therefore, \hat{a} = \overrightarrow{O A} = \overrightarrow{O L} +\overrightarrow{L A} = \cos \alpha \hat{i} - \sin \alpha \hat{j} … (1)

Similarly, \hat{b} = \cos \beta \hat{i} +\sin \beta \hat{j} … (2)

The angle between \hat{a} and \hat{b} is \alpha +\beta and so,

\hat{a}\cdot \hat{b} = |\hat{a} |\mid \hat{b} |\cos (\alpha +\beta) = \cos (\alpha +\beta) \dots (3)

On the other hand, from (1) and (2)

\hat{a}\cdot \hat{b} = (\cos \alpha \hat{i} -\sin \alpha \hat{j})\cdot (\cos \beta \hat{i} +\sin \beta \hat{j}) = \cos \alpha \cos \beta -\sin \alpha \sin \beta \dots (4)

From (3) and (4), we get \cos (\alpha +\beta) = \cos \alpha \cos \beta - \sin \alpha \sin \beta.

Example 6.4

With usual notations, in any triangle A B C, prove by vector method that \frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C}.

Solution

With usual notations in triangle A B C, we have \overrightarrow{B C} = \vec{a},\overrightarrow{C A} = \vec{b}, and \overrightarrow{A B} = \vec{c}. Then |\overrightarrow{B C}| = a, |\overrightarrow{C A}| = b and |\overrightarrow{A B}| = c.

Since in \Delta A B C, \overrightarrow{B C} +\overrightarrow{C A} +\overrightarrow{A B} = 0, we have \overrightarrow{B C}\times (\overrightarrow{B C} +\overrightarrow{C A} +\overrightarrow{A B}) = \vec{0}.

Simplification gives,

\overrightarrow{B C}\times \overrightarrow{C A} = \overrightarrow{A B}\times \overrightarrow{B C}.

Similarly, since \overrightarrow{B C} +\overrightarrow{C A} +\overrightarrow{A B} = \vec{0}, we have

\overrightarrow{C A}\times (\overrightarrow{B C} +\overrightarrow{C A} +\overrightarrow{A B}) = \vec{0}.

On Simplification, we obtain \overline{BC}\times \overline{CA} = \overline{CA}\times \overline{AB} (2) Equations (1) and (2), we get

\overline{AB}\times \overline{BC} = \overline{CA}\times \overline{AB} = \overline{BC}\times \overline{CA}.

\mathrm{So}, |\overline{AB}\times \overline{BC}| = |\overline{CA}\times \overline{AB}| = |\overline{BC}\times \overline{CA}|.

c a\sin (\pi -B) = b c\sin (\pi -A) = a b\sin (\pi -C).

That is, c a\sin B = b c\sin A = a b\sin C. Dividing by a b c, leads to

\frac{\sin A}{a} = \frac{\sin B}{b} = \frac{\sin C}{c}\quad \mathrm{or}\quad \frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C}

Example 6.5

Prove by vector method that \sin (\alpha - \beta) = \sin \alpha \cos \beta - \cos \alpha \sin \beta.

Solution

Let \hat{a} = \overline{OA} and \vec{b} = \overline{OB} be the unit vectors making angles \alpha and \beta respectively, with positive x - axis, where A and B are as shown in the Fig. 6.10. Then, we get \hat{a} = \cos \alpha \hat{i} +\sin \alpha \hat{j} and \hat{b} = \cos \beta \hat{i} +\sin \beta \hat{j}

The angle between \hat{a} and \hat{b} is \alpha - \beta and, the vectors \hat{b},\hat{a},\hat{k} form a right- handed system.

Hence, we get

\hat{b}\times \hat{a} = |\hat{b} |\mid \hat{a} |\sin (\alpha -\beta)\hat{k} = \sin (\alpha -\beta)\hat{k}.

On the other hand,

\hat{b}\times \hat{a} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\ \cos \beta & \sin \beta & 0\ \cos \alpha & \sin \alpha & 0 \end{vmatrix} = (\sin \alpha \cos \beta - \cos \alpha \sin \beta)\hat{k} \quad (2)

Hence, equations (1) and (2), leads to

\sin (\alpha -\beta) = \sin \alpha \cos \beta -\cos \alpha \sin \beta .

6.3.3 Application of dot and cross products in Geometry

Example 6.6 (Apollonius’s theorem)

If D is the midpoint of the side B C of a triangle A B C, show by vector method that \mid \overline{{A B}}\mid^{2} + \mid \overline{{A C}}\mid^{2} = 2(\mid \overline{{A D}}\mid^{2} + \mid \overline{{B D}}\mid^{2})

Solution

Let A be the origin, \vec{b} be the position vector of B and \vec{c} be the position vector of C. Now D is the midpoint of B C, and so the, position vector of D is \frac{\vec{b} + \vec{c}}{2}. Therefore, we have

\begin{array}{r}{\overline{{A D}}\big|^{2} = \overline{{A D}}\cdot \overline{{A D}} = \left(\frac{\bar{b} + \bar{c}}{2}\right)\left(\frac{\bar{b} + \bar{c}}{2}\right) = \frac{1}{4}\big(\bar{b}\big|^{2} + \big|\bar{c}\big|^{2} + 2\bar{b}\cdot \bar{c}\big).} \end{array} (1)

Now, \overline{{B D}} = \overline{{A D}} - \overline{{A B}} = \frac{\bar{b} + \bar{c}}{2} - \bar{b} = \frac{\bar{c} - \bar{b}}{2}. Then, this gives, \mid \overline{{B D}}\mid^{2} = \overline{{B D}}\cdot \overline{{B D}} = \left(\frac{\bar{c} - \bar{b}}{2}\right)\left(\frac{\bar{c} - \bar{b}}{2}\right) = \frac{1}{4}\big(\bar{b}\big|^{2} + \big|\bar{c}\big|^{2} - 2\bar{b}\cdot \bar{c}\big) (2) Now, adding (1) and (2), we get Therefore, \mid \overline{{A D}}\mid^{2} + \mid \overline{{B D}}\mid^{2} = \frac{1}{4}\big(\bar{b}\big|^{2} + \big|\bar{c}\big|^{2} + 2\bar{b}\cdot \bar{c}\big) + \frac{1}{4}\big(\bar{b}\big|^{2} + \big|\bar{c}\big|^{2} - 2\bar{b}\cdot \bar{c}\big) = \frac{1}{2}\big(\bar{b}\big|^{2} + \big|\bar{c}\big|^{2}\big)

\Rightarrow \mid \overline{{A D}}\mid^{2} + \mid \overline{{B D}}\mid^{2} = \frac{1}{2}\big(\mid \overline{{A B}}\mid^{2} + \mid \overline{{A C}}\mid^{2}\big).

Hence, \mid \overline{{A B}}\mid^{2} + \mid \overline{{A C}} \mid^{2} = 2\big(\mid \overline{{A D}}\mid^{2} + \mid \overline{{B D}}\mid^{2}\big)

Example 6.7

Prove by vector method that the perpendiculars (altitudes) from the vertices to the opposite sides of a triangle are concurrent.

Consider a triangle ABC in which the two altitudes AD and BE intersect at O. Let CO be produced to meet AB at F. We take O as the origin and let \overline{{O A}} = \bar{a},\overline{{O B}} = \bar{b} and \overline{{O C}} = \bar{c}.

Since \overline{{A D}} is perpendicular to \overline{{B C}}, we have \overline{{O A}} is perpendicular to \overline{{B C}}, and hence we get \overline{{O A}}\cdot \overline{{B C}} = 0. That is, \bar{a}\cdot (\bar{c} - \bar{b}) = 0, which means

\bar{a}\cdot \bar{c} -\bar{a}\cdot \bar{b} = 0. \quad (1)

Similarly, since \overline{{B E}} is perpendicular to \overline{{C A}}, we have \overline{{O B}} is perpendicular to \overline{{C A}}, and hence we get \overline{{O B}}\cdot \overline{{C A}} = 0. That is, \bar{b}\cdot (\bar{a} - \bar{c}) = 0, which means,

\bar{a}\cdot \bar{b} -\bar{b}\cdot \bar{c} = 0. \quad (2)

Adding equations (1) and (2), gives \bar{a}\cdot \bar{c} - \bar{b}\cdot \bar{c} = 0. That is, \bar{c}\cdot (\bar{a} - \bar{b}) = 0.

That is, \overline{{O C}}\cdot \overline{{B A}} = 0. Therefore, \overline{{B A}} is perpendicular to \overline{{O C}} which implies that \overline{{C F}} is perpendicular to \overline{{A B}}. Hence, the perpendicular drawn from C to the side AB passes through O. Thus, the altitudes are concurrent.

Example 6.8

In triangle ABC, the points D, E, F are the midpoints of the sides BC, CA, and AB respectively. Using vector method, show that the area of \Delta DEF is equal to \frac{1}{4} (area of \Delta ABC).

Solution

In triangle A B C, consider A as the origin. Then the position vectors of D,E,F are given by \frac{\overline{{A B}} + \overline{{A C}}}{2},\frac{\overline{{A C}}}{2},\frac{\overline{{A B}}}{2} respectively. Since |\overline{{A B}}\times \overline{{A C}} | is the area of the parallelogram formed by the two vectors \overline{{A B}} \overline{{A C}} as adjacent sides, the area of \Delta A B C is \frac{1}{2} |\overline{{A B}}\times \overline{{A C}} |. Similarly, considering \Delta D E F, we have the area of \Delta D E F = \frac{1}{2} |\overline{{D E}}\times \overline{{D F}} |

= \frac{1}{2} \left| \left( \frac{\overline{AC}}{2} - \frac{\overline{AB}}{2} \right) \times \left( \frac{\overline{AB}}{2} - \frac{\overline{AB}+\overline{AC}}{2} \right) \right|

=\frac{1}{2}\left| \left( \frac{\overline{AC} - \overline{AB}}{2} \right) \times \left( \frac{-\overline{AC}}{2} \right) \right|

=\frac{1}{2}\left| \frac{1}{4} (\overline{AB} - \overline{AC}) \times \overline{AC} \right|

=\frac{1}{8} |\overline{AB} \times \overline{AC}|

=\frac{1}{4}\left(\frac{1}{2}|\overline{{A B}}\times\overline{{A C}}|\right)

=\frac{1}{4}\left(\mathrm{theareaof~}\Delta A B C\right).

6.3.4 Application of dot and cross product in Physics

Definition 6.2

If \vec{d} is the displacement vector of a particle moved from a point to another point after applying a constant force \vec{F} on the particle, then the work done by the force on the particle is w = \vec{F}\cdot \vec{d}.

If the force has an acute angle, perpendicular angle, and an obtuse angle, the work done by the force is positive, zero, and negative respectively.

Example 6.9

A particle acted upon by constant forces 2\hat{i} +5\hat{j} +6\hat{k} and - \hat{i} - 2\hat{j} - \hat{k} is displaced from the point (4, - 3, - 2) to the point (6,1, - 3). Find the total work done by the forces.

Solution

Resultant of the given forces is \vec{F} = (2\hat{i} +5\hat{j} +6\hat{k}) + (- \hat{i} - 2\hat{j} - \hat{k}) = \hat{i} +3\hat{j} +5\hat{k}.

Let A and B be the points (4, - 3, - 2) and (6,1, - 3) respectively. Then the displacement vector of the particle is \vec{d} = \overline{{A B}} = \overline{{O B}} -\overline{{O A}} = (6\hat{i} +\hat{j} - 3\hat{k}) - (4\hat{i} - 3\hat{j} - 2\hat{k}) = 2\hat{i} +4\hat{j} - \hat{k}.

Therefore the work done w = \vec{F}\cdot \vec{d} = (\hat{i} +3\hat{j} +5\hat{k})\cdot (2\hat{i} +4\hat{j} - \hat{k}) = 9 units.

Example 6.10

A particle is acted upon by the forces 3\hat{i} - 2\hat{j} +2\hat{k} and 2\hat{i} +\hat{j} -\hat{k} is displaced from the point (1,3, - 1) to the point (4, - 1,\lambda). If the work done by the forces is 16 units, find the value of \lambda.

Solution

The resultant force is \vec{F} = (3\hat{i} -2\hat{j} +2\hat{k}) + (2\hat{i} +\hat{j} -\hat{k}) = 5\hat{i} -\hat{j} +\hat{k}.

The displacement of the particle is given by

\vec{d} = (4\hat{i} -\hat{j} +\lambda \hat{k}) - (\hat{i} +3\hat{j} -\hat{k}) = (3\hat{i} -4\hat{j} +(\lambda +1)\hat{k}).

As the work done by the forces is 16 units, we have

\vec{F}\cdot \vec{d} = 16.

That is, (5\hat{i} -\hat{j} +\hat{k})\cdot (3\hat{i} -4\hat{j} +(\lambda +1)\hat{k}) = 16 \Rightarrow \lambda +20 = 16.

So, \lambda = - 4

Definition 6.3

If a force \vec{F} is applied on a particle at a point with position vector \vec{r}, then the torque or moment on the particle is given by \vec{t} = \vec{r}\times \vec{F}. The torque is also called the rotational force.

Example 6.11

Find the magnitude and the direction cosines of the torque about the point (2,0, - 1) of a force 2\hat{i} +\hat{j} -\hat{k}, whose line of action passes through the origin.

Solution

Let \mathcal{A} be the point (2,0, - 1). Then the position vector of \mathcal{A} is \overrightarrow{OA} = 2\hat{i} -\hat{k} and therefore \vec{r} = \overrightarrow{AO} = - 2\hat{i} +\hat{k}

Then the given force is \vec{F} = 2\hat{i} +\hat{j} -\hat{k}. So, the torque is

\vec{t} = \vec{r} \times \vec{F} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ -2 & 0 & 1 \ 2 & 1 & -1 \end{vmatrix} = (0 \cdot (-1) - 1 \cdot 1)\hat{i} - ((-2)(-1) - 1 \cdot 2)\hat{j} + ((-2)\cdot 1 - 0 \cdot 2)\hat{k} = -\hat{i} - 0\hat{j} - 2\hat{k}.

The magnitude of the torque = | - \hat{i} - 2\hat{k} | = \sqrt{5} and the direction cosines of the torque are -\frac{1}{\sqrt{5}},0, - \frac{2}{\sqrt{5}}.

EXERCISE 6.1

1. Prove by vector method that if a line is drawn from the centre of a circle to the midpoint of a chord, then the line is perpendicular to the chord.
2. Prove by vector method that the median to the base of an isosceles triangle is perpendicular to the base.
3. Prove by vector method that an angle in a semi-circle is a right angle.
4. Prove by vector method that the diagonals of a rhombus bisect each other at right angles.
5. Using vector method, prove that if the diagonals of a parallelogram are equal, then it is a rectangle.
6. Prove by vector method that the area of the quadrilateral ABCD having diagonals AC and BD is \frac{1}{2} |\overrightarrow{AC} \times \overrightarrow{BD}|.
7. Prove by vector method that the parallelograms on the same base and between the same parallels are equal in area.
8. If G is the centroid of a \Delta ABC, prove that (area of \Delta GAB) = (area of \Delta GBC) = (area of \Delta GCA) = \frac{1}{3} (area of \Delta ABC).
9. Using vector method, prove that \cos (\alpha - \beta) = \cos \alpha \cos \beta + \sin \alpha \sin \beta.
10. Prove by vector method that \sin (\alpha + \beta) = \sin \alpha \cos \beta + \cos \alpha \sin \beta,
11. A particle acted on by constant forces 8\hat{i} + 2\hat{j} - 6\hat{k} and 6\hat{i} + 2\hat{j} - 2\hat{k} is displaced from the point (1,2,3) to the point (5,4,1). Find the total work done by the forces.
12. Forces of magnitudes 5\sqrt{2} and 10\sqrt{2} units acting in the directions 3\hat{i} + 4\hat{j} + 5\hat{k} and 10\hat{i} + 6\hat{j} - 8\hat{k}, respectively, act on a particle which is displaced from the point with position vector 4\hat{i} - 3\hat{j} - 2\hat{k} to the point with position vector 6\hat{i} + \hat{j} - 3\hat{k}. Find the work done by the forces.
13. Find the magnitude and direction cosines of the torque of a force represented by 3\hat{i} + 4\hat{j} - 5\hat{k} about the point with position vector 2\hat{i} - 3\hat{j} + 4\hat{k} acting through a point whose position vector is 4\hat{i} + 2\hat{j} - 3\hat{k}.
14. Find the torque of the resultant of the three forces represented by -3\hat{i} + 6\hat{j} - 3\hat{k}, 4\hat{i} - 10\hat{j} + 12\hat{k} and 4\hat{i} + 7\hat{j} acting at the point with position vector 8\hat{i} - 6\hat{j} - 4\hat{k}, about the point with position vector 18\hat{i} + 3\hat{j} - 9\hat{k}.

6.4 Scalar triple product

Definition 6.4

For a given set of three vectors \vec{a}, \vec{b}, and \vec{c}, the scalar (\vec{a} \times \vec{b}) \cdot \vec{c} is called a scalar triple product of \vec{a}, \vec{b}, \vec{c}.

Remark

\vec{a} \cdot \vec{b} is a scalar and so (\vec{a} \cdot \vec{b}) \times \vec{c} has no meaning.

Theorem 6.2

For any three vectors \vec{a},\vec{b},\vec{c},

(\vec{a}\times\vec{b})\cdot\vec{c} = \vec{a}\cdot(\vec{b}\times\vec{c})

Proof

Let \vec{a} = a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k}, \vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k} and \vec{c} = c*{1}\hat{i} +c*{2}\hat{j} +c_{3}\hat{k}.

Then, \vec{a}\times\vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix} and so (\vec{a}\times\vec{b})\cdot\vec{c} = \begin{vmatrix} c_1 & c_2 & c_3 \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix}.

Similarly, \vec{b}\times\vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ b_1 & b_2 & b_3 \ c_1 & c_2 & c_3 \end{vmatrix} and so \vec{a}\cdot(\vec{b}\times\vec{c}) = \begin{vmatrix} a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \ c_1 & c_2 & c_3 \end{vmatrix}.

Since the determinant changes sign when two rows are interchanged, we have

\begin{vmatrix} c_1 & c_2 & c_3 \ a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \end{vmatrix} = \begin{vmatrix} a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \ c_1 & c_2 & c_3 \end{vmatrix}.

Hence the theorem is proved.

Note

By Theorem 6.2, it follows that, in a scalar triple product, dot and cross can be interchanged without altering the order of occurrences of the vectors, by placing the parentheses in such a way that dot lies outside the parentheses, and cross lies between the vectors inside the parentheses. For instance, we have

(\vec{a}\times \vec{b})\cdot \vec{c} = \vec{a}\cdot (\vec{b}\times \vec{c}),\mathrm{sincedotandcrosscanbe~interchanged.}

\qquad = (\vec{b}\times \vec{c})\cdot \vec{a},\mathrm{sincedotproductis~commutative.}

\qquad = \vec{b}\cdot (\vec{c}\times \vec{a}),\mathrm{sincedotandcrosscanbe~interchanged}

\qquad = (\vec{c}\times \vec{a})\cdot \vec{b},\mathrm{sincedotproductis~commutative}

\qquad = \vec{c}\cdot (\vec{a}\times \vec{b}),\mathrm{sincedotandcrosscanbe~interchanged}

Notation

For any three vectors \vec{a},\vec{b} and \vec{c}, the scalar triple product (\vec{a}\times \vec{b})\cdot \vec{c} is denoted by [\vec{a},\vec{b},\vec{c} ].

[\vec{a},\vec{b},\vec{c} ] is read as box \vec{a},\vec{b},\vec{c}. For this reason and also because the absolute value of a scalar triple product represents the volume of a box (rectangular parallelepiped),a scalar triple product is also called a box product.

Note

[\vec{a},\vec{b},\vec{c}] = (\vec{a}\times \vec{b})\cdot \vec{c} = \vec{a}\cdot (\vec{b}\times \vec{c}) = (\vec{b}\times \vec{c})\cdot \vec{a} = \vec{b}\cdot (\vec{c}\times \vec{a}) = [\vec{b},\vec{c},\vec{a}]

[\vec{b},\vec{c},\vec{a}] = (\vec{b}\times \vec{c})\cdot \vec{a} = \vec{b}\cdot (\vec{c}\times \vec{a}) = (\vec{c}\times \vec{a})\cdot \vec{b} = \vec{c}\cdot (\vec{a}\times \vec{b}) = [\vec{c},\vec{a},\vec{b} ].

In other words, [\vec{a},\vec{b},\vec{c} ] = [\vec{b},\vec{c},\vec{a} ] = [\vec{c},\vec{a},\vec{b} ]; that is, if the three vectors are permuted in the same cyclic order, the value of the scalar triple product remains the same.

(2) If any two vectors are interchanged in their position in a scalar triple product, then the value of the scalar triple product is (-1) times the original value. More explicitly,

[\vec{a},\vec{b},\vec{c}] = [\vec{b},\vec{c},\vec{a}] = [\vec{c},\vec{a},\vec{b}] = -[\vec{a},\vec{c},\vec{b}] = -[\vec{c},\vec{b},\vec{a}] = -[\vec{b},\vec{a},\vec{c} ]

Theorem 6.5

The scalar triple product [\vec{a},\vec{b},\vec{c}] = 0 if and only if \vec{a},\vec{b},\vec{c} are coplanar.

Proof

Let \vec{a} = a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k} \vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k} \vec{c} = c*{1}\hat{i} +c*{2}\hat{j} +c_{3}\hat{k}. Then, we have

[\vec{a},\vec{b},\vec{c}] = \begin{vmatrix} a_1 & a_2 & a_3 \ b_1 & b_2 & b_3 \ c_1 & c_2 & c_3 \end{vmatrix} = 0

\Leftrightarrow there exist scalars r,s,t\in \mathbb{R} atleast one of them non- zero such that

a*{1}r + a*{2}s + a*{3}t = 0,\quad b*{1}r + b*{2}s + b*{3}t = 0,\quad c*{1}r + c*{2}s + c_{3}t = 0

\Leftrightarrow there exist scalars r,s,t\in \mathbb{R} atleast one of them non- zero such that r\vec{a} +s\vec{b} +t\vec{c} = \vec{0}

Theorem 6.6

If \vec{a},\vec{b},\vec{c} and \overrightarrow{p},\overrightarrow{q},\overrightarrow{r} are any two systems of three vectors, and if \overrightarrow{p} = x*{1}\overrightarrow{a} +y*{1}\overrightarrow{b} +z*{1}\overrightarrow{c} \vec{q} = x*{2}\vec{a} +y*{2}\vec{b} +z*{2}\vec{c}, and, \vec{r} = x*{3}\vec{a} +y*{3}\vec{b} +z_{3}\vec{c}, then

[\vec{p},\vec{q},\vec{r}] = \begin{vmatrix} x_1 & y_1 & z_1 \ x_2 & y_2 & z_2 \ x_3 & y_3 & z_3 \end{vmatrix} [\vec{a},\vec{b},\vec{c}]

Note

By theorem 6.6, if \vec{a},\vec{b},\vec{c} are non- coplanar and

\begin{vmatrix} x_1 & y_1 & z_1 \ x_2 & y_2 & z_2 \ x_3 & y_3 & z_3 \end{vmatrix} \neq 0

then the three vectors \overrightarrow{p} = x*{1}\overrightarrow{a} +y*{1}\overrightarrow{b} +z*{1}\overrightarrow{c} \vec{q} = x*{2}\vec{a} +y*{2}\vec{b} +z*{2}\vec{c}, and, \vec{r} = x*{3}\vec{a} +y*{3}\vec{b} +z_{3}\vec{c} are also non- coplanar.

Example 6.12

\vec{a} = -3\hat{i} -\hat{j} +5\hat{k},\vec{b} = \hat{i} -2\hat{j} +\hat{k},\vec{c} = 4\hat{j} -5\hat{k},\mathrm{find}\vec{a}\cdot (\vec{b}\times \vec{c}).

Solution: By the definition of scalar triple product of three vectors,

\vec{a}\cdot(\vec{b}\times\vec{c}) = \begin{vmatrix} -3 & -1 & 5 \ 1 & -2 & 1 \ 0 & 4 & -5 \end{vmatrix} = -3(10-4) + 1(-5-0) + 5(4-0) = -18 -5 +20 = -3.

Example 6.13

Find the volume of the parallelepiped whose coterminus edges are given by the vectors 2\hat{i} - 3\hat{j} +4\hat{k},\hat{i} +2\hat{j} - \hat{k} and 3\hat{i} - \hat{j} +2\hat{k}.

Solution

We know that the volume of the parallelepiped whose coterminus edges are \vec{a},\vec{b},\vec{c} is given by \left|\left[\vec{a},\vec{b},\vec{c}\right]\right|. Here, \vec{a} = 2\hat{i} - 3\hat{j} +4\hat{k} \vec{b} = \hat{i} +2\hat{j} - \hat{k} \vec{c} = 3\hat{i} - \hat{j} +2\hat{k}.

[\vec{a},\vec{b},\vec{c}] = \begin{vmatrix} 2 & -3 & 4 \ 1 & 2 & -1 \ 3 & -1 & 2 \end{vmatrix} = 2(4-1) + 3(2+3) + 4(-1-6) = 6 + 15 - 28 = -7.

Hence the volume is |;[\vec{a},\vec{b},\vec{c}];| = 7 cubic units.

Example 6.14

Show that the vectors \hat{i} +2\hat{j} - 3\hat{k} 2\hat{i} - \hat{j} +2\hat{k} and 3\hat{i} +\hat{j} - \hat{k} are coplanar.

Solution

\begin{vmatrix} 1 & 2 & -3 \ 2 & -1 & 2 \ 3 & 1 & -1 \end{vmatrix} = 1(1-2) - 2(-2-6) - 3(2+3) = -1 + 16 - 15 = 0.

Therefore, the three given vectors are coplanar.

Example 6.15

If 2\hat{i} - \hat{j} +3\hat{k} 3\hat{i} +2\hat{j} +\hat{k} \hat{i} +m\hat{j} +4\hat{k} are coplanar, find the value of m

Solution

Since the given three vectors are coplanar, we have \left| \begin{array}{lll}2 & - 1 & 3\ 3 & 2 & 1\ 1 & m & 4 \end{array} \right| = 0\Rightarrow m = - 3.

Example 6.16

Show that the four points (6, - 7,0) (16, - 19, - 4) (0,3, - 6) (2, - 5,10) lie on a same plane.

Solution

Let A = (6, - 7,0) B = (16, - 19, - 4) C = (0,3, - 6) D = (2, - 5,10). To show that the four points A,B,C,D lie on a plane, we have to prove that the three vectors \overrightarrow{AB},\overrightarrow{AC},\overrightarrow{AD} are coplanar.

\overline{{A B}} = \overline{{O B}} -\overline{{O A}} = (16\hat{i} -19\hat{j} -4\hat{k}) - (6\hat{i} -7\hat{j}) = 10\hat{i} -12\hat{j} -4\hat{k}

\overline{{A C}} = \overline{{O C}} -\overline{{O A}} = -6\hat{i} +10\hat{j} -6\hat{k}\mathrm{and}\overline{{A D}} = \overline{{O D}} -\overline{{O A}} = -4\hat{i} +2\hat{j} +10\hat{k}.

[\overline{{A B}},\overline{{A C}},\overline{{A D}}] = \begin{vmatrix} 10 & -12 & -4 \ -6 & 10 & -6 \ -4 & 2 & 10 \end{vmatrix} = 0.

Therefore, the three vectors \overrightarrow{AB},\overrightarrow{AC},\overrightarrow{AD} are coplanar and hence the four points A,B,C, and D lie on a plane.

EXERCISE 6.2

1. If \vec{a} = 2\hat{i} + 3\hat{j} - \hat{k}, \vec{b} = 3\hat{i} + 5\hat{j} + 2\hat{k}, \vec{c} = -\hat{i} - 2\hat{j} + 3\hat{k}, verify that (\vec{a}\times\vec{b})\times\vec{c} = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{b}\cdot\vec{c})\vec{a} and \vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c}.

2. If \vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}, \vec{b} = 2\hat{i} - \hat{j} + \hat{k}, \vec{c} = 3\hat{i} + 2\hat{j} + \hat{k} and \vec{a}\times(\vec{b}\times\vec{c}) = l\vec{a} + m\vec{b} + n\vec{c}, find the values of l, m, n.

3. For any vector \vec{a}, prove that \hat{i}\times(\vec{a}\times\hat{i}) + \hat{j}\times(\vec{a}\times\hat{j}) + \hat{k}\times(\vec{a}\times\hat{k}) = 2\vec{a}.

4. Prove that [\vec{a} - \vec{b}, \vec{b} - \vec{c}, \vec{c} - \vec{a}] = 0.

5. If \vec{a} = 2\hat{i} + 3\hat{j} - \hat{k}, \vec{b} = -\hat{i} + 2\hat{j} - 4\hat{k}, \vec{c} = \hat{i} + \hat{j} + \hat{k}, then find the value of (\vec{a}\times\vec{b})\cdot(\vec{a}\times\vec{c}).

6. If \vec{a}, \vec{b}, \vec{c}, \vec{d} are coplanar vectors, show that (\vec{a}\times\vec{b})\times(\vec{c}\times\vec{d}) = \vec{0}.

7. If \hat{a}, \hat{b}, \hat{c} are three unit vectors such that \hat{b} and \hat{c} are non-parallel and \hat{a}\times(\hat{b}\times\hat{c}) = \frac{1}{2}\hat{b}, find the angle between \hat{a} and \hat{c}.

6.5 Vector triple product

Definition 6.5

For a given set of three vectors \vec{a},\vec{b},\vec{c}, the vector \vec{a}\times(\vec{b}\times\vec{c}) is called a vector triple product.

Theorem 6.8

For any three vectors \vec{a},\vec{b},\vec{c},

\vec{a}\times(\vec{b}\times\vec{c}) = (\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c}

Proof (for a special case)

Let \vec{a} = a_1\hat{i}, \vec{b} = b_1\hat{i} + b_2\hat{j}, \vec{c} = c_1\hat{i} + c_2\hat{j} + c_3\hat{k}.

Then, \vec{b}\times\vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ b_1 & b_2 & 0 \ c_1 & c_2 & c_3 \end{vmatrix} = b_2 c_3 \hat{i} - b_1 c_3 \hat{j} + (b_1 c_2 - b_2 c_1)\hat{k}.

Now, \vec{a}\times(\vec{b}\times\vec{c}) = a_1\hat{i} \times [b_2 c_3 \hat{i} - b_1 c_3 \hat{j} + (b_1 c_2 - b_2 c_1)\hat{k}] = -a_1 b_1 c_3 \hat{k} + a_1(b_1 c_2 - b_2 c_1)\hat{j} …(1)

And, (\vec{a}\cdot\vec{c})\vec{b} - (\vec{a}\cdot\vec{b})\vec{c} = a_1 c_1 (b_1\hat{i} + b_2\hat{j}) - a_1 b_1 (c_1\hat{i} + c_2\hat{j} + c_3\hat{k}) = a_1(b_1 c_2 - b_2 c_1)\hat{j} - a_1 b_1 c_1 \hat{k} …(2)

From equations (1) and (2), we get

\vec{a}\times (\vec{b}\times \vec{c}) = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{a}\cdot \vec{b})\vec{c}

Note

(1) \vec{a}\times (\vec{b}\times \vec{c}) = \alpha \vec{b} +\beta \vec{c}, where \alpha = \vec{a}\cdot \vec{c} and \beta = -(\vec{a}\cdot \vec{b}), and so it lies in the plane parallel to \vec{b} and \vec{c}.

(2) We also note that

(\vec{a}\times \vec{b})\times \vec{c} = -\vec{c}\times (\vec{a}\times \vec{b}) = -{(\vec{c}\cdot \vec{b})\vec{a} -(\vec{c}\cdot \vec{a})\vec{b}} = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{b}\cdot \vec{c})\vec{a}

Therefore, (\vec{a}\times \vec{b})\times \vec{c} lies in the plane parallel to \vec{a} and \vec{b}.

(3) In (\vec{a}\times \vec{b})\times \vec{c}, consider the vectors inside the brackets, call \vec{b} as the middle vector and \vec{a} as the non-middle vector. Similarly, in \vec{a}\times (\vec{b}\times \vec{c}), \vec{b} is the middle vector and \vec{c} is the non-middle vector. Then we observe that a vector triple product of these vectors is equal to \lambda (middle vector) -\mu (non-middle vector) where \lambda is the dot product of the vectors other than the middle vector and \mu is the dot product of the vectors other than the non- middle vector.

6.6 Jacobi’s Identity and Lagrange’s Identity

Theorem 6.9 (Jacobi’s identity)

For any three vectors \vec{a},\vec{b},\vec{c}, we have \vec{a}\times (\vec{b}\times \vec{c}) + \vec{b}\times (\vec{c}\times \vec{a}) + \vec{c}\times (\vec{a}\times \vec{b}) = \vec{0}.

Proof

Using vector triple product expansion, we have

\vec{a}\times (\vec{b}\times \vec{c}) = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{a}\cdot \vec{b})\vec{c}

\vec{b}\times (\vec{c}\times \vec{a}) = (\vec{b}\cdot \vec{a})\vec{c} -(\vec{b}\cdot \vec{c})\vec{a}

\vec{c}\times (\vec{a}\times \vec{b}) = (\vec{c}\cdot \vec{b})\vec{a} -(\vec{c}\cdot \vec{a})\vec{b}

Adding these three equations, we get the required identity.

Theorem 6.10 (Lagrange’s identity)

For any three vectors \vec{a},\vec{b},\vec{c},

(\vec{a}\times\vec{b})\cdot(\vec{c}\times\vec{d}) = (\vec{a}\cdot\vec{c})(\vec{b}\cdot\vec{d}) - (\vec{a}\cdot\vec{d})(\vec{b}\cdot\vec{c})

Proof is left as an exercise.

Example 6.17

If \vec{a} = 2\hat{i} + \hat{j} - \hat{k}, \vec{b} = 4\hat{i} + 4\hat{j}, \vec{c} = 2\hat{i} + 5\hat{j} + \hat{k} and \vec{d} = 3\hat{j} - \hat{k}, verify that (\vec{a}\times\vec{b})\times(\vec{c}\times\vec{d}) = [\vec{a},\vec{b},\vec{d}]\vec{c} - [\vec{a},\vec{b},\vec{c}]\vec{d}.

Solution

\vec{a}\times\vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2 & 1 & -1 \ 4 & 4 & 0 \end{vmatrix} = 4\hat{i} - 4\hat{j} + 4\hat{k}

\vec{c}\times\vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2 & 5 & 1 \ 0 & 3 & -1 \end{vmatrix} = -8\hat{i} + 2\hat{j} + 6\hat{k}

Then,

(\vec{a}\times\vec{b})\times(\vec{c}\times\vec{d}) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 4 & -4 & 4 \ -8 & 2 & 6 \end{vmatrix} = -24\hat{i} - 24\hat{j} - 40\hat{k} \quad (1)

On the other hand, we have

[\vec{a},\vec{b},\vec{d}] = \begin{vmatrix} 2 & 1 & -1 \ 4 & 4 & 0 \ 0 & 3 & -1 \end{vmatrix} = 28, \quad [\vec{a},\vec{b},\vec{c}] = \begin{vmatrix} 2 & 1 & -1 \ 4 & 4 & 0 \ 2 & 5 & 1 \end{vmatrix} = 12

[\vec{a},\vec{b},\vec{d}]\vec{c} - [\vec{a},\vec{b},\vec{c}]\vec{d} = 28(2\hat{i} + 5\hat{j} + \hat{k}) - 12(3\hat{j} - \hat{k}) = -24\hat{i} + 24\hat{j} - 40\hat{k} \quad (2)

Therefore, from equations (1) and (2), the identity is verified.

EXERCISE 6.3

1. If \vec{a} = \hat{i} -2\hat{j} +3\hat{k} \vec{b} = 2\hat{i} +\hat{j} -2\hat{k} \vec{c} = 3\hat{i} +2\hat{j} +\hat{k} find (i) (\vec{a}\times \vec{b})\times \vec{c} (ii) \vec{a}\times (\vec{b}\times \vec{c})
2. For any vector \vec{a}, prove that \hat{i}\times (\vec{a}\times \hat{i}) + \hat{j}\times (\vec{a}\times \hat{j}) + \hat{k}\times (\vec{a}\times \hat{k}) = 2\vec{a}
3. Prove that [\vec{a} -\vec{b},\vec{b} -\vec{c},\vec{c} -\vec{a}] = 0
4. If \vec{a} = 2\hat{i} +3\hat{j} -\hat{k} \vec{b} = 3\hat{i} +5\hat{j} +2\hat{k} \vec{c} = -\hat{i} -2\hat{j} +3\hat{k}, verify that

(\vec{a}\times \vec{b})\times \vec{c} = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{b}\cdot \vec{c})\vec{a} \qquad (\vec{a}\times (\vec{b}\times \vec{c}) = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{a}\cdot \vec{b})\vec{c}

5. \vec{a} = 2\hat{i} +3\hat{j} -\hat{k} \vec{b} = -\hat{i} +2\hat{j} -4\hat{k} \vec{c} = \hat{i} +\hat{j} +\hat{k} then find the value of (\vec{a}\times \vec{b})\cdot (\vec{a}\times \vec{c})
6. If \vec{a},\vec{b},\vec{c},\vec{d} are coplanar vectors, show that (\vec{a}\times \vec{b})\times (\vec{c}\times \vec{d}) = \vec{0}
7. If \vec{a} = \hat{i} +2\hat{j} +3\hat{k} \vec{b} = 2\hat{i} -\hat{j} +\hat{k} \vec{c} = 3\hat{i} +2\hat{j} +\hat{k} and \vec{a}\times (\vec{b}\times \vec{c}) = l\vec{a} +m\vec{b} +n\vec{c}, find the values of l,m,n
8. If \hat{a},\hat{b},\hat{c} are three unit vectors such that \hat{b} and \hat{c} are non- parallel and \hat{a}\times (\hat{b}\times \hat{c}) = \frac{1}{2}\hat{b}, find the angle between \hat{a} and \hat{c}.

6.7 Application of Vectors to 3-Dimensional Geometry

Vectors provide an elegant approach to study straight lines and planes in three dimension. All straight lines and planes are subsets of \mathbb{R}^{3}. For brevity, we shall call a straight line simply as line. A plane is a surface which is understood as a set P of points in \mathbb{R}^{3} such that, if A,B, and C are any three non- collinear points of P, then the line passing through any two of them is a subset of P. Two planes are said to be intersecting if they have at least one point in common and at least one point which lies on one plane but not on the other. Two planes are said to be coincident if they have exactly the same points. Two planes are said to be parallel but not coincident if they have no point in common. Similarly, a straight line can be understood as the set of points common to two intersecting planes. In this section, we obtain vector and Cartesian equations of straight line and plane by applying vector methods. By a vector form of equation of a geometrical object, we mean an equation which is satisfied by the position vector of every point of the object. The equation may be a vector equation or a scalar equation.

XII - Mathematics

6.7.1 Different forms of equation of a straight line

A straight line can be uniquely fixed if

• a point on the straight line and the direction of the straight line are given
• two points on the straight line are given

We find equations of a straight line in vector and Cartesian form. To find the equation of a straight line in vector form, an arbitrary point P with position vector \vec{r} on the straight line is taken and a relation satisfied by \vec{r} is obtained by using the given conditions. This relation is called the vector equation of the straight line. A vector equation of a straight line may or may not involve parameters. If a vector equation involves parameters, then it is called a vector equation in parametric form. If no parameter is involved, then the equation is called a vector equation in non- parametric form.

6.7.2 A point on the straight line and the direction of the straight line are given

(a) Parametric form of vector equation

Theorem 6.11

The vector equation of a straight line passing through a fixed point with position vector \vec{a} and parallel to a given vector \vec{b} is \vec{r} = \vec{a} +t\vec{b}, where t\in \mathbb{R}.

Proof

If \vec{a} is the position vector of a given point A and \vec{r} is the position vector of an arbitrary point P on the straight line, then

\overrightarrow{AP} = \vec{r} -\vec{a}.

Since \overrightarrow{AP} is parallel to \vec{b}, we have

\vec{r} -\vec{a} = t\vec{b},t\in \mathbb{R}

\vec{r} = \vec{a} +t\vec{b},t\in \mathbb{R}

This is the vector equation of the straight line in parametric form.

Remark

The position vector of any point on the line is taken as \vec{a} +t\vec{b}.

(b) Non-parametric form of vector equation

Since \overrightarrow{AP} is parallel to \vec{b}, we have \overrightarrow{AP}\times \vec{b} = \vec{0}

That is, (\vec{r} -\vec{a})\times \vec{b} = \vec{0}.

This is known as the vector equation of the straight line in non- parametric form.

(c) Cartesian equation

Suppose P is (x,y,z) A is (x*{1},y*{1},z*{1}) and \vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k}. Then, substituting \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} \vec{a} = x*{1}\hat{i} +y*{1}\hat{j} +z_{1}\hat{k} in (1) and comparing the coefficients of \hat{i},\hat{j},\hat{k}, we get

x - x*{1} = tb*{1},y - y*{1} = tb*{2},z - z*{1} = tb*{3} \quad (4)

Conventionally (4) can be written as

\frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} \quad (5)

which are called the Cartesian equations or symmetric equations of a straight line passing through the point (x*{1},y*{1},z*{1}) and parallel to a vector with direction ratios b*{1},b*{2},b*{3}.

Remark

(i) Every point on the line (5) is of the form (x*{1} + t b*{1},y*{1} + t b*{2},z*{1} + t b*{3}), where t\in \mathbb{R}.

(ii) Since the direction cosines of a line are proportional to direction ratios of the line, if l,m,n are the direction cosines of the line, then the Cartesian equations of the line are

\frac{x - x*{1}}{l} = \frac{y - y*{1}}{m} = \frac{z - z_{1}}{n}.

(iii) In (5), if any one or two of b*{1},b*{2},b*{3} are zero, it does not mean that we are dividing by zero. But it means that the corresponding numerator is zero. For instance, If b*{1}\neq 0,b*{2}\neq 0 and b*{3} = 0, then

\frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z_{1}}{0}

(iv) We know that the direction cosines of x - axis are 1,0,0. Therefore, the equations of x - axis are

\frac{x - 0}{1} = \frac{y - 0}{0} = \frac{z - 0}{0} \text{or} x = t,y = 0,z = 0, \text{where} t\in \mathbb{R}.

Similarly the equations of y - axis and z - axis are given by \frac{x - 0}{0} = \frac{y - 0}{1} = \frac{z - 0}{0} and \frac{x - 0}{0} = \frac{y - 0}{0} = \frac{z - 0}{1} respectively.

6.7.3 Straight Line passing through two given points

(a) Parametric form of vector equation

Theorem 6.12

The parametric form of vector equation of a line passing through two given points whose position vectors are \vec{a} and \vec{b} respectively is \vec{r} = \vec{a} +t(\vec{b} -\vec{a}),t\in \mathbb{R}.

(b) Non-parametric form of vector equation

The above equation can be written equivalently in non- parametric form of vector equation as

(\vec{r} -\vec{a})\times (\vec{b} -\vec{a}) = \vec{0}

(c) Cartesian form of equation

Suppose P is (x,y,z), A is (x*{1},y*{1},z*{1}) and B is (x*{2},y*{2},z*{2}). Then substituting \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}, \vec{a} = x*{1}\hat{i} +y*{1}\hat{j} +z*{1}\hat{k} and \vec{b} = x*{2}\hat{i} +y*{2}\hat{j} +z*{2}\hat{k} in theorem 6.12 and comparing the coefficients of \hat{i},\hat{j},\hat{k}, we get x - x*{1} = t(x*{2} - x*{1}),y - y*{1} = t(y*{2} - y*{1}),z - z*{1} = t(z*{2} - z*{1}) and so the Cartesian equations of a line passing through two given points (x*{1},y*{1},z*{1}) and (x*{2},y*{2},z_{2}) are given by

\frac{x - x*{1}}{x*{2} - x*{1}} = \frac{y - y*{1}}{y*{2} - y*{1}} = \frac{z - z*{1}}{z*{2} - z_{1}}

Example 6.26

Find the vector equation in parametric form and Cartesian equations of the line passing through (- 4,2, - 3) and is parallel to the line \frac{- x - 2}{4} = \frac{y + 3}{- 2} = \frac{2z - 6}{3}.

Solution

Rewriting the given equations as \frac{x + 2}{- 4} = \frac{y + 3}{- 2} = \frac{z - 3}{3 / 2} and comparing with \frac{x - x_1}{b_1} = \frac{y - y_1}{b_2} = \frac{z - z_1}{b_3}, we have \vec{b} = b_1\vec{i} +b_2\vec{j} +b_3\vec{k} = - 4\vec{i} - 2\vec{j} +\frac{3}{2}\vec{k} = -\frac{1}{2} (8\vec{i} +4\vec{j} -3\vec{k}). Clearly, \vec{b} is parallel to the vector 8\vec{i} +4\vec{j} -3\vec{k}. Therefore, a vector equation of the required straight line passing through the given point (- 4,2, - 3) and parallel to the vector 8\vec{i} +4\vec{j} -3\vec{k} in parametric form is

\vec{r} = (-4\vec{i} +2\vec{j} -3\vec{k}) + t(8\vec{i} +4\vec{j} -3\vec{k}),t\in \mathbb{R}.

Therefore, Cartesian equations of the required straight line are given by

\frac{x + 4}{8} = \frac{y - 2}{4} = \frac{z + 3}{-3}.

Example 6.27

Find the vector equation in parametric form and Cartesian equations of a straight passing through the points (- 5,7, - 4) and (13, - 5,2). Find the point where the straight line crosses the xy - plane.

Solution

The straight line passes through the points (- 5,7, - 4) and (13, - 5,2), and therefore, direction ratios of the straight line joining these two points are 18, - 12, 6. That is, 3, - 2, 1.

So, the straight line is parallel to 3\vec{i} - 2\vec{j} +\vec{k}. Therefore,

Required vector equation of the straight line in parametric form is \vec{r} = (- 5\vec{i} +7\vec{j} -4\vec{k}) + t(3\vec{i} -2\vec{j} +\vec{k}) or \vec{r} = (13\vec{i} -5\vec{j} +2\vec{k}) + s(3\vec{i} -2\vec{j} +\vec{k}) where s,t\in \mathbb{R}

Required cartesian equations of the straight line are \frac{x + 5}{3} = \frac{y - 7}{- 2} = \frac{z + 4}{1} or \frac{x - 13}{3} = \frac{y + 5}{- 2} = \frac{z - 2}{1}.

An arbitrary point on the straight line is of the form

(3t - 5, - 2t + 7,t - 4)\mathrm{or}(3s + 13, - 2s - 5,s + 2)

Since the straight line crosses the xy - plane, the z - coordinate of the point of intersection is zero. Therefore, we have t - 4 = 0, that is, t = 4, and hence the straight line crosses the xy - plane at (7, - 1,0).

Example 6.28

Find the angle made by the straight line \frac{x + 3}{2} = \frac{y - 1}{2} = - z with coordinate axes.

Solution

If \hat{b} is a unit vector parallel to the given line, then \hat{b} = \frac{2\vec{i} + 2\vec{j} - \vec{k}}{|\vec{2}\vec{i} + 2\vec{j} - \vec{k}|} = \frac{1}{3} (2\vec{i} +2\vec{j} - \vec{k}). Therefore, from the definition of direction cosines of \hat{b}, we have the direction cosines as \frac{2}{3}, \frac{2}{3}, -\frac{1}{3}.

Hence, the angles made by the line with the coordinate axes are \cos^{-1}(\frac{2}{3}), \cos^{-1}(\frac{2}{3}), \cos^{-1}(-\frac{1}{3}).

6.7.4 Angle between two straight lines

(a) Vector form

The acute angle between two given straight lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} is same as that of the angle between \vec{b} and \vec{d}. So, \cos \theta = \frac{|\vec{b}\cdot\vec{d}|}{|\vec{b}||\vec{d}|} or \theta = \cos^{- 1}\left(\frac{|\vec{b}\cdot\vec{d}|}{|\vec{b}||\vec{d}|}\right).

Remark

(i) The two given lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are parallel

\Leftrightarrow \theta = 0\Leftrightarrow \cos \theta = 1\Leftrightarrow |\vec{b}\cdot \vec{d}| = |\vec{b} | |\vec{d} |.

(ii) The two given lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are parallel if, and only if \vec{b} = \lambda \vec{d}, for some scalar \lambda.

(iii) The two given lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are perpendicular if, and only if \vec{b}\cdot \vec{d} = 0.

(b) Cartesian form

If two lines are given in Cartesian form as \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}}, then the acute angle \theta between the two given lines is given by

\theta = \cos^{-1}\left(\frac{|b*{1}d*{1} + b*{2}d*{2} + b*{3}d*{3}|}{\sqrt{b*{1}^{2} + b*{2}^{2} + b*{3}^{2}}\sqrt{d*{1}^{2} + d*{2}^{2} + d*{3}^{2}}}\right)

Remark

(i) The two given lines with direction ratios b*{1},b*{2},b*{3} and d*{1},d*{2},d*{3} are parallel if, and only if

\frac{b*{1}}{d*{1}} = \frac{b*{2}}{d*{2}} = \frac{b*{3}}{d*{3}}.

(ii) The two given lines with direction ratios b*{1},b*{2},b*{3} and d*{1},d*{2},d*{3} are perpendicular if and only if b*{1}d*{1} + b*{2}d*{2} + b*{3}d*{3} = 0.

(iii) If the direction cosines of two given straight lines are l*{1},m*{1},n*{1} and l*{2},m*{2},n*{2}, then the angle between the two given straight lines is \cos \theta = |l*{1}l*{2} + m*{1}m*{2} + n*{1}n*{2}|.

Example 6.29

Find the acute angle between the lines \vec{r} = (\hat{i} +2\hat{j} +4\hat{k}) + t(2\hat{i} +2\hat{j} +\hat{k}) and the straight line passing through the points (5,1,4) and (9,2,12).

Solution

We know that the line \vec{r} = (\hat{i} +2\hat{j} +4\hat{k}) + t(2\hat{i} +2\hat{j} +\hat{k}) is parallel to the vector 2\hat{i} +2\hat{j} +\hat{k}.

Direction ratios of the straight line joining the two given points (5,1,4) and (9,2,12) are 4,1,8 and hence this line is parallel to the vector 4\hat{i} +\hat{j} +8\hat{k}.

Therefore, the acute angle between the given two straight lines is

\theta = \cos^{-1}\left(\frac{|\vec{b}\cdot\vec{d}|}{|\vec{b}||\vec{d}|}\right),\mathrm{where~}\vec{b} = 2\hat{i} +2\hat{j} +\hat{k}\mathrm{and}\vec{d} = 4\hat{i} +\hat{j} +8\hat{k}.

\theta = \cos^{-1}\left(\frac{|(2\hat{i} +2\hat{j} +\hat{k})\cdot(4\hat{i} +\hat{j} +8\hat{k})|}{|2\hat{i} +2\hat{j} +\hat{k}||4\hat{i} +\hat{j} +8\hat{k}|}\right) = \cos^{-1}\left(\frac{2}{3}\right).

Example 6.30

Find the acute angle between the straight lines \frac{x - 4}{2} = \frac{y}{1} = \frac{z + 1}{- 2} and \frac{x - 1}{4} = \frac{y + 1}{- 4} = \frac{z - 2}{2} and state whether they are parallel or perpendicular.

Solution

Comparing the given lines with the general Cartesian equations of straight lines,

\frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}}\mathrm{and}\frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}}

we find (b*{1},b*{2},b*{3}) = (2,1, - 2) and (d*{1},d*{2},d*{3}) = (4, - 4,2). Therefore, the acute angle between the two straight lines is

\theta = \cos^{-1}\left(\frac{|(2)(4) + (1)(-4) + (-2)(2)|}{\sqrt{2^{2} + 1^{2} + (-2)^{2}}\sqrt{4^{2} + (-4)^{2} + 2^{2}}}\right) = \cos^{-1}(0) = \frac{\pi}{2}

Thus the two straight lines are perpendicular.

Example 6.31

Show that the straight line passing through the points A(6,7,5) and B(8,10,6) is perpendicular to the straight line passing through the points C(10,2, - 5) and D(8,3, - 4).

Solution

The straight line passing through the points A(6,7,5) and B(8,10,6) is parallel to the vector \vec{b} = \overrightarrow{A B} = \overrightarrow{O B} - \overrightarrow{O A} = 2\hat{i} +3\hat{j} +\hat{k} and the straight line passing through the points C(10,2, - 5) and D(8,3, - 4) is parallel to the vector \vec{d} = \overrightarrow{C D} = - 2\hat{i} +\hat{j} +\hat{k}. Therefore, the angle between the two straight lines is the angle between the two vectors \vec{b} and \vec{d}. Since

\vec{b}\cdot \vec{d} = (2\hat{i} +3\hat{j} +\hat{k})\cdot (-2\hat{i} +\hat{j} +\hat{k}) = 0.

the two vectors are perpendicular, and hence the two straight lines are perpendicular.

Aliter

We find that direction ratios of the straight line joining the points A(6,7,5) and B(8,10,6) are (b*{1},b*{2},b*{3}) = (2,3,1) and direction ratios of the line joining the points C(10,2, - 5) and D(8,3, - 4) are (d*{1},d*{2},d*{3}) = (- 2,1,1). Since b*{1}d*{1} + b*{2}d*{2} + b*{3}d*{3} = (2)(- 2) + (3)(1) + (1)(1) = 0, the two straight lines are perpendicular.

Example 6.32

Show that the lines \frac{x - 1}{4} = \frac{2 - y}{6} = \frac{z - 4}{12} and \frac{x - 3}{- 2} = \frac{y - 3}{3} = \frac{5 - z}{6} are parallel.

Solution

We observe that the straight line \frac{x - 1}{4} = \frac{2 - y}{6} = \frac{z - 4}{12} is parallel to the vector 4\hat{i} - 6\hat{j} +12\hat{k} and the straight line \frac{x - 3}{- 2} = \frac{y - 3}{3} = \frac{5 - z}{6} is parallel to the vector - 2\hat{i} +3\hat{j} - 6\hat{k}.

Since 4\hat{i} - 6\hat{j} +12\hat{k} = - 2(- 2\hat{i} +3\hat{j} - 6\hat{k}), the two vectors are parallel, and hence the two straight lines are parallel.

EXERCISE 6.4

1. Find the non-parametric form of vector equation and Cartesian equations of the straight line passing through the point with position vector 4\hat{i} +3\hat{j} -7\hat{k} and parallel to the vector 2\hat{i} -6\hat{j} +7\hat{k}.

2. Find the parametric form of vector equation and Cartesian equations of the straight line passing through the point (-2,3,4) and parallel to the straight line \frac{x - 1}{-4} = \frac{y + 3}{5} = \frac{8 - z}{6}.

3. Find the points where the straight line passes through (6,7,4) and (8,4,9) cuts the xz and yz planes.

4. Find the direction cosines of the straight line passing through the points (5,6,7) and (7,9,13). Also, find the parametric form of vector equation and Cartesian equations of the straight line passing through two given points.

5. Find the acute angle between the following lines. (i) \vec{r}=(4\hat{i}-\hat{j})+t(\hat{i}+2\hat{j}-2\hat{k}),\vec{r}=(\hat{i}-2\hat{j}+4\hat{k})+s(-\hat{i}-2\hat{j}+2\hat{k}) (ii) \frac{x+4}{3}=\frac{y-7}{4}=\frac{z+5}{5},\vec{r}=4\hat{k}+t(2\hat{i}+\hat{j}+\hat{k}).

6. The vertices of \Delta ABC are A(7,2,1),B(6,0,3), and C(4,2,4). Find \angle ABC.

7. If the straight line joining the points (2,1,4) and (a - 1,4, - 1) is parallel to the line joining the points (0,2,b - 1) and (5,3, - 2), find the values of a and b.

8. If the straight lines \frac{x - 5}{5m + 2} = \frac{2 - y}{5} = \frac{1 - z}{-1} and x = \frac{2y + 1}{4m} = \frac{1 - z}{-3} are perpendicular to each other, find the value of m.

9. Show that the points (2,3,4),(-1,4,5) and (8,1,2) are collinear.

6.7.5 Point of intersection of two straight lines

If \frac{x - x*{1}}{a*{1}} = \frac{y - y*{1}}{a*{2}} = \frac{z - z*{1}}{a*{3}} and \frac{x - x*{2}}{b*{1}} = \frac{y - y*{2}}{b*{2}} = \frac{z - z*{2}}{b*{3}} are two lines, then every point on the line is of the form (x*{1} + sa*{1},y*{1} + sa*{2},z*{1} + sa*{3}) and (x*{2} + tb*{1},y*{2} + tb*{2},z*{2} + tb*{3}) respectively. If the lines are intersecting, then there must be a common point. So, at the point of intersection, for some values of s and t, we have

(x*{1} + sa*{1},y*{1} + sa*{2},z*{1} + sa*{3}) = (x*{2} + tb*{1},y*{2} + tb*{2},z*{2} + tb*{3})

\qquad \mathrm{Therefore,}x*{1} + sa*{1} = x*{2} + tb*{1},y*{1} + sa*{2} = y*{2} + tb*{2},z*{1} + sa*{3} = z*{2} + tb*{3}

By solving any two of the above three equations, we obtain the values of s and t. If s and t satisfy the remaining equation, the lines are intersecting lines. Otherwise the lines are non- intersecting. Substituting the value of s, (or by substituting the value of t), we get the point of intersection of two lines.

If the equations of straight lines are given in vector form, write them in cartesian form and proceed as above to find the point of intersection.

Example 6.33

Find the point of intersection of the lines \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} and \frac{x - 4}{5} = \frac{y - 1}{2} = z.

Solution

Every point on the line \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} = s (say) is of the form (2s + 1,3s + 2,4s + 3) and every point on the line \frac{x - 4}{5} = \frac{y - 1}{2} = z = t (say) is of the form (5t + 4,2t + 1,t). So, at the point of intersection, for some values of s and t, we have

(2s + 1,3s + 2,4s + 3) = (5t + 4,2t + 1,t)

Therefore, 2s - 5t = 3, 3s - 2t = - 1 and 4s - t = - 3. Solving the first two equations we get t = - 1, s = - 1. These values of s and t satisfy the third equation. Therefore, the given lines intersect. Substituting, these values of t or s in the respective points, the point of intersection is (- 1, - 1, - 1).

6.7.6 Shortest distance between two straight lines

We have just explained how the point of intersection of two lines are found and we have also studied how to determine whether the given two lines are parallel or not.

Definition 6.6

Two lines are said to be coplanar if they lie in the same plane.

Note

If two lines are either parallel or intersecting, then they are coplanar.

Definition 6.7

Two lines in space are called skew lines if they are not parallel and do not intersect

Note

If two lines are skew lines, then they are non coplanar.

If the lines are not parallel and intersect, the distance between them is zero. If they are parallel and non- intersecting, the distance is determined by the length of the line segment perpendicular to both the parallel lines. In the same way, the shortest distance between two skew lines is defined as the length of the line segment perpendicular to both the skew lines. Two lines will either be parallel or skew.

Theorem 6.13

The shortest distance between the two parallel lines \vec{r} = \vec{a} + s\vec{b} and \vec{r} = \vec{c} + t\vec{b} is given by d = \frac{|(\vec{c} - \vec{a})\times\vec{b}|}{|\vec{b}|}, where |\vec{b}|\neq 0.

Proof

The given two parallel lines \vec{r} = \vec{a} + s\vec{b} and \vec{r} = \vec{c} + t\vec{b} are denoted by L*{1} and L*{2} respectively. Let A and B be the points on L*{1} and L*{2} whose position vectors are \vec{a} and \vec{c} respectively. The two given lines are parallel to \vec{b}.

Let AD be a perpendicular to the two given lines. If \theta is the acute angle between \overline{AB} and \vec{b}, then

\sin \theta = \frac{|\overline{AB}\times\vec{b}|}{|\overline{AB}||\vec{b}|} = \frac{|(\vec{c} - \vec{a})\times\vec{b}|}{|\vec{c} - \vec{a}||\vec{b}|}

But, from the right angle triangle ABD

\sin \theta = \frac{d}{AB} = \frac{d}{|\overline{AB}||\vec{b}|} = \frac{d}{|\vec{c} - \vec{a}|}

From (1) and (2), we have d = \frac{|(\vec{c} - \vec{a})\times\vec{b}|}{|\vec{b}|}, where |\vec{b}|\neq 0.

Theorem 6.14

The shortest distance between the two skew lines \vec{r} = \vec{a} + s\vec{b} and \vec{r} = \vec{c} + t\vec{d} is given by

\delta = \frac{|(\vec{c} - \vec{a})\cdot(\vec{b}\times\vec{d})|}{|\vec{b}\times\vec{d}|},\mathrm{where}|\vec{b}\times\vec{d}|\neq 0

Proof

The two skew lines \vec{r} = \vec{a} + s\vec{b} and \vec{r} = \vec{c} + t\vec{d} are denoted by L*{1} and L*{2} respectively.

Let A and C be the points on L*{1} and L*{2} with position vectors \vec{a} and \vec{c} respectively.

From the given equations of skew lines, we observe that L*{1} is parallel to the vector \vec{b} and L*{2} is parallel to the vector \vec{d}. So, \vec{b} \times \vec{d} is perpendicular to the lines L*{1} and L*{2}.

Let SD be the line segment perpendicular to both the lines L*{1} and L*{2}. Then the vector \overline{SD} is perpendicular to the vectors \vec{b} and \vec{d} and therefore it is parallel to the vector \vec{b} \times \vec{d}.

So, \frac{\vec{b} \times \vec{d}}{|\vec{b} \times \vec{d}|} is a unit vector in the direction of \overline{SD}. Then, the shortest distance |\overline{SD}| is the absolute value of the projection of \overline{AC} on \overline{SD}. That is,

\begin{array}{l}{\delta = |\overline{{S D}} | = |\overline{{A C}} .(\mathrm{Unitvectorinthedirectionof}\overline{{S D}} )| = \left|(\vec{c} -\vec{a})\cdot \frac{\vec{b}\times\vec{d}}{|\vec{b}\times\vec{d}|}\right|}\ {\delta = \frac{|(\vec{c} -\vec{a})\cdot(\vec{b}\times\vec{d})|}{|\vec{b}\times\vec{d}|},\mathrm{where~}|\vec{b}\times\vec{d}|\neq 0.} \end{array} \quad (1)

Remark

(i) It follows from theorem (6.14) that two straight lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} intersect each other (that is, coplanar) if (\vec{c} -\vec{a})\cdot (\vec{b}\times \vec{d}) = 0.

(2) If two lines \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} intersect each other (that is, coplanar), then we have

\begin{vmatrix} x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

Example 6.34

Find the parametric form of vector equation of a straight line passing through the point of intersection of the straight lines \vec{r} = (\hat{i} +3\hat{j} -\hat{k}) + t(2\hat{i} +3\hat{j} +2\hat{k}) and \frac{x - 2}{1} = \frac{y - 4}{2} = \frac{z + 3}{4}, and perpendicular to both straight lines.

Solution

The Cartesian equations of the straight line \vec{r} = (\hat{i} +3\hat{j} -\hat{k}) + t(2\hat{i} +3\hat{j} +2\hat{k}) is

\frac{x - 1}{2} = \frac{y - 3}{3} = \frac{z + 1}{2} = s \mathrm{(say)}

Then any point on this line is of the form (2s + 1, 3s + 3, 2s - 1) … (1)

The Cartesian equation of the second line is \frac{x - 2}{1} = \frac{y - 4}{2} = \frac{z + 3}{4} = t (say)

Then any point on this line is of the form (t + 2, 2t + 4, 4t - 3) … (2)

If the given lines intersect, then there must be a common point. Therefore, for some s,t\in \mathbb{R} we have (2s + 1,3s + 3,2s - 1) = (t + 2,2t + 4,4t - 3).

Equating the coordinates of x,y and z we get

2s - t = 1,3s - 2t = 1\mathrm{and}s - 2t = -1.

Solving the first two of the above three equations, we get s = 1 and t = 1. These values of s and t satisfy the third equation. So, the lines are intersecting.

Now, using the value of s in (1) or the value of t in (2), the point of intersection (3,6,1) of these two straight lines is obtained.

If we take \vec{b} = 2\hat{i} +3\hat{j} +2\hat{k} and \vec{d} = \hat{i} +2\hat{j} +4\hat{k}, then \vec{b}\times \vec{d} = \left| \begin{array}{lll}\hat{i} & \hat{j} & \hat{k}\ 2 & 3 & 2\ 1 & 2 & 4 \end{array} \right| = 8\hat{i} - 6\hat{j} +\hat{k} is a vector perpendicular to both the given straight lines. Therefore, the required straight line passing through (3,6,1) and perpendicular to both the given straight lines is the same as the straight line passing through (3,6,1) and parallel to 8\hat{i} - 6\hat{j} +\hat{k}. Thus, the equation of the required straight line is

\vec{r} = (3\hat{i} +6\hat{j} +\hat{k}) + m(8\hat{i} -6\hat{j} +\hat{k}),m\in \mathbb{R}.

Example 6.35

Determine whether the pair of straight lines \vec{r} = (2\hat{i} +6\hat{j} +3\hat{k}) + t(2\hat{i} +3\hat{j} +4\hat{k}) \vec{r} = (2\hat{j} - 3\hat{k}) + s(\hat{i} +2\hat{j} +3\hat{k}) are parallel. Find the shortest distance between them.

Solution

Comparing the given two equations with

\vec{r} = \vec{a} +s\vec{b}\mathrm{and}\vec{r} = \vec{c} +s\vec{d},

\vec{a} = 2\hat{i} +6\hat{j} +3\hat{k},\vec{b} = 2\hat{i} +3\hat{j} +4\hat{k},\vec{c} = 2\hat{j} -3\hat{k},\vec{d} = \hat{i} +2\hat{j} +3\hat{k}

Clearly, \vec{b} is not a scalar multiple of \vec{d}. So, the two vectors are not parallel and hence the two lines are not parallel.

The shortest distance between the two straight lines is given by

\delta = \frac{|(\vec{c} - \vec{a})\cdot(\vec{b}\times \vec{d})|}{|\vec{b}\times \vec{d}|}

Now, \vec{c} - \vec{a} = -2\hat{i} -4\hat{j} -6\hat{k} and \vec{b}\times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2 & 3 & 4 \ 1 & 2 & 3 \end{vmatrix} = \hat{i} - 2\hat{j} + \hat{k}.

\mathrm{So},\quad (\vec{c} -\vec{a})\cdot (\vec{b}\times \vec{d}) = (-2\hat{i} -4\hat{j} -6\hat{k})\cdot (\hat{i} -2\hat{j} +\hat{k}) = 0.

Therefore, the distance between the two given straight lines is zero. Thus, the given lines intersect each other.

Example 6.36

Find the shortest distance between the two given straight lines \vec{r} = (2\vec{i} +3\vec{j} +4\vec{k}) + t(- 2\vec{i} +\vec{j} - 2\vec{k}) and \frac{x - 3}{2} = \frac{y}{- 1} = \frac{z + 2}{2}.

Solution

The parametric form of vector equations of the given straight lines are

\vec{r} = (2\vec{i} +3\vec{j} +4\vec{k}) + t(-2\vec{i} +\vec{j} -2\vec{k})

\mathrm{and}\quad \vec{r} = (3\vec{i} -2\vec{k}) + t(2\vec{i} -\vec{j} +2\vec{k})

Comparing the given two equations with \vec{r} = \vec{a} +t\vec{b} \vec{r} = \vec{c} +s\vec{d}

we have \vec{a} = 2\vec{i} +3\vec{j} +4\vec{k} \vec{b} = - 2\vec{i} +\vec{j} - 2\vec{k} \vec{c} = 3\vec{i} - 2\vec{k} \vec{d} = 2\vec{i} -\vec{j} +2\vec{k}

Clearly, \vec{b} is a scalar multiple of \vec{d}, and hence the two straight lines are parallel. We know that the shortest distance between two parallel straight lines is given by d = \frac{|(\vec{c} - \vec{a})\times\vec{b}|}{|\vec{b}|}.

(\vec{c} - \vec{a})\times\vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 1 & -3 & -6 \ -2 & 1 & -2 \end{vmatrix} = 12\hat{i} + 14\hat{j} - 5\hat{k}

\mathrm{Therefore}, d = \frac{|12\hat{i} + 14\hat{j} - 5\hat{k}|}{|-2\hat{i} + \hat{j} - 2\hat{k}|} = \frac{\sqrt{365}}{3}.

Example 6.37

Find the coordinate of the foot of the perpendicular drawn from the point (- 1,2,3) to the straight line \vec{r} = (\vec{i} - 4\vec{j} +3\vec{k}) + t(2\vec{i} +3\vec{j} +\vec{k}). Also, find the shortest distance from the given point to the straight line.

Solution

Comparing the given equation \vec{r} = (\vec{i} - 4\vec{j} +3\vec{k}) + t(2\vec{i} +3\vec{j} +\vec{k}) with \vec{r} = \vec{a} +t\vec{b}, we get \vec{a} = \vec{i} - 4\vec{j} +3\vec{k}, and \vec{b} = 2\vec{i} +3\vec{j} +\vec{k}. We denote the given point (- 1,2,3) by D, and the point (1, - 4,3) on the straight line by F. If F is the foot of the perpendicular from D to the straight line, then F is of the form (2t + 1,3t - 4,t + 3) and \overline{DF} = \overline{OF} - \overline{OD} = (2t + 2)\hat{i} +(3t - 6)\hat{j} +t\hat{k}.

Since \vec{b} is perpendicular to \overline{DF}, we have

\vec{b}\cdot \overline{DF} = 0\Rightarrow 2(2t + 2) + 3(3t - 6) + 1(t) = 0\Rightarrow t = 1

Therefore, the coordinate of F is (3, - 1,4)

Now, the perpendicular distance from the given point to the given line is

DF = |\overline{DF}| = \sqrt{4^{2} + (-3)^{2} + 1^{2}} = \sqrt{26}\mathrm{~units}.

EXERCISE 6.5

1. Find the parametric form of vector equation and Cartesian equations of a straight line passing through (5,2,8) and is perpendicular to the straight lines \vec{r} = (\hat{i} +\hat{j} -\hat{k}) + s(2\hat{i} -2\hat{j} +\hat{k}) and \vec{r} = (2\hat{i} -\hat{j} -3\hat{k}) + t(\hat{i} +2\hat{j} +2\hat{k}).

2. Show that the lines \vec{r} = (6\hat{i} +\hat{j} +2\hat{k}) + s(\hat{i} +2\hat{j} -3\hat{k}) and \vec{r} = (3\hat{i} +2\hat{j} -2\hat{k}) + t(2\hat{i} +4\hat{j} -5\hat{k}) are skew lines and hence find the shortest distance between them.

3. If the two lines \frac{x - 1}{2} = \frac{y + 1}{3} = \frac{z - 1}{4} and \frac{x - 3}{1} = \frac{y - m}{2} = z intersect at a point, find the value of m.

4. Show that the lines \frac{x - 3}{3} = \frac{y - 3}{-1},z - 1 = 0 and \frac{x - 6}{2} = \frac{z - 1}{3},y - 2 = 0 intersect. Also find the point of intersection.

5. Show that the straight lines x + 1 = 2y = -12z and x = y + 2 = 6z - 6 are skew and hence find the shortest distance between them.

6. Find the parametric form of vector equation of the straight line passing through (-1,2,1) and parallel to the straight line \vec{r} = (2\hat{i} +3\hat{j} -\hat{k}) + t(\hat{i} -2\hat{j} +\hat{k}) and hence find the shortest distance between the lines.

7. Find the foot of the perpendicular drawn from the point (5,4,2) to the line \frac{x + 1}{2} = \frac{y - 3}{3} = \frac{z - 1}{- 1}. Also, find the equation of the perpendicular.

6.8 Different forms of Equation of a plane

We have already seen the notion of a plane.

Definition 6.8

A vector which is perpendicular to a plane is called a normal to the plane.

Note

Every normal to a plane is perpendicular to every straight line lying on the plane.

A plane is uniquely fixed if any one of the following is given:

• a unit normal to the plane and the distance of the plane from the origin
• a point of the plane and a normal to the plane
• three non- collinear points of the plane
• a point of the plane and two non- parallel lines or non- parallel vectors which are parallel to the plane
• two distinct points of the plane and a straight line or non- zero vector parallel to the plane but not parallel to the line joining the two points.

Let us find the vector and Cartesian equations of planes using the above situations.

6.8.1 Equation of a plane when a normal to the plane and the distance of the plane from the origin are given

(a) Vector equation of a plane in normal form

Theorem 6.15

The equation of the plane at a distance p from the origin and perpendicular to the unit normal vector \hat{d} is \vec{r}\cdot \hat{d} = p

Consider a plane whose perpendicular distance from the origin is p.

Let A be the foot of the perpendicular from O to the plane.

Let \hat{d} be the unit normal vector in the direction of \overline{OA}.

Then \overline{OA} = p\hat{d}.

If \vec{r} is the position vector of an arbitrary point P on the plane,

then \overline{AP} is perpendicular to \overline{OA}.

\overline{AP}\cdot \overline{OA} = 0\Rightarrow (\vec{r} -p\hat{d})\cdot p\hat{d} = 0

\Rightarrow (\vec{r} -p\hat{d})\cdot \hat{d} = 0

\vec{r}\cdot \hat{d} = p.

The above equation is called the vector equation of the plane in normal form.

(b) Cartesian equation of a plane in normal form

Let l,m,n be the direction cosines of \hat{d}. Then we have \hat{d} = l\hat{i} +m\hat{j} +n\hat{k}.

Thus, equation (1) becomes

\vec{r}\cdot (l\hat{i} +m\hat{j} +n\hat{k}) = p

If P is (x,y,z), then \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}

Therefore, (x\hat{i} +y\hat{j} +z\hat{k})\cdot (l\hat{i} +m\hat{j} +n\hat{k}) = p or lx + my + nz = p

Equation (2) is called the Cartesian equation of the plane in normal form.

Remark

(i) If the plane passes through the origin, then p = 0. So, the equation of the plane is

lx + my + nz = 0.

(ii) If \vec{d} is normal vector to the plane, then \hat{d} = \frac{\vec{d}}{|\vec{d}|} is a unit normal to the plane. So, the vector equation of the plane is \vec{r}\cdot \frac{\vec{d}}{|\vec{d}|} = p or \vec{r}\cdot \vec{d} = q, where q = p|\vec{d} |. The equation \vec{r}\cdot \vec{d} = q is the vector equation of a plane in standard form.

Note

In the standard form \vec{r}\cdot \vec{d} = q, \vec{d} need not be a unit normal and q need not be the perpendicular distance.

6.8.2 Equation of a plane perpendicular to a vector and passing through a given point

(a) Vector form of equation

Consider a plane passing through a point A with position vector \vec{a} and \vec{n} is a normal vector to the given plane.

Let \vec{r} be the position vector of an arbitrary point P on the plane.

Then \overline{AP} is perpendicular to \vec{n}.

\overline{AP}\cdot \vec{n} = 0 \quad (1)

which is the vector form of the equation of a plane passing through a point with position vector \vec{a} and perpendicular to \vec{n}.

Note

(\vec{r} -\vec{a})\cdot \vec{n} = 0\Rightarrow \vec{r}\cdot \vec{n} = \vec{a}\cdot \vec{n}\Rightarrow \vec{r}\cdot \vec{n} = q,\mathrm{where}q = \vec{a}\cdot \vec{n}.

(b) Cartesian form of equation

If a,b,c are the direction ratios of \vec{n}, then we have \vec{n} = a\vec{i} +b\vec{j} +c\vec{k}. Suppose, A is (x*{1},y*{1},z*{1}) then equation (1) becomes \left((x - x*{1})\hat{i} +(y - y*{1})\hat{j} +(z - z*{1})\hat{k}\right)\cdot (a\vec{i} +b\vec{j} +c\vec{k}) = 0. That is,

a(x - x*{1}) + b(y - y*{1}) + c(z - z_{1}) = 0

which is the Cartesian equation of a plane, normal to a vector with direction ratios a,b,c and passing through a given point (x*{1},y*{1},z_{1}).

6.8.3 Intercept form of the equation of a plane

Let the plane \vec{r}\cdot \vec{n} = q meets the coordinate axes at A,B,C respectively such that the intercepts on the axes are OA = a OB = b OC = c. Now position vector of the point A is a\vec{i} Since A lies on the given plane, we have a\vec{i}\cdot \vec{n} = q which gives \hat{i}\cdot \vec{n} = \frac{q}{a} Similarly, since the vectors b\hat{j} and c\hat{k} lie on the given plane, we have \hat{j}\cdot \vec{n} = \frac{q}{b} and \hat{k}\cdot \vec{n} = \frac{q}{c}. Substituting \vec{r} = x\vec{i} +y\vec{j} +z\vec{k} in \vec{r}\cdot \vec{n} = q, we get x\vec{i}\cdot \vec{n} +y\vec{j}\cdot \vec{n} +z\vec{k}\cdot \vec{n} = q. So x\left(\frac{q}{a}\right) + y\left(\frac{q}{b}\right) + z\left(\frac{q}{c}\right) = q.

Dividing by q, we get, \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1. This is called the intercept form of equation of the plane having intercepts a,b,c on the x,y,z axes respectively.

Theorem 6.16

The general equation ax + by + cz + d = 0 of first degree in x,y,z represents a plane.

Proof

The equation ax + by + cz + d = 0 can be written in the vector form as follows

(x\vec{i} +y\vec{j} +z\vec{k})\cdot (a\vec{i} +b\vec{j} +c\vec{k}) = -d\quad \mathrm{or}\quad \vec{r}\cdot \vec{n} = -d.

Since this is the vector form of the equation of a plane in standard form, the given equation ax + by + cz + d = 0 represents a plane. Here \vec{n} = a\vec{i} +b\vec{j} +c\vec{k} is a vector normal to the plane.

Note

In the general equation ax + by + cz + d = 0 of a plane, a,b,c are direction ratios of the normal to the plane.

Example 6.38

Find the vector and Cartesian form of the equations of a plane which is at a distance of 12 units from the origin and perpendicular to 6\hat{i} +2\hat{j} - 3\hat{k}.

Solution

Let \vec{d} = 6\hat{i} +2\hat{j} - 3\hat{k} and p = 12.

If \hat{d} is the unit normal vector in the direction of the vector 6\hat{i} +2\hat{j} - 3\hat{k}

\mathrm{then} \hat{d} = \frac{\vec{d}}{|\vec{d}|} = \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}).

If \vec{r} is the position vector of an arbitrary point (x,y,z) on the plane, then using \vec{r}\cdot \hat{d} = p, the vector equation of the plane in normal form is \vec{r}\cdot \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}) = 12.

Substituting \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} in the above equation, we get (x\hat{i} +y\hat{j} +z\hat{k})\cdot \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}) = 12 Applying dot product in the above equation and simplifying, we get 6x + 2y - 3z = 84, which is the Cartesian equation of the required plane.

Example 6.39

If the Cartesian equation of a plane is 3x - 4y + 3z = - 8, find the vector equation of the plane in the standard form.

Solution

If \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} is the position vector of an arbitrary point (x,y,z) on the plane, then the given equation can be written as (x\hat{i} +y\hat{j} +z\hat{k})\cdot (3\hat{i} - 4\hat{j} +3\hat{k}) = - 8 or (x\hat{i} +y\hat{j} +z\hat{k})\cdot (- 3\hat{i} +4\hat{j} - 3\hat{k}) = 8. That is, \vec{r}\cdot (- 3\hat{i} +4\hat{j} - 3\hat{k}) = \mathbf{8} which is the vector equation of the given plane in standard form.

Example 6.40

Find the direction cosines of the normal to the plane and length of the perpendicular from the origin to the plane \vec{r}\cdot (3\hat{i} - 4\hat{j} +12\hat{k}) = 5.

Solution

Let \vec{d} = 3\hat{i} - 4\hat{j} +12\hat{k} and q = 5.

If \hat{d} is the unit vector in the direction of the vector 3\hat{i} - 4\hat{j} +12\hat{k}, then \hat{d} = \frac{1}{13} (3\hat{i} - 4\hat{j} +12\hat{k}).

Now, dividing the given equation by 13, we get

\vec{r}\cdot \left(\frac{3}{13}\hat{i} -\frac{4}{13}\hat{j} +\frac{12}{13}\hat{k}\right) = \frac{5}{13}

which is the equation of the plane in the normal form \vec{r}\cdot \hat{d} = p.

From this equation, we infer that \hat{d} = \frac{1}{13} (3\hat{i} - 4\hat{j} +12\hat{k}) is a unit vector normal to the plane from the origin. Therefore, the direction cosines of \hat{d} are \frac{3}{13},\frac{- 4}{13},\frac{12}{13} and the length of the perpendicular from the origin to the plane is \frac{5}{13}.

Example 6.41

Find the vector and Cartesian equations of the plane passing through the point with position vector 4\hat{i} +2\hat{j} -3\hat{k} and normal to vector 2\hat{i} - \hat{j} +\hat{k}.

Solution

If the position vector of the given point is \vec{a} = 4\hat{i} +2\hat{j} - 3\hat{k} and \vec{n} = 2\hat{i} - \hat{j} +\hat{k}, then the equation of the plane passing through a point and normal to a vector is given by (\vec{r} -\vec{a})\cdot \vec{n} = 0 or \vec{r}\cdot \vec{n} = \vec{a}\cdot \vec{n}.

Substituting \vec{a} = 4\hat{i} +2\hat{j} - 3\hat{k} and \vec{n} = 2\hat{i} - \hat{j} +\hat{k} in the above equation, we get

\vec{r}\cdot (2\hat{i} -\hat{j} +\hat{k}) = (4\hat{i} +2\hat{j} -3\hat{k})\cdot (2\hat{i} -\hat{j} +\hat{k})

Thus, the required vector equation of the plane is \vec{r}\cdot (2\hat{i} -\hat{j} +\hat{k}) = 3. If \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} then we get the Cartesian equation of the plane 2x - y + z = 3.

Example 6.42

A variable plane moves in such a way that the sum of the reciprocals of its intercepts on the coordinate axes is a constant. Show that the plane passes through a fixed point

Solution

The equation of the plane having intercepts a,b,c on the x,y,z axes respectively is \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1. Since the sum of the reciprocals of the intercepts on the coordinate axes is a constant, we have \frac{1}{a} +\frac{1}{b} +\frac{1}{c} = k, where k is a constant, and which can be written as \frac{1}{a}\left(\frac{1}{k}\right) + \frac{1}{b}\left(\frac{1}{k}\right) + \frac{1}{c}\left(\frac{1}{k}\right) = 1. This shows that the plane \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1 passes through the fixed point \left(\frac{1}{k},\frac{1}{k},\frac{1}{k}\right).

EXERCISE 6.6

1. Find the vector equation of a plane which is at a distance of 7 units from the origin having 3, -4,5 as direction ratios of a normal to it.

2. Find the direction cosines of the normal to the plane 12x + 3y - 4z = 65. Also, find the non-parametric form of vector equation of a plane and the length of the perpendicular to the plane from the origin.

3. Find the vector and Cartesian equations of the plane passing through the point with position vector 2\hat{i} +6\hat{j} +3\hat{k} and normal to the vector \hat{i} +3\hat{j} +5\hat{k}.

4. A plane passes through the point (-1,1,2) and the normal to the plane of magnitude 3\sqrt{3} makes equal acute angles with the coordinate axes. Find the equation of the plane.

5. Find the intercepts cut off by the plane \vec{r}\cdot (6\hat{i} +4\hat{j} -3\hat{k}) = 12 on the coordinate axes.

6. If a plane meets the coordinate axes at A,B,C such that the centroid of the triangle ABC is the point (u,v,w), find the equation of the plane.

6.8.4 Equation of a plane passing through three given non- collinear points

(a) Parametric form of vector equation

Theorem 6.17

If three non- collinear points with position vectors \vec{a},\vec{b},\vec{c} are given, then the vector equation of the plane passing through the given points in parametric form is

\vec{r} = \vec{a} +s(\vec{b} -\vec{a}) + t(\vec{c} -\vec{a}),\mathrm{where}\vec{b}\neq \vec{0},\vec{c}\neq \vec{0}\mathrm{and}s,t\in \mathbb{R}.

Proof

Consider a plane passing through three non- collinear points A,B,C with position vectors \vec{a},\vec{b},\vec{c} respectively. Then atleast two of them are non- zero vectors. Let us take \vec{b}\neq \vec{0} and \vec{c}\neq \vec{0}. Let \vec{r} be the position vector of an arbitrary point P on the plane. Take a point D on AB (produced) such that \overline{AD} is parallel to \overline{AB} and \overline{DP} is parallel to \overline{AC}. Therefore,

\overline{AD} = s(\vec{b} -\vec{a}),\overline{DP} = t(\vec{c} -\vec{a}).

Now, in triangle ADP, we have

\overline{AP} = \overline{AD} +\overline{DP}\mathrm{or}\vec{r} -\vec{a} = s(\vec{b} -\vec{a}) + t(\vec{c} -\vec{a}),\mathrm{where}\vec{b}\neq \vec{0},\vec{c}\neq \vec{0}\mathrm{and}s,t\in \mathbb{R}

. That is, \vec{r} = \vec{a} +s(\vec{b} -\vec{a}) + t(\vec{c} -\vec{a})

This is the parametric form of vector equation of the plane passing through the given three non- collinear points.

(b) Non-parametric form of vector equation

Let A,B, and C be the three non collinear points on the plane with position vectors \vec{a},\vec{b},\vec{c} respectively. Then atleast two of them are non- zero vectors. Let us take \vec{b}\neq \vec{0} and \vec{c}\neq \vec{0}. Now \overline{AB} = \vec{b} -\vec{a} and \overline{AC} = \vec{c} -\vec{a}. The vectors (\vec{b} -\vec{a}) and (\vec{c} -\vec{a}) lie on the plane. Since \vec{a},\vec{b},\vec{c} are non- collinear, \overline{AB} is not parallel to \overline{AC}. Therefore, (\vec{b} -\vec{a})\times (\vec{c} -\vec{a}) is perpendicular to the plane.

If \vec{r} is the position vector of an arbitrary point P(x,y,z) on the plane, then the equation of the plane passing through the point A with position vector \vec{a} and perpendicular to the vector (\vec{b} -\vec{a})\times (\vec{c} -\vec{a}) is given by

(\vec{r} -\vec{a})\cdot ((\vec{b} -\vec{a})\times (\vec{c} -\vec{a})) = 0\quad \mathrm{or}\quad [\vec{r} -\vec{a},\vec{b} -\vec{a},\vec{c} -\vec{a}] = 0

This is the non- parametric form of vector equation of the plane passing through three non- collinear points.

(c) Cartesian form of equation

If (x*{1},y*{1},z*{1}),(x*{2},y*{2},z*{2}) and (x*{3},y*{3},z*{3}) are the coordinates of three non- collinear points A,B,C with position vectors \vec{a},\vec{b},\vec{c} respectively and (x,y,z) is the coordinates of the point P with position vector \vec{r}, then we have \vec{a} = x*{1}\hat{i} +y*{1}\hat{j} +z*{1}\hat{k} \vec{b} = x*{2}\hat{i} +y*{2}\hat{j} +z*{2}\hat{k} \vec{c} = x*{3}\hat{i} +y*{3}\hat{j} +z*{3}\hat{k} and \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}

Using these vectors, the non- parametric form of vector equation of the plane passing through the given three non- collinear points can be equivalently written as

\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ x_3 - x_1 & y_3 - y_1 & z_3 - z_1 \end{vmatrix} = 0

which is the Cartesian equation of the plane passing through three non- collinear points.

6.8.5 Equation of a plane passing through a given point and parallel to two given non-parallel vectors.

(a) Parametric form of vector equation

Consider a plane passing through a given point A with position vector \vec{a} and parallel to two given non- parallel vectors \vec{b} and \vec{c}. If \vec{r} is the position vector of an arbitrary point P on the plane, then the vectors (\vec{r} - \vec{a}),\vec{b} and \vec{c} are coplanar. So, (\vec{r} - \vec{a}) lies in the plane containing \vec{b} and \vec{c}. Then, there exists scalars s,t\in \mathbb{R} such that \vec{r} - \vec{a} = s\vec{b} +t\vec{c} which implies

\vec{r} = \vec{a} +s\vec{b} +t\vec{c},\mathrm{where}s,t\in \mathbb{R} \quad (1)

This is the parametric form of vector equation of the plane passing through a given point and parallel to two given non- parallel vectors.

(b) Non-parametric form of vector equation

Equation (1) can be equivalently written as

(\vec{r} - \vec{a})\cdot (\vec{b}\times \vec{c}) = 0 \quad (2)

which is the non- parametric form of vector equation of the plane passing through a given point and parallel to two given non- parallel vectors.

(c) Cartesian form of equation

If \vec{a} = x*{1}\hat{i} +y*{1}\hat{j} +z*{1}\hat{k} \vec{b} = b*{1}\hat{i} +b*{2}\hat{j} +b*{3}\hat{k} \vec{c} = c*{1}\hat{i} +c*{2}\hat{j} +c_{3}\hat{k} and \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}, then the equation (2) is equivalent to

\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ b_1 & b_2 & b_3 \ c_1 & c_2 & c_3 \end{vmatrix} = 0

This is the Cartesian equation of the plane passing through a given point and parallel to two given non- parallel vectors.

6.8.6 Equation of a plane passing through two given distinct points and is parallel to a non-zero vector

(a) Parametric form of vector equation

The parametric form of vector equation of the plane passing through two given distinct points A and B with position vectors \vec{a} and \vec{b}, and parallel to a non- zero vector \vec{c} is

\vec{r} = \vec{a} +s(\vec{b} -\vec{a}) + t\vec{c}\mathrm{or}\vec{r} = (1 - s)\vec{a} +s\vec{b} +t\vec{c} \quad (1)

where s,t\in \mathbb{R},(\vec{b} -\vec{a}) and \vec{c} are not parallel vectors.

(b) Non-parametric form of vector equation

Equation (1) can be written equivalently in non- parametric vector form as

(\vec{r} -\vec{a})\cdot ((\vec{b} -\vec{a})\times \vec{c}) = 0 \quad (2)

where (\vec{b} -\vec{a}) and \vec{c} are not parallel vectors.

(c) Cartesian form of equation

If \vec{a} = x*{1}\hat{i} +y*{1}\hat{j} +z*{1}\hat{k},\vec{b} = x*{2}\hat{i} +y*{2}\hat{j} +z*{2}\hat{k},\vec{c} = c*{1}\hat{i} +c*{2}\hat{j} +c_{3}\hat{k}\neq \vec{0} and \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}, then equation (2) is equivalent to

\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ c_1 & c_2 & c_3 \end{vmatrix} = 0

This is the required Cartesian equation.

Example 6.43

Find the non- parametric form of vector equation, and Cartesian equation of the plane passing through the point (0,1, - 5) and parallel to the straight lines \vec{r} = (\hat{i} +2\hat{j} - 4\hat{k}) + s(2\hat{i} +3\hat{j} +6\hat{k}) and \vec{r} = (\hat{i} - 3\hat{j} +5\hat{k}) + t(\hat{i} +\hat{j} -\hat{k}).

Solution

We observe that the required plane is parallel to the vectors \vec{b} = 2\hat{i} +3\hat{j} +6\hat{k},\vec{c} = \hat{i} +\hat{j} -\hat{k} and passing through the point (0,1, - 5) with position vector \vec{a}. We observe that \vec{b} is not parallel to \vec{c}. Then the vector equation of the plane in non- parametric form is given by (\vec{r} -\vec{a})\cdot (\vec{b}\times \vec{c}) = 0. \therefore (1)

\vec{b}\times\vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 2 & 3 & 6 \ 1 & 1 & -1 \end{vmatrix} = (-3-6)\hat{i} - (-2-6)\hat{j} + (2-3)\hat{k} = -9\hat{i} + 8\hat{j} - \hat{k}

(\vec{r} -(\hat{j} -5\hat{k}))\cdot (-9\hat{i} +8\hat{j} -\hat{k}) = 0,\mathrm{whichimpliesthat}

\vec{r}\cdot (-9\hat{i} +8\hat{j} -\hat{k}) = 13.

If \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} is the position vector of an arbitrary point on the plane, then from the above equation, we get the Cartesian equation of the plane as - 9x + 8y - z = 13 or 9x - 8y + z + 13 = 0.

Example 6.44

Find the vector parametric, vector non- parametric and Cartesian form of the equation of the plane passing through the points (- 1,2,0), (2,2 - 1) and parallel to the straight line \frac{x - 1}{1} = \frac{2y + 1}{2} = \frac{z + 1}{- 1}.

Solution

The required plane is parallel to the given line and so it is parallel to the vector \vec{c} = \hat{i} +\hat{j} -\hat{k} and the plane passes through the points \vec{a} = -\hat{i} +2\hat{j},\vec{b} = 2\hat{i} +2\hat{j} -\hat{k}.

Vector equation of the plane in parametric form is \vec{r} = \vec{a} +s\left(\vec{b} -\vec{a}\right) +t\vec{c}, where s t\in \mathbb{R} which implies that \vec{r} = \left(-\hat{i} +2\hat{j}\right) +s\left(3\hat{i} -\hat{k}\right) +t\left(\hat{i} +\hat{j} -\hat{k}\right), where s,t\in \mathbb{R} vector equation of the plane in non- parametric form is (\vec{r} -\vec{a})\cdot ((\vec{b} -\vec{a})\times \vec{c}) = 0 \mathrm{Now},(\vec{b} -\vec{a})\times \vec{c} = \left| \begin{array}{ccc}\hat{i} & \hat{j} & \hat{k}\ 3 & 0 & -1\ 1 & 1 & -1 \end{array} \right| = \hat{i} +2\hat{j} +3\hat{k}, we have (\vec{r} -(-\hat{i} +2\hat{j}))\cdot (\hat{i} +2\hat{j} +3\hat{k}) = 0\Rightarrow \vec{r}\cdot (\hat{i} +2\hat{j} +3\hat{k}) = 3 If \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} is the position vector of an arbitrary point on the plane, then from the above equation, we get the Cartesian equation of the plane as x + 2y + 3z = 3

EXERCISE 6.7

1. Find the non-parametric form of vector equation, and Cartesian equation of the plane passing through the point (2,3,6) and parallel to the straight lines \frac{x - 1}{2} = \frac{y + 1}{3} = \frac{z - 3}{1} and \frac{x + 3}{2} = \frac{y - 3}{-5} = \frac{z + 1}{-3}

2. Find the non-parametric form of vector equation, and Cartesian equations of the plane passing through the points (2,2,1), (9,3,6) and perpendicular to the plane 2x + 6y + 6z = 9.

3. Find parametric form of vector equation and Cartesian equations of the plane passing through the points (2,2,1), (1, -2,3) and parallel to the straight line passing through the points (2,1, -3) and (-1,5, -8).

4. Find the non-parametric form of vector equation and Cartesian equation of the plane passing through the point (1, -2,4) and perpendicular to the plane x + 2y - 3z = 11 and parallel to the line \frac{x + 7}{3} = \frac{y + 3}{-1} = \frac{z}{1}.

5. Find the parametric form of vector equation, and Cartesian equations of the plane containing the line \vec{r} = (\hat{i} -\hat{j} +3\hat{k}) + t(2\hat{i} -\hat{j} +4\hat{k}) and perpendicular to plane \vec{r}\cdot (\hat{i} +2\hat{j} +\hat{k}) = 8.

6. Find the parametric vector, non-parametric vector and Cartesian form of the equations of the plane passing through the three non-collinear points (3,6, -2), (-1, -2,6), and (6,4, -2).

7. Find the non-parametric form of vector equation, and Cartesian equations of the plane

   \vec{r} = \left(6\hat{i} -\hat{j} +\hat{k}\right) + s\left(-\hat{i} +2\hat{j} +\hat{k}\right) + t\left(-5\hat{i} -4\hat{j} -5\hat{k}\right).

6.8.7 Condition for a line to lie in a plane

We observe that a straight line will lie in a plane if every point on the line, lie in the plane and the normal to the plane is perpendicular to the line.

(i) If the line \vec{r} = \vec{a} +t\vec{b} lies in the plane \vec{r}\cdot \vec{n} = d, then \vec{a}\cdot \vec{n} = d and \vec{b}\cdot \vec{n} = 0

(ii) If the line \frac{x - x*{1}}{a} = \frac{y - y*{1}}{b} = \frac{z - z_{1}}{c} lies in the plane Ax + By + Cz + D = 0, then

Ax*{1} + By*{1} + Cz_{1} + D = 0 \text{and} aA + bB + cC = 0.

Example 6.45

Verify whether the line \frac{x - 3}{- 4} = \frac{y - 4}{- 7} = \frac{z + 3}{12} lies in the plane 5x - y + z = 8.

Solution

Here, (x*{1},y*{1},z_{1}) = (3,4, - 3) and direction ratios of the given straight line are (a,b,c) = (- 4, - 7,12). Direction ratios of the normal to the given plane are (A,B,C) = (5, - 1,1).

We observe that, the given point (x*{1},y*{1},z_{1}) = (3,4, - 3) satisfies the given plane 5x - y + z = 8

Next, aA + bB + cC = (- 4)(5) + (- 7)(- 1) + (12)(1) = - 1\neq 0. So, the normal to the plane is not perpendicular to the line. Hence, the given line does not lie in the plane.

6.8.8 Condition for coplanarity of two lines

(a) Condition in vector form

The two given non- parallel lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are coplanar. So they lie in a single plane. Let A and C be the points whose position vectors are \vec{a} and \vec{c}. Then A and C lie on the plane. Since \vec{b} and \vec{d} are parallel to the plane, \vec{b}\times \vec{d} is perpendicular to the plane. So \overrightarrow{AC} is perpendicular to \vec{b}\times \vec{d}. That is,

(\vec{c} -\vec{a})\cdot (\vec{b}\times \vec{d}) = 0

This is the required condition for coplanarity of two lines in vector form.

(b) Condition in Cartesian form

Two lines \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} are coplanar if

\begin{vmatrix} x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

This is the required condition for coplanarity of two lines in Cartesian form.

6.8.9 Equation of plane containing two non-parallel coplanar lines

(a) Parametric form of vector equation

Let \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} be two non- parallel coplanar lines. Then \vec{b}\times \vec{d}\neq \vec{0}. Let P be any point on the plane and let \vec{r}{0} be its position vector. Then, the vectors \vec{r}{0} - \vec{a},\vec{b},\vec{d} as well as \vec{r}{0} - \vec{c},\vec{b},\vec{d} are also coplanar. So, we get \vec{r}{0} - \vec{a} = t\vec{b} +s\vec{d} or \vec{r}_{0} - \vec{c} = t\vec{b} +s\vec{d}. Hence, the vector equation in parametric form is \vec{r} = \vec{a} +t\vec{b} +s\vec{d} or \vec{r} = \vec{c} +t\vec{b} +s\vec{d}.

(b) Non-parametric form of vector equation

Let \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} be two non- parallel coplanar lines. Then \vec{b}\times \vec{d}\neq \vec{0}. Let P be any point on the plane and let \vec{r}{0} be its position vector. Then, the vectors \vec{r}{0} - \vec{a},\vec{b},\vec{d} as well as \vec{r}{0} - \vec{c},\vec{b},\vec{d} are also coplanar. So, we get \left(\vec{r}{0} - \vec{a}\right).\left(\vec{b}\times \vec{d}\right) = 0 or \left(\vec{r}_{0} - \vec{c}\right).\left(\vec{b}\times \vec{d}\right) = 0. Hence, the vector equation in non- parametric form is \left(\vec{r} - \vec{a}\right).\left(\vec{b}\times \vec{d}\right) = 0 or \left(\vec{r} - \vec{c}\right).\left(\vec{b}\times \vec{d}\right) = 0.

(C) Cartesian form of equation of plane

In Cartesian form the equation of the plane containing the two given coplanar lines

\frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} is given by

\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

or

\begin{vmatrix} x - x_2 & y - y_2 & z - z_2 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

Example 6.46

Show that the lines \vec{r} = \left(-\hat{i} -3\hat{j} -5\hat{k}\right) + s\left(3\hat{i} +5\hat{j} +7\hat{k}\right) and \vec{r} = \left(2\hat{i} +4\hat{j} +6\hat{k}\right) + t\left(\hat{i} +4\hat{j} +7\hat{k}\right) are coplanar. Also, find the non- parametric form of vector equation of the plane containing these lines.

Solution

Comparing the two given lines with

\vec{r} = \vec{a} +t\vec{b},\vec{r} = \vec{c} +s\vec{d}

\vec{a} = -\hat{i} -3\hat{j} -5\hat{k},\vec{b} = 3\hat{i} +5\hat{j} +7\hat{k},\vec{c} = 2\hat{i} +4\hat{j} +6\hat{k}\mathrm{and}\vec{d} = \hat{i} +4\hat{j} +7\hat{k}

We know that the two given lines are coplanar, if \left(\vec{c} - \vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

\vec{c} - \vec{a} = 3\hat{i} +7\hat{j} +11\hat{k},\quad \vec{b}\times\vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 3 & 5 & 7 \ 1 & 4 & 7 \end{vmatrix} = 7\hat{i} -14\hat{j} +7\hat{k}

Then, \left(\vec{c} - \vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = \left(3\hat{i} +7\hat{j} +11\hat{k}\right)\cdot \left(7\hat{i} -14\hat{j} +7\hat{k}\right) = 0.

Therefore the two given lines are coplanar. Then we find the non- parametric form of vector equation of the plane containing the two given coplanar lines. We know that the plane containing the two given coplanar lines is

\left(\vec{r} -\vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

which implies that \left(\vec{r} - \left(-\hat{i} -3\hat{j} -5\hat{k}\right)\right)\cdot \left(7\hat{i} -14\hat{j} +7\hat{k}\right) = 0. Thus, the required non- parametric vector equation of the plane containing the two given coplanar lines is \vec{r}\cdot \left(\hat{i} - 2\hat{j} +\hat{k}\right) = 0

EXERCISE 6.8

1. Find the parametric form of vector equation and Cartesian equations of a straight line passing through (5,2,8) and is perpendicular to the straight lines \vec{r} = (\hat{i} +\hat{j} -\hat{k}) + s(2\hat{i} -2\hat{j} +\hat{k}) and \vec{r} = (2\hat{i} -\hat{j} -3\hat{k}) + t(\hat{i} +2\hat{j} +2\hat{k}).

2. Show that the lines \vec{r} = (6\hat{i} +\hat{j} +2\hat{k}) + s(\hat{i} +2\hat{j} -3\hat{k}) and \vec{r} = (3\hat{i} +2\hat{j} -2\hat{k}) + t(2\hat{i} +4\hat{j} -5\hat{k}) are skew lines and hence find the shortest distance between them.

3. If the two lines \frac{x - 1}{2} = \frac{y + 1}{3} = \frac{z - 1}{4} and \frac{x - 3}{1} = \frac{y - m}{2} = z intersect at a point, find the value of m.

4. Show that the lines \frac{x - 3}{3} = \frac{y - 3}{-1}, z - 1 = 0 and \frac{x - 6}{2} = \frac{z - 1}{3}, y - 2 = 0 intersect. Also find the point of intersection.

5. Show that the straight lines x + 1 = 2y = -12z and x = y + 2 = 6z - 6 are skew and hence find the shortest distance between them.

6. Find the parametric form of vector equation of the straight line passing through (-1,2,1) and parallel to the straight line \vec{r} = (2\hat{i} +3\hat{j} -\hat{k}) + t(\hat{i} -2\hat{j} +\hat{k}) and hence find the shortest distance between the lines.

7. Find the foot of the perpendicular drawn from the point (5,4,2) to the line \frac{x + 1}{2} = \frac{y - 3}{3} = \frac{z - 1}{-1}. Also, find the equation of the perpendicular.

6.8 Different forms of Equation of a plane

We have already seen the notion of a plane.

Definition 6.8

A vector which is perpendicular to a plane is called a normal to the plane.

Note

Every normal to a plane is perpendicular to every straight line lying on the plane.

A plane is uniquely fixed if any one of the following is given:

• a unit normal to the plane and the distance of the plane from the origin
• a point of the plane and a normal to the plane
• three non-collinear points of the plane
• a point of the plane and two non-parallel lines or non-parallel vectors which are parallel to the plane
• two distinct points of the plane and a straight line or non-zero vector parallel to the plane but not parallel to the line joining the two points.

Let us find the vector and Cartesian equations of planes using the above situations.

6.8.1 Equation of a plane when a normal to the plane and the distance of the plane from the origin are given

(a) Vector equation of a plane in normal form

Theorem 6.15

The equation of the plane at a distance p from the origin and perpendicular to the unit normal vector \hat{d} is \vec{r}\cdot \hat{d} = p.

Consider a plane whose perpendicular distance from the origin is p.

Let A be the foot of the perpendicular from O to the plane.

Let \hat{d} be the unit normal vector in the direction of \overline{OA}.

Then \overline{OA} = p\hat{d}.

If \vec{r} is the position vector of an arbitrary point P on the plane,

then \overline{AP} is perpendicular to \overline{OA}.

Therefore, \overline{AP} \cdot \overline{OA} = 0 \Rightarrow (\vec{r} - p\hat{d}) \cdot p\hat{d} = 0

\Rightarrow (\vec{r} -p\hat{d})\cdot \hat{d} = 0

which gives \vec{r} \cdot \hat{d} = p.

Fig. 6.24

The above equation is called the vector equation of the plane in normal form.

(b) Cartesian equation of a plane in normal form

Let l,m,n be the direction cosines of \hat{d}. Then we have \hat{d} = l\hat{i} +m\hat{j} +n\hat{k}.

Thus, equation (1) becomes

\vec{r} \cdot (l\hat{i} +m\hat{j} +n\hat{k}) = p

If P is (x,y,z), then \vec{r} = x\hat{i} +y\hat{j} +z\hat{k}

Therefore, (x\hat{i} +y\hat{j} +z\hat{k}) \cdot (l\hat{i} +m\hat{j} +n\hat{k}) = p or lx + my + nz = p

Equation (2) is called the Cartesian equation of the plane in normal form.

Remark

(i) If the plane passes through the origin, then p = 0. So, the equation of the plane is

lx + my + nz = 0.

(ii) If \vec{d} is normal vector to the plane, then \hat{d} = \frac{\vec{d}}{|\vec{d}|} is a unit normal to the plane. So, the vector equation of the plane is \vec{r} \cdot \frac{\vec{d}}{|\vec{d}|} = p or \vec{r} \cdot \vec{d} = q, where q = p |\vec{d} |. The equation \vec{r} \cdot \vec{d} = q is the vector equation of a plane in standard form.

Note

In the standard form \vec{r} \cdot \vec{d} = q, \vec{d} need not be a unit normal and q need not be the perpendicular distance.

6.8.2 Equation of a plane perpendicular to a vector and passing through a given point

(a) Vector form of equation

Consider a plane passing through a point A with position vector \vec{a} and \vec{n} is a normal vector to the given plane.

Let \vec{r} be the position vector of an arbitrary point P on the plane.

Fig. 6.25

Then \overline{AP} is perpendicular to \vec{n}.

\overline{AP}\cdot \vec{n} = 0 \quad (1)

which is the vector form of the equation of a plane passing through a point with position vector \vec{a} and perpendicular to \vec{n}.

Note

(\vec{r} -\vec{a})\cdot \vec{n} = 0\Rightarrow \vec{r}\cdot \vec{n} = \vec{a}\cdot \vec{n}\Rightarrow \vec{r}\cdot \vec{n} = q,

where q = \vec{a}\cdot \vec{n}.

(b) Cartesian form of equation

If a,b,c are the direction ratios of \vec{n}, then we have \vec{n} = a\vec{i} +b\vec{j} +c\vec{k}. Suppose, A is (x*{1},y*{1},z*{1}) then equation (1) becomes \left((x - x*{1})\hat{i} +(y - y*{1})\hat{j} +(z - z*{1})\hat{k}\right)\cdot (a\vec{i} +b\vec{j} +c\vec{k}) = 0. That is,

a(x - x*{1}) + b(y - y*{1}) + c(z - z_{1}) = 0

which is the Cartesian equation of a plane, normal to a vector with direction ratios a,b,c and passing through a given point (x*{1},y*{1},z_{1}).

6.8.3 Intercept form of the equation of a plane

Let the plane \vec{r}\cdot \vec{n} = q meets the coordinate axes at A,B,C respectively such that the intercepts on the axes are OA = a, OB = b, OC = c. Now position vector of the point A is a\vec{i}. Since A lies on the given plane, we have a\vec{i}\cdot \vec{n} = q which gives \hat{i}\cdot \vec{n} = \frac{q}{a}. Similarly, since the vectors \vec{b}\vec{j} and c\vec{k} lie on the given plane, we have \hat{j}\cdot \vec{n} = \frac{q}{b} and \hat{k}\cdot \vec{n} = \frac{q}{c}. Substituting \vec{r} = x\vec{i} +y\vec{j} +z\vec{k} in \vec{r}\cdot \vec{n} = q, we get x\vec{i}\cdot \vec{n} +y\vec{j}\cdot \vec{n} +z\vec{k}\cdot \vec{n} = q. So x\left(\frac{q}{a}\right) + y\left(\frac{q}{b}\right) + z\left(\frac{q}{c}\right) = q.

Fig. 6.26

Dividing by q, we get, \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1. This is called the intercept form of equation of the plane having intercepts a,b,c on the x,y,z axes respectively.

Theorem 6.16

The general equation ax + by + cz + d = 0 of first degree in x,y,z represents a plane.

Proof

The equation ax + by + cz + d = 0 can be written in the vector form as follows

(x\vec{i} +y\vec{j} +z\vec{k})\cdot (a\vec{i} +b\vec{j} +c\vec{k}) = -d\quad \text{or}\quad \vec{r}\cdot \vec{n} = -d.

Since this is the vector form of the equation of a plane in standard form, the given equation ax + by + cz + d = 0 represents a plane. Here \vec{n} = a\vec{i} +b\vec{j} +c\vec{k} is a vector normal to the plane.

Note

In the general equation ax + by + cz + d = 0 of a plane, a,b,c are direction ratios of the normal to the plane.

Example 6.38

Find the vector and Cartesian form of the equations of a plane which is at a distance of 12 units from the origin and perpendicular to 6\hat{i} +2\hat{j} - 3\hat{k}.

Solution

Let \vec{d} = 6\hat{i} +2\hat{j} - 3\hat{k} and p = 12.

If \hat{d} is the unit normal vector in the direction of the vector 6\hat{i} +2\hat{j} - 3\hat{k}

\text{then} \hat{d} = \frac{\vec{d}}{|\vec{d}|} = \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}).

If \vec{r} is the position vector of an arbitrary point (x,y,z) on the plane, then using \vec{r}\cdot \hat{d} = p, the vector equation of the plane in normal form is \vec{r}\cdot \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}) = 12.

Substituting \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} in the above equation, we get (x\hat{i} +y\hat{j} +z\hat{k})\cdot \frac{1}{7} (6\hat{i} +2\hat{j} - 3\hat{k}) = 12. Applying dot product in the above equation and simplifying, we get 6x + 2y - 3z = 84, which is the Cartesian equation of the required plane.

Example 6.39

If the Cartesian equation of a plane is 3x - 4y + 3z = - 8, find the vector equation of the plane in the standard form.

Solution

If \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} is the position vector of an arbitrary point (x,y,z) on the plane, then the given equation can be written as (x\hat{i} +y\hat{j} +z\hat{k})\cdot (3\hat{i} - 4\hat{j} +3\hat{k}) = - 8 or (x\hat{i} +y\hat{j} +z\hat{k})\cdot (- 3\hat{i} +4\hat{j} - 3\hat{k}) = 8. That is, \vec{r}\cdot (- 3\hat{i} +4\hat{j} - 3\hat{k}) = 8 which is the vector equation of the given plane in standard form.

Example 6.40

Find the direction cosines of the normal to the plane and length of the perpendicular from the origin to the plane \vec{r}\cdot (3\hat{i} - 4\hat{j} +12\hat{k}) = 5.

Solution

Let \vec{d} = 3\hat{i} - 4\hat{j} +12\hat{k} and q = 5.

If \hat{d} is the unit vector in the direction of the vector 3\hat{i} - 4\hat{j} +12\hat{k}, then \hat{d} = \frac{1}{13} (3\hat{i} - 4\hat{j} +12\hat{k}).

Now, dividing the given equation by 13, we get

\vec{r}\cdot \left(\frac{3}{13}\hat{i} -\frac{4}{13}\hat{j} +\frac{12}{13}\hat{k}\right) = \frac{5}{13}

which is the equation of the plane in the normal form \vec{r}\cdot \hat{d} = p.

From this equation, we infer that \hat{d} = \frac{1}{13} (3\hat{i} - 4\hat{j} +12\hat{k}) is a unit vector normal to the plane from the origin. Therefore, the direction cosines of \hat{d} are \frac{3}{13},\frac{- 4}{13},\frac{12}{13} and the length of the perpendicular from the origin to the plane is \frac{5}{13}.

Example 6.41

Find the vector and Cartesian equations of the plane passing through the point with position vector 4\dot{i} +2\dot{j} -3\dot{k} and normal to vector 2\dot{i} - \dot{j} +\dot{k}.

Solution

If the position vector of the given point is \vec{a} = 4\dot{i} +2\dot{j} - 3\dot{k} and \vec{n} = 2\dot{i} - \dot{j} +\dot{k}, then the equation of the plane passing through a point and normal to a vector is given by (\vec{r} -\vec{a})\cdot \vec{n} = 0 or \vec{r}\cdot \vec{n} = \vec{a}\cdot \vec{n}.

Substituting \vec{a} = 4\dot{i} +2\dot{j} - 3\dot{k} and \vec{n} = 2\dot{i} - \dot{j} +\dot{k} in the above equation, we get

\vec{r}\cdot (2\dot{i} -\dot{j} +\dot{k}) = (4\dot{i} +2\dot{j} -3\dot{k})\cdot (2\dot{i} -\dot{j} +\dot{k})

Thus, the required vector equation of the plane is \vec{r}\cdot (2\dot{i} -\dot{j} +\dot{k}) = 3. If \vec{r} = x\dot{i} +y\dot{j} +z\dot{k} then we get the Cartesian equation of the plane 2x - y + z = 3.

Example 6.42

A variable plane moves in such a way that the sum of the reciprocals of its intercepts on the coordinate axes is a constant. Show that the plane passes through a fixed point

Solution

The equation of the plane having intercepts a,b,c on the x,y,z axes respectively is \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1. Since the sum of the reciprocals of the intercepts on the coordinate axes is a constant, we have \frac{1}{a} +\frac{1}{b} +\frac{1}{c} = k, where k is a constant, and which can be written as \frac{1}{a}\left(\frac{1}{k}\right) + \frac{1}{b}\left(\frac{1}{k}\right) + \frac{1}{c}\left(\frac{1}{k}\right) = 1. This shows that the plane \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1 passes through the fixed point \left(\frac{1}{k},\frac{1}{k},\frac{1}{k}\right).

EXERCISE 6.6

1. Find the vector equation of a plane which is at a distance of 7 units from the origin having 3, -4,5 as direction ratios of a normal to it.

2. Find the direction cosines of the normal to the plane 12x + 3y - 4z = 65. Also, find the non-parametric form of vector equation of a plane and the length of the perpendicular to the plane from the origin.

3. Find the vector and Cartesian equations of the plane passing through the point with position vector 2\dot{i} +6\dot{j} +3\dot{k} and normal to the vector \dot{i} +3\dot{j} +5\dot{k}.

4. A plane passes through the point (-1,1,2) and the normal to the plane of magnitude 3\sqrt{3} makes equal acute angles with the coordinate axes. Find the equation of the plane.

5. Find the intercepts cut off by the plane \vec{r}\cdot (6\dot{i} +4\dot{j} -3\dot{k}) = 12 on the coordinate axes.

6. If a plane meets the coordinate axes at A,B,C such that the centroid of the triangle ABC is the point (u,v,w), find the equation of the plane.

EXERCISE 6.7

1. Find the non-parametric form of vector equation, and Cartesian equation of the plane passing through the point (2,3,6) and parallel to the straight lines \frac{x - 1}{2} = \frac{y + 1}{3} = \frac{z - 3}{1} and \frac{x + 3}{2} = \frac{y - 3}{-5} = \frac{z + 1}{-3}

2. Find the non-parametric form of vector equation, and Cartesian equations of the plane passing through the points (2,2,1), (9,3,6) and perpendicular to the plane 2x + 6y + 6z = 9.

3. Find parametric form of vector equation and Cartesian equations of the plane passing through the points (2,2,1), (1, -2,3) and parallel to the straight line passing through the points (2,1, -3) and (-1,5, -8).

4. Find the non-parametric form of vector equation and Cartesian equation of the plane passing through the point (1, -2,4) and perpendicular to the plane x + 2y - 3z = 11 and parallel to the line \frac{x + 7}{3} = \frac{y + 3}{-1} = \frac{z}{1}.

5. Find the parametric form of vector equation, and Cartesian equations of the plane containing the line \vec{r} = (\hat{i} -\hat{j} +3\hat{k}) + t(2\hat{i} -\hat{j} +4\hat{k}) and perpendicular to plane \vec{r}\cdot (\hat{i} +2\hat{j} +\hat{k}) = 8.

6. Find the parametric vector, non-parametric vector and Cartesian form of the equations of the plane passing through the three non-collinear points (3,6, -2), (-1, -2,6), and (6,4, -2).

7. Find the non-parametric form of vector equation, and Cartesian equations of the plane

\vec{r} = \left(6\hat{i} -\hat{j} +\hat{k}\right) + s\left(-\hat{i} +2\hat{j} +\hat{k}\right) + t\left(-5\hat{i} -4\hat{j} -5\hat{k}\right).

6.8.7 Condition for a line to lie in a plane

We observe that a straight line will lie in a plane if every point on the line, lie in the plane and the normal to the plane is perpendicular to the line.

(i) If the line \vec{r} = \vec{a} +t\vec{b} lies in the plane \vec{r}\cdot \vec{n} = d, then \vec{a}\cdot \vec{n} = d and \vec{b}\cdot \vec{n} = 0

(ii) If the line \frac{x - x*{1}}{a} = \frac{y - y*{1}}{b} = \frac{z - z_{1}}{c} lies in the plane Ax + By + Cz + D = 0, then

Ax*{1} + By*{1} + Cz_{1} + D = 0 \text{ and } aA + bB + cC = 0.

Example 6.45

Verify whether the line \frac{x - 3}{- 4} = \frac{y - 4}{- 7} = \frac{z + 3}{12} lies in the plane 5x - y + z = 8.

Solution

Here, (x*{1},y*{1},z_{1}) = (3,4, - 3) and direction ratios of the given straight line are (a,b,c) = (- 4, - 7,12). Direction ratios of the normal to the given plane are (A,B,C) = (5, - 1,1).

We observe that, the given point (x*{1},y*{1},z_{1}) = (3,4, - 3) satisfies the given plane 5x - y + z = 8.

Next, aA + bB + cC = (- 4)(5) + (- 7)(- 1) + (12)(1) = - 1\neq 0. So, the normal to the plane is not perpendicular to the line. Hence, the given line does not lie in the plane.

6.8.8 Condition for coplanarity of two lines

(a) Condition in vector form

The two given non- parallel lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are coplanar. So they lie in a single plane. Let A and C be the points whose position vectors are \vec{a} and \vec{c}. Then A and C lie on the plane. Since \vec{b} and \vec{d} are parallel to the plane, \vec{b}\times \vec{d} is perpendicular to the plane. So \overrightarrow{AC} is perpendicular to \vec{b}\times \vec{d}. That is,

Fig. 6.29

(\vec{c} -\vec{a})\cdot (\vec{b}\times \vec{d}) = 0

This is the required condition for coplanarity of two lines in vector form.

(b) Condition in Cartesian form

Two lines \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} are coplanar if

\begin{vmatrix} x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

This is the required condition for coplanarity of two lines in Cartesian form.

6.8.9 Equation of plane containing two non-parallel coplanar lines

(a) Parametric form of vector equation

Let \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} be two non- parallel coplanar lines. Then \vec{b}\times \vec{d}\neq \vec{0}. Let P be any point on the plane and let \vec{r}{0} be its position vector. Then, the vectors \vec{r}{0} - \vec{a},\vec{b},\vec{d} as well as \vec{r}{0} - \vec{c},\vec{b},\vec{d} are also coplanar. So, we get \vec{r}{0} - \vec{a} = t\vec{b} +s\vec{d} or \vec{r}_{0} - \vec{c} = t\vec{b} +s\vec{d}. Hence, the vector equation in parametric form is \vec{r} = \vec{a} +t\vec{b} +s\vec{d} or \vec{r} = \vec{c} +t\vec{b} +s\vec{d}.

(b) Non-parametric form of vector equation

Let \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} be two non- parallel coplanar lines. Then \vec{b}\times \vec{d}\neq \vec{0}. Let P be any point on the plane and let \vec{r}{0} be its position vector. Then, the vectors \vec{r}{0} - \vec{a},\vec{b},\vec{d} as well as \vec{r}{0} - \vec{c},\vec{b},\vec{d} are also coplanar. So, we get \left(\vec{r}{0} - \vec{a}\right).\left(\vec{b}\times \vec{d}\right) = 0 or \left(\vec{r}_{0} - \vec{c}\right).\left(\vec{b}\times \vec{d}\right) = 0. Hence, the vector equation in non- parametric form is \left(\vec{r} - \vec{a}\right).\left(\vec{b}\times \vec{d}\right) = 0 or \left(\vec{r} - \vec{c}\right).\left(\vec{b}\times \vec{d}\right) = 0.

(C) Cartesian form of equation of plane

In Cartesian form the equation of the plane containing the two given coplanar lines

\frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} is given by

\begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

Example 6.46

Show that the lines \vec{r} = \left(-\hat{i} -3\hat{j} -5\hat{k}\right) + s\left(3\hat{i} +5\hat{j} +7\hat{k}\right) and \vec{r} = \left(2\hat{i} +4\hat{j} +6\hat{k}\right) + t\left(\hat{i} +4\hat{j} +7\hat{k}\right) are coplanar. Also, find the non- parametric form of vector equation of the plane containing these lines.

Solution

Comparing the two given lines with

\vec{r} = \vec{a} +t\vec{b},\quad \vec{r} = \vec{c} +s\vec{d}

\vec{a} = -\hat{i} -3\hat{j} -5\hat{k},\quad \vec{b} = 3\hat{i} +5\hat{j} +7\hat{k},\quad \vec{c} = 2\hat{i} +4\hat{j} +6\hat{k}\quad \text{and}\quad \vec{d} = \hat{i} +4\hat{j} +7\hat{k}

We know that the two given lines are coplanar, if \left(\vec{c} - \vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0.

First, compute \vec{b}\times \vec{d}:

\vec{b}\times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ 3 & 5 & 7 \ 1 & 4 & 7 \end{vmatrix} = (35-28)\hat{i} - (21-7)\hat{j} + (12-5)\hat{k} = 7\hat{i} - 14\hat{j} + 7\hat{k}

Now, \vec{c} - \vec{a} = (2\hat{i} +4\hat{j} +6\hat{k}) - (-\hat{i} -3\hat{j} -5\hat{k}) = 3\hat{i} +7\hat{j} +11\hat{k}.

Then, \left(\vec{c} - \vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = \left(3\hat{i} +7\hat{j} +11\hat{k}\right)\cdot \left(7\hat{i} -14\hat{j} +7\hat{k}\right) = 21 - 98 + 77 = 0.

Therefore the two given lines are coplanar. Then we find the non- parametric form of vector equation of the plane containing the two given coplanar lines. We know that the plane containing the two given coplanar lines is

\left(\vec{r} -\vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

which implies that \left(\vec{r} - \left(-\hat{i} -3\hat{j} -5\hat{k}\right)\right)\cdot \left(7\hat{i} -14\hat{j} +7\hat{k}\right) = 0. Thus, the required non-parametric vector equation of the plane containing the two given coplanar lines is \vec{r}\cdot \left(\hat{i} - 2\hat{j} +\hat{k}\right) = 0.

EXERCISE 6.8

1. Show that the straight lines \vec{r} = (5\hat{i} +7\hat{j} -3\hat{k}) + s(4\hat{i} +4\hat{j} -5\hat{k}) and \vec{r} = \left(8\hat{i} +4\hat{j} +5\hat{k}\right) + t\left(7\hat{i} +\hat{j} +3\hat{k}\right) are coplanar. Find the vector equation of the plane in which they lie.

2. Show that the lines \frac{x - 2}{1} = \frac{y - 3}{1} = \frac{z - 4}{3} and \frac{x - 1}{-3} = \frac{y - 4}{2} = \frac{z - 5}{1} are coplanar. Also, find the plane containing these lines.

3. If the straight lines \frac{x - 1}{1} = \frac{y - 2}{2} = \frac{z - 3}{m^{2}} and \frac{x - 3}{1} = \frac{y - 2}{m^{2}} = \frac{z - 1}{2} are coplanar, find the distinct real values of m .

4. If the straight lines \frac{x - 1}{2} = \frac{y + 1}{\lambda} = \frac{z}{5} and \frac{x + 1}{5} = \frac{y + 1}{\lambda} = \frac{z}{\lambda} are coplanar, find \lambda and equations of the planes containing these two lines.

6.8.10 Angle between two planes

The angle between two given planes is same as the angle between their normals.

Theorem 6.18

The acute angle \theta between the two planes \vec{r}\cdot \vec{n}{1} = p{1} and \vec{r}\cdot \vec{n}{2} = p{2} is given by

\theta = \cos^{-1}\left(\frac{|\vec{n}{1}\cdot\vec{n}{2}|}{|\vec{n}{1}||\vec{n}{2}|}\right)

Fig.6.30

Proof

If \theta is the acute angle between two planes \vec{r}\cdot \vec{n}{1} = p{1} and \vec{r}\cdot \vec{n}{2} = p{2} , then \theta is the acute angle between their normal vectors \vec{n}{1} and \vec{n}{2} .

Therefore, \cos \theta = \left(\frac{|\vec{n}{1}\cdot\vec{n}{2}|}{|\vec{n}{1}||\vec{n}{2}|}\right)\Rightarrow \theta = \cos^{- 1}\left(\frac{|\vec{n}{1}\cdot\vec{n}{2}|}{|\vec{n}{1}||\vec{n}{2}|}\right) … (1)

Remark

(i) If two planes \vec{r}\cdot \vec{n}{1} = p{1} and \vec{r}\cdot \vec{n}{2} = p{2} are perpendicular, then \vec{n}{1}\cdot \vec{n}{2} = 0

(ii) If the planes \vec{r}\cdot \vec{n}{1} = p{1} and \vec{r}\cdot \vec{n}{2} = p{2} are parallel, then \vec{n}{1} = \lambda \vec{n}{2} , where \lambda is a scalar

(iii) Equation of a plane parallel to the plane \vec{r}\cdot \vec{n} = p is \vec{r}\cdot \vec{n} = k , k\in \mathbb{R}

Theorem 6.19

The acute angle \theta between the planes a*{1}x + b*{1}y + c*{1}z + d*{1} = 0 and

a*{2}x + b*{2}y + c*{2}z + d*{2} = 0 \text{ is given by } \theta = \cos^{-1}\left(\frac{|a*{1}a*{2} + b*{1}b*{2} + c*{1}c*{2}|}{\sqrt{a*{1}^{2} + b*{1}^{2} + c*{1}^{2}}\sqrt{a*{2}^{2} + b*{2}^{2} + c*{2}^{2}}}\right)

XII - Mathematics

If \vec{n}{1} and \vec{n}{2} are the vectors normal to the two given planes a*{i}x + b*{i}y + c*{i}z + d*{1} = 0 and a*{2}x + b*{2}y + c*{2}z + d*{2} = 0 respectively. Then, \vec{n}{1} = a{1}\hat{i} +b*{1}\hat{j} +c*{1}\hat{k} and \vec{n}{2} = a{2}\hat{i} +b*{2}\hat{j} +c*{2}\hat{k}

Therefore, using equation (1) in theorem 6.18 the acute angle \theta between the planes is given by equation

Remark

(i) The planes a*{1}x + b*{1}y + c*{1}z + d*{1} = 0 and a*{2}x + b*{2}y + c*{2}z + d*{2} = 0 are perpendicular if

a*{1}a*{2} + b*{1}b*{2} + c*{1}c*{2} = 0

(ii) The planes a*{1}x + b*{1}y + c*{1}z + d*{1} = 0 and a*{2}x + b*{2}y + c*{2}z + d*{2} = 0 are parallel if \frac{a*{1}}{a*{2}} = \frac{b*{1}}{b*{2}} = \frac{c*{1}}{c*{2}}

(iii) Equation of a plane parallel to the plane ax + by + cz = p is ax + by + cz = k , k \in \mathbb{R}

Example 6.47

Find the acute angle between the planes \vec{r} \cdot \left(2\hat{i} +2\hat{j} +2\hat{k}\right) = 11 and 4x - 2y + 2z = 15 .

Solution

The normal vectors of the two given planes \vec{r} \cdot \left(2\hat{i} +2\hat{j} +2\hat{k}\right) = 11 and 4x - 2y + 2z = 15 are \vec{n}{1} = 2\hat{i} +2\hat{j} +2\hat{k} and \vec{n}{2} = 4\hat{i} - 2\hat{j} +2\hat{k} respectively.

If \theta is the acute angle between the planes, then we have equation

6.8.11 Angle between a line and a plane

We know that the angle between a line and a plane is the complement of the angle between the normal to the plane and the line

Let \vec{r} = \vec{a} +t\vec{b} be the equation of the line and \vec{r}\cdot \vec{n} = p be the equation of the plane. We know that \vec{b} is parallel to the given line and \vec{n} is normal to the given plane. If \theta is the acute angle between the line and the plane, then the acute angle between \vec{n} and \vec{b} is \left(\frac{\pi}{2} -\theta\right) . Therefore,

\cos \left(\frac{\pi}{2} -\theta\right) = \sin \theta = \frac{\left|\vec{b}\cdot\vec{n}\right|}{\left|\vec{b}\right|\left|\vec{n}\right|}

So, the acute angle between the line and the plane is given by \theta = \sin^{- 1}\left(\frac{|\vec{b}\cdot\vec{n}|}{|\vec{b}||\vec{n}|}\right) … (1)

In Cartesian form if \frac{x - x*{1}}{a*{1}} = \frac{y - y*{1}}{b*{1}} = \frac{z - z*{1}}{c*{1}} and a x + b y + c z = p are the equations of the line and the plane, then \vec{b} = a*{1}\hat{i} +b*{1}\hat{j} +c_{1}\hat{k} and \vec{n} = a\hat{i} +b\hat{j} +c\hat{k} . Therefore, using (1), the acute angle \theta between the line and plane is given by

the plane, then \vec{b} = a*{1}\hat{i} +b*{1}\hat{j} +c_{1}\hat{k} and \vec{n} = a\hat{i} +b\hat{j} +c\hat{k} . Therefore, using (1), the acute angle \theta between the line and plane is given by

\theta = \sin^{-1}\left(\frac{|a a*{1} + b b*{1} + c c*{1}|}{\sqrt{a^{2} + b^{2} + c^{2}}\sqrt{a*{1}^{2} + b*{1}^{2} + c*{1}^{2}}}\right)

Remark

(i) If the line is perpendicular to the plane, then the line is parallel to the normal to the plane.

So, \vec{b} is perpendicular to \vec{n} . Then we have \vec{b} = \lambda \vec{n} where \lambda \in \mathbb{R} , which gives \frac{a*{1}}{a} = \frac{b*{1}}{b} = \frac{c_{1}}{c} .

(ii) If the line is parallel to the plane, then the line is perpendicular to the normal to the plane.

Therefore, \vec{b}\cdot \vec{n} = 0\Rightarrow a a*{1} + b b*{1} + c c_{1} = 0

Example 6.48

Find the angle between the straight line \vec{r} = \left(2\hat{i} +3\hat{j} +\hat{k}\right) + t\left(\hat{i} -\hat{j} +\hat{k}\right) and the plane 2x - y + z = 5 .

Solution

The angle between a line \vec{r} = \vec{a} +t\vec{b} and a plane \vec{r}\cdot \vec{n} = p with normal \vec{n} is \theta = \sin^{- 1}\left(\frac{|\vec{b}\cdot\vec{n}|}{|\vec{b}||\vec{n}|}\right) .

Here, \vec{b} = \hat{i} -\hat{j} +\hat{k} and \vec{n} = 2\hat{i} -\hat{j} +\hat{k} .

equation

6.8.12 Distance of a point from a plane

(a) Equation of a plane in vector form

Theorem 6.20

The perpendicular distance from a point with position vector \vec{u} to the plane \vec{r}\cdot \vec{n} = p is given by

\delta = \frac{|\vec{u}\cdot\vec{n} - p|}{|\vec{n}|}.

Proof

Let \mathcal{A} be the point whose position vector is \vec{u} .

Let F be the foot of the perpendicular from the point A to the plane \vec{r}\cdot \vec{n} = p . The line joining F and A is parallel to the normal vector \vec{n} and hence its equation is \vec{r} = \vec{u} +t\vec{n} .

But F is the point of intersection of the line \vec{r} = \vec{u} +t\vec{n} and the given plane \vec{r}\cdot \vec{n} = p . If \vec{r}{1} is the position vector of F , then \vec{r}{1} = \vec{u} +t*{1}\vec{n} for some t*{1}\in \mathbb{R} , and \vec{r}{1}\cdot \vec{n} = p . Eliminating \vec{r}{1} we get

(\vec{u} +t*{1}\vec{n})\cdot \vec{n} = p \text{ which implies } t*{1} = \frac{p - (\vec{u}\cdot\vec{n})}{|\vec{n}|^{2}}.

Fig. 6.32

\overline{{F A}} = \vec{u} -(\vec{u} +t*{1}\vec{n}) = -t*{1}\vec{n} = \left(\frac{(\vec{u}\cdot\vec{n}) - p}{|\vec{n}|^{2}}\right)\vec{n}

Therefore, the length of the perpendicular from the point A to the given plane is

\delta = |\overline{{F A}} | = \left|\left(\frac{(\vec{u}\cdot\vec{n}) - p}{|\vec{n}|^{2}}\right)\vec{n}\right| = \left|\left(\vec{u}\cdot\vec{n}\right) - p\right|

The position vector of the foot F of the perpendicular AF is given by

\vec{r}{1} = \vec{u} +t{1}\vec{n} \text{ or } \vec{r}_{1} = \vec{u} +\left(\frac{p - \vec{u}\cdot\vec{n}}{|\vec{n}|^{2}}\right)\vec{n}

(b) Equation of a plane in Cartesian form

In Cartesian form if A\left(x*{1},y*{1},z*{1}\right) is the given point with position vector \vec{u} and a x + b y + c z = p is the Cartesian equation of the given plane, then \vec{u} = x*{1}\hat{i} +y*{1}\hat{j} +z*{1}\hat{k} and \vec{n} = a\hat{i} +b\hat{j} +c\hat{k} . Therefore, using these vectors in \delta = \frac{|\vec{u}\cdot\vec{n} - p|}{|\vec{n}|} , we get the perpendicular distance from a point to the plane in Cartesian form as

\delta = \frac{|a x*{1} + b y*{1} + c z*{1} - p|}{\sqrt{a^{2} + b^{2} + c^{2}}} = \frac{|a x*{1} + b y*{1} + c z*{1} - p|}{\sqrt{a^{2} + b^{2} + c^{2}}}

Remark

The perpendicular distance from the origin to the plane a x + b y + c z + d = 0 is given by

\delta = \frac{|d|}{\sqrt{a^{2} + b^{2} + c^{2}}}

Example 6.49

Find the distance of a point (2,5, - 3) from the plane \vec{r}\cdot \left(6\hat{i} - 3\hat{j} +2\hat{k}\right) = 5

Solution

Comparing the given equation of the plane with \vec{r}\cdot \vec{n} = p , we have \vec{n} = 6\hat{i} - 3\hat{j} +2\hat{k} .

We know that the perpendicular distance from the given point with position vector \vec{u} to the plane \vec{r}\cdot \vec{n} = p is given by \delta = \frac{|\vec{u}\cdot\vec{n} - p|}{|\vec{n}|} . Therefore, substituting \vec{u} = (2,5, - 3) = 2\hat{i} +5\hat{j} - 3\hat{k} and \vec{n} = 6\hat{i} - 3\hat{j} +2\hat{k} in the formula, we get

\delta = \frac{|\vec{u}\cdot\vec{n} - p|}{|\vec{n}|} = \frac{\left|(2\hat{i} +5\hat{j} - 3\hat{k})\cdot(6\hat{i} -3\hat{j} +2\hat{k}) - 5\right|}{|6\hat{i} -3\hat{j} +2\hat{k}|} = 2 \text{ units}.

Example 6.50

Find the distance of the point (5, - 5, - 10) from the point of intersection of a straight line passing through the points A(4,1,2) and B(7,5,4) with the plane x - y + z = 5 .

Solution

The Cartesian equation of the straight line joining A and B is

\frac{x - 4}{3} = \frac{y - 1}{4} = \frac{z - 2}{2} = t \text{ (say).}

Therefore, an arbitrary point on the straight line is of the form (3t + 4,4t + 1,2t + 2) . To find the point of intersection of the straight line and the plane, we substitute x = 3t + 4,y = 4t + 1,z = 2t + 2 in x - y + z = 5 , and we get t = 0 . Therefore, the point of intersection of the straight line is (4,1,2) . Now, the distance between the two points (4,1,2) and (5, - 5, - 10) is

\sqrt{(4 - 5)^2 + (1 + 5)^2 + (2 + 10)^2} = \sqrt{181} \text{ units}.

6.8.13 Distance between two parallel planes

Theorem 6.21

The distance between two parallel planes ax + by + cz + d_1 = 0 and ax + by + cz + d_2 = 0 is given by \frac{|d_1 - d_2|}{\sqrt{a^2 + b^2 + c^2}} .

Proof

Let A(x*{1},y*{1},z_{1}) be any point on the plane ax + by + cz + d_2 = 0 , then we have

ax*{1} + by*{1} + cz*{1} + d*{2} = 0\Rightarrow ax*{1} + by*{1} + cz*{1} = -d*{2}

The distance of the plane ax + by + cz + d1 = 0 from the point A(x{1},y*{1},z*{1}) is given by

\delta = \frac{|ax*{1} + by*{1} + cz*{1} + d*{1}|}{\sqrt{a^{2} + b^{2} + c^{2}}} = \frac{|d*{1} - d*{2}|}{\sqrt{a^{2} + b^{2} + c^{2}}}

Hence, the distance between two parallel planes ax + by + cz + d_1 = 0 and ax + by + cz + d_2 = 0 is given by \delta = \frac{|d_1 - d_2|}{\sqrt{a^2 + b^2 + c^2}} .

Find the distance between the parallel planes x + 2y - 2z + 1 = 0 and 2x + 4y - 4z + 5 = 0 .

Solution

We know that the formula for the distance between two parallel planes a x + b y + c z + d*{1} = 0 and a x + b y + c z + d*{2} = 0 is \delta = \frac{\left|d*{1} - d*{2}\right|}{\sqrt{a^{2} + b^{2} + c^{2}}} . Rewrite the second equation as x + 2y - 2z + \frac{5}{2} = 0 .

Comparing the given equations with the general equations, we get a = 1,b = 2,c = - 2,d*{1} = 1,d*{2} = \frac{5}{2} .

Substituting these values in the formula, we get the distance

\delta = \frac{\left|d*{1} - d*{2}\right|}{\sqrt{a^{2} + b^{2} + c^{2}}} = \frac{\left|1 - \frac{5}{2}\right|}{\sqrt{1^{2} + 2^{2} + \left(-2^{2}\right)}} = \frac{1}{2} \text{ units}.

Example 6.52

Find the distance between the planes \vec{r}\cdot \left(2\hat{i} -\hat{j} -2\hat{k}\right) = 6 and \vec{r}\cdot \left(6\hat{i} -3\hat{j} -6\hat{k}\right) = 27

Solution

Let \vec{u} be the position vector of an arbitrary point on the plane \vec{r}\cdot (2\hat{i} -\hat{j} -2\hat{k}) = 6 . Then, we have

\vec{u}\cdot (2\hat{i} -\hat{j} -2\hat{k}) = 6. \quad (1)

If \delta is the distance between the given planes, then \delta is the perpendicular distance from \vec{u} to the plane

\vec{r}\cdot (6\hat{i} -3\hat{j} -6\hat{k}) = 27. Therefore, \delta = \frac{\left|\vec{u}\cdot\vec{n} - p\right|}{\left|\vec{n}\right|} = \frac{\left|\vec{u}\cdot(6\hat{i} - 3\hat{j} - 6\hat{k}) - 27\right|}{\sqrt{6^{2} + (-3)^{2} + (-6)^{2}}} = \left|\frac{3(\vec{u}\cdot(2\hat{i} - \hat{j} - 2\hat{k})) - 27}{9}\right| = \left|\frac{(3(6) - 27)}{9}\right| = 1 unit.

6.8.14 Equation of line of intersection of two planes

Let \vec{r}\cdot \vec{n} = p and \vec{r}\cdot \vec{m} = q be two non- parallel planes. We know that \vec{n} and \vec{m} are perpendicular to the given planes respectively. So, the line of intersection of these planes is perpendicular to both \vec{n} and \vec{m} . Therefore, it is parallel to the vector \vec{n}\times \vec{m} . Let \vec{n}\times \vec{m} = l*{1}\hat{i} +l*{2}\hat{j} +l_{3}\hat{k}

Consider the equations of two planes a*{1}x + b*{1}y + c*{1}z = p and a*{2}x + b*{2}y + c*{2}z = q . The line of intersection of the two given planes intersects at least one of the coordinate planes. For simplicity, we assume that the line meets the coordinate plane z = 0 . Substitute z = 0 and obtain the two equations a*{1}x + b*{1}y - p = 0 and a*{2}x + b*{2}y - q = 0 . Then by solving these equations, we get the values of x and y as x*{1} and y*{1} respectively.

Fig. 6.33

6.8.15 Equation of a plane passing through the line of intersection of two given planes

Theorem 6.22

The vector equation of a plane which passes through the line of intersection of the planes \vec{r}\cdot \vec{n}{1} = d{1} and \vec{r}\cdot \vec{n}{2} = d{2} is given by \left(\vec{r}\cdot \vec{n}{1} - d{1}\right) + \lambda \left(\vec{r}\cdot \vec{n}{2} - d{2}\right) = 0 , where \lambda \in \mathbb{R} .

Proof

Consider the equation

\left(\vec{r}\cdot \vec{n}{1} - d{1}\right) + \lambda \left(\vec{r}\cdot \vec{n}{2} - d{2}\right) = 0 \quad (1)

The above equation can be simplified as

\vec{r}\cdot (\vec{n}{1} + \lambda \vec{n}{2}) - (d*{1} + \lambda d*{2}) = 0 \quad (2)

Put \vec{n} = \vec{n}{1} + \lambda \vec{n}{2} , d = (d*{1} + \lambda d*{2}) .

Then the equation (2) becomes

\vec{r}\cdot \vec{n} = d \quad (3)

Fig. 6.34

The equation (3) represents a plane. Hence (1) represents a plane.

Let \vec{r}{1} be the position vector of any point on the line of intersection of the plane. Then \vec{r}{1} satisfies both the equations \vec{r}\cdot \vec{n}{1} = d{1} and \vec{r}\cdot \vec{n}{2} = d{2} . So, we have

\begin{array}{r l r} & {} & {\vec{r}{1}\cdot \vec{n}{1} = d*{1}}\ & {} & {\text{and}\quad \vec{r}*{2}\cdot \vec{n}{2} = d{2}} \end{array} \quad (4)

By (4) and (5), \vec{r}_{1} satisfies (1). So, any point on the line of intersection lies on the plane (1). This proves that the plane (1) passes through the line of intersection.

The cartesian equation of a plane which passes through the line of intersection of the planes a*{1}x + b*{1}y + c*{1}z = d*{1} and a*{2}x + b*{2}y + c*{2}z = d*{2} is given by

(a*{1}x + b*{1}y + c*{1}z - d*{1}) + \lambda (a*{2}x + b*{2}y + c*{2}z - d*{2}) = 0

Example 6.53

Find the equation of the plane passing through the intersection of the planes \vec{r}\cdot \left(\hat{i} +\hat{j} +\hat{k}\right) + 1 = 0 and \vec{r}\cdot \left(2\hat{i} - 3\hat{j} +5\hat{k}\right) = 2 and the point (- 1,2,1) .

Solution

We know that the vector equation of a plane passing through the line of intersection of the planes \vec{r}\cdot \vec{n}{1} = d{1} and \vec{r}\cdot \vec{n}{2} = d{2} is given by \left(\vec{r}\cdot \vec{n}{1} - d{1}\right) + \lambda \left(\vec{r}\cdot \vec{n}{2} - d{2}\right) = 0

Substituting \vec{r} = x\hat{i} +y\hat{j} +z\hat{k} , \vec{n}{1} = \hat{i} +\hat{j} +\hat{k} , \vec{n}{2} = 2\hat{i} - 3\hat{j} +5\hat{k} , d*{1} = 1 , d*{2} = - 2 in the above equation, we get

(x + y + z + 1) + \lambda (2x - 3y + 5z - 2) = 0

XII - Mathematics

Since this plane passes through the point (- 1,2,1) , we get \lambda = \frac{3}{5} , and hence the required equation of the plane is 11x - 4y + 20z = 1 .

Example 6.54

Find the equation of the plane passing through the intersection of the planes 2x + 3y - z + 7 = 0 and x + y - 2z + 5 = 0 and is perpendicular to the plane x + y - 3z - 5 = 0 .

Solution

The equation of the plane passing through the intersection of the planes 2x + 3y - z + 7 = 0 and x + y - 2z + 5 = 0 is \left(2x + 3y - z + 7\right) + \lambda \left(x + y - 2z + 5\right) = 0 or

\left(2 + \lambda\right)x + \left(3 + \lambda\right)y + \left(-1 - 2\lambda\right)z + \left(7 + 5\lambda\right) = 0

since this plane is perpendicular to the given plane x + y - 3z - 5 = 0 , the normals of these two planes are perpendicular to each other. Therefore, we have

(1)\left(2 + \lambda\right) + (1)\left(3 + \lambda\right) + (-3)\left(-1 - 2\lambda\right) = 0

which implies that \lambda = - 1 . Thus the required equation of the plane is

\left(2x + 3y - z + 7\right) - \left(x + y - 2z + 5\right) = 0\Rightarrow x + 2y + z + 2 = 0.

6.9 Image of a Point in a Plane

Let A be the given point whose position vector is \vec{u} . Let \vec{r}\cdot \vec{n} = p be the equation of the plane. Let \vec{v} be the position vector of the mirror image A^{\prime} of A in the plane. Then \overline{{A A^{\prime}}} is perpendicular to the plane. So it is parallel to \vec{n} . Then

\overline{{A A^{\prime}}} = \lambda \vec{n} \text{ or } \vec{v} -\vec{u} = \lambda \vec{n}\Rightarrow \vec{v} = \vec{u} +\lambda \vec{n} \quad (1)

Let M be the middle point of A A^{\prime} . Then the position vector of M is \frac{\vec{u} + \vec{v}}{2} . But M lies on the plane.

\text{So},\quad \left(\frac{\vec{u} + \vec{v}}{2}\right)\cdot \vec{n} = p. \quad (2)

Substituting (1) in (2), we get

\left(\frac{\vec{u} + \lambda\vec{n} + \vec{u}}{2}\right)\cdot \vec{n} = p\Rightarrow \lambda = \frac{2\left[p - (\vec{u}\cdot\vec{n})\right]}{|\vec{n}|^{2}}

Therefore, the position vector of A^{\prime}

\text{is } \vec{v} = \vec{u} +\frac{2[p - (\vec{u}\cdot\vec{n})]}{|\vec{n}|^{2}}

Fig.6.35

Note

The mid point of M of A A^{\prime} is the foot of the perpendicular from the point A to the plane \vec{r}\cdot \vec{n} = p . So the position vector of the foot M of the perpendicular is given by.

\frac{\vec{u} + \vec{v}}{2} = \frac{\vec{u}}{2} +\frac{1}{2}\left(\vec{u} +\frac{2[p - (\vec{u}\cdot\vec{n})]}{|\vec{n}|^{2}}\vec{n}\right)

6.9.1 The coordinates of the image of a point in a plane

Let (a*{1},a*{2},a*{3}) be the point \vec{u} whose image in the plane is required. Then \vec{u} = a*{1}\hat{i} +a*{2}\hat{j} +a*{3}\hat{k} .

Let a x + b y + c z = d be the equation of the given plane. Writing the equation in the vector form we get \vec{r}\cdot \vec{n} = p where \vec{n} = a\vec{i} +b\vec{j} +c\vec{k} . Then the position vector of the image is

\vec{v} = \vec{u} +\frac{2\big[p - (\vec{u}\cdot\vec{n})\big]}{|\vec{n}|^{2}}\vec{n}.

If \vec{v} = \nu*{1}\hat{i} +\nu*{2}\hat{j} +\nu*{3}\hat{k} , then \nu*{1} = a*{1} + 2a\alpha , \nu*{2} = a*{2} + 2a\alpha , \nu*{3} = a_{3} + 2a\alpha

\text{where } \alpha = \frac{2\big[p - (a a_{1} + b a_{2} + c a_{3})\big]}{a^{2} + b^{2} + c^{2}}.

Example 6.55

Find the image of the point whose position vector is \vec{i} +2\vec{j} +3\vec{k} in the plane \vec{r}\cdot \left(\vec{i} +2\vec{j} +4\vec{k}\right) = 38 .

Solution

Here, \vec{u} = \hat{i} +2\hat{j} +3\hat{k} , \vec{n} = \hat{i} +2\hat{j} +4\hat{k} , p = 38 . Then the position vector of the image \vec{v} of

\vec{u} = \hat{i} +2\hat{j} +3\hat{k} is given by \vec{v} = \vec{u} +\frac{2\big[p - (\vec{u}\cdot\vec{n})\big]}{|\vec{n}|^{2}}\vec{n}.

\vec{v} = \left(\hat{i} +2\hat{j} +3\hat{k}\right) + \frac{2\left[38 - \left(\left(\hat{i} +2\hat{j} +3\hat{k}\right)\cdot \left(\hat{i} +2\hat{j} +4\hat{k}\right)\right)\right]}{\left(\hat{i} +2\hat{j} +4\hat{k}\right)\cdot\left(\hat{i} +2\hat{j} +4\hat{k}\right)}\left(\hat{i} +2\hat{j} +4\hat{k}\right).

That is, \vec{v} = \left(\hat{i} +2\hat{j} +3\hat{k}\right) + 2\left(\frac{38 - 17}{21}\right)\left(\hat{i} +2\hat{j} +4\hat{k}\right) = 3\hat{i} +6\hat{j} +11\hat{k} .

Therefore, the image of the point with position vector \hat{i} +2\hat{j} +3\hat{k} is 3\hat{i} +6\hat{j} +11\hat{k} .

Note

The foot of the perpendicular from the point with position vector \hat{i} +2\hat{j} +3\hat{k} in the given plane is

\frac{(\hat{i} +2\hat{j} +3\hat{k}) + (3\hat{i} +6\hat{j} +11\hat{k})}{2} = 2\hat{i} +4\hat{j} +7\hat{k}.

6.10 Meeting Point of a Line and a Plane

Theorem 6.23

The position vector of the point of intersection of the straight line \vec{r} = \vec{a} +t\vec{b} and the plane \vec{r}\cdot \vec{n} = p is \vec{a} +\left(\frac{p - (\vec{a}\cdot\vec{n})}{\vec{b}\cdot\vec{n}}\right)\vec{b} , provided \vec{b}\cdot \vec{n}\neq 0 .

Proof

Let \vec{r} = \vec{a} +t\vec{b} be the equation of the given line which is not parallel to the given plane whose equation is \vec{r}\cdot \vec{n} = p . So, \vec{b}\cdot \vec{n}\neq 0 .

EXERCISE 6.9

1. Find the equation of the plane passing through the line of intersection of the planes \vec{r}\cdot \left(2\vec{i} -7\vec{j} +4\vec{k}\right) = 3 and 3x - 5y + 4z + 11 = 0 , and the point (-2,1,3) .

2. Find the equation of the plane passing through the line of intersection of the planes x + 2y + 3z = 2 and x - y + z = 3 , and at a distance \frac{2}{\sqrt{3}} from the point (3,1, - 1) .

3. Find the angle between the line \vec{r} = \left(2\vec{i} - \vec{j} +\vec{k}\right) + t\left(\vec{i} +2\vec{j} -2\vec{k}\right) and the plane \vec{r}\cdot \left(6\vec{i} +3\vec{j} +2\vec{k}\right) = 8

4. Find the angle between the planes \vec{r}\cdot \left(\vec{i} +\vec{j} -2\vec{k}\right) = 3 and 2x - 2y + z = 2 .

5. Find the equation of the plane which passes through the point (3,4, - 1) and is parallel to the plane 2x - 3y + 5z + 7 = 0 . Also, find the distance between the two planes.

6. Find the length of the perpendicular from the point (1, - 2,3) to the plane x - y + z = 5 .

7. Find the point of intersection of the line x - 1 = \frac{y}{2} = z + 1 with the plane 2x - y + 2z = 2 . Also, find the angle between the line and the plane.

8. Find the coordinates of the foot of the perpendicular and length of the perpendicular from the point (4,3,2) to the plane x + 2y + 3z = 2 .

EXERCISE 6.10

Choose the correct or the most suitable answer from the given four alternatives:

1. If \vec{a} and \vec{b} are parallel vectors, then [\vec{a},\vec{c},\vec{b}] is equal to

   (1) 2 (2) -1 (3) 1 (4) 0

2. If a vector \vec{a} lies in the plane of \vec{\beta} and \vec{\gamma} , then

   [\vec{a},\vec{\beta},\vec{\gamma}] = 1\qquad (2)[\vec{a},\vec{\beta},\vec{\gamma}] = -1\qquad (3)[\vec{a},\vec{\beta},\vec{\gamma}] = 0\qquad (4)[\vec{a},\vec{\beta},\vec{\gamma}] = 2

3. If \vec{a}\cdot \vec{b} = \vec{b}\cdot \vec{c} = \vec{c}\cdot \vec{a} = 0 , then the value of [\vec{a},\vec{b},\vec{c}] is

   (1)|\vec{a}||\vec{b}||\vec{c}|\qquad (2)\frac{1}{3} |\vec{a}||\vec{b}||\vec{c}|\qquad (3)1 \quad (4) -1

4. If \vec{a},\vec{b},\vec{c} are three unit vectors such that \vec{a} is perpendicular to \vec{b} , and is parallel to \vec{c} then \vec{a}\times (\vec{b}\times \vec{c}) is equal to

   (1)\vec{a}\qquad (2)\vec{b}\qquad (3)\vec{c}\qquad (4)\vec{0}

5. If [\vec{a},\vec{b},\vec{c}] = 1 , then the value of \frac{\vec{a}\cdot(\vec{b}\times\vec{c})}{(\vec{c}\times\vec{a})\cdot\vec{b}} +\frac{\vec{b}\cdot(\vec{c}\times\vec{a})}{(\vec{a}\times\vec{b})\cdot\vec{c}} +\frac{\vec{c}\cdot(\vec{a}\times\vec{b})}{(\vec{c}\times\vec{b})\cdot\vec{a}} is

   (1) 1 (2) -1 (3) 2 (4) 3

6. The volume of the parallelepiped with its edges represented by the vectors \vec{i} +\vec{j} , \vec{i} +2\vec{j} , \vec{i} +\vec{j} +\pi \vec{k} is

   (1)\frac{\pi}{2}\qquad (2)\frac{\pi}{3}\qquad (3)\pi \qquad (4)\frac{\pi}{4}

7. If \vec{a} and \vec{b} are unit vectors such that [\vec{a},\vec{b},\vec{a}\times \vec{b}] = \frac{1}{4} , then the angle between \vec{a} and \vec{b} is

   (1)\frac{\pi}{6}\qquad (2)\frac{\pi}{4}\qquad (3)\frac{\pi}{3}\qquad (4)\frac{\pi}{2}

8. If \vec{a} = \hat{i} +\hat{j} +\hat{k} , \vec{b} = \hat{i} +\hat{j} , \vec{c} = \hat{i} and (\vec{a}\times \vec{b})\times \vec{c} = \lambda \vec{a} +\mu \vec{b} , then the value of \lambda +\mu is

   (1) 0 (2) 1 (3) 6 (4) 3

9. If \vec{a},\vec{b},\vec{c} are non-coplanar, non-zero vectors such that [\vec{a},\vec{b},\vec{c} ] = 3 , then [\vec{a}\times \vec{b},\vec{b}\times \vec{c},\vec{c}\times \vec{a} ]^{2} is equal to

   (1) 81 (2) 9 (3) 27 (4) 18

10. If \vec{a},\vec{b},\vec{c} are three non-coplanar unit vectors such that \vec{a}\times (\vec{b}\times \vec{c}) = \frac{\vec{b} + \vec{c}}{\sqrt{2}} , then the angle between \vec{a} and \vec{b} is

    (1) \frac{\pi}{2} (2) \frac{3\pi}{4} (3) \frac{\pi}{4} (4) \pi

11. If the volume of the parallelepiped with \vec{a}\times \vec{b}, \vec{b}\times \vec{c}, \vec{c}\times \vec{a} as coterminous edges is 8 cubic units, then the volume of the parallelepiped with (\vec{a}\times \vec{b})\times (\vec{b}\times \vec{c}),(\vec{b}\times \vec{c})\times (\vec{c}\times \vec{a}) and (\vec{c}\times \vec{a})\times (\vec{a}\times \vec{b}) as coterminous edges is,

    (1) 8 cubic units (2) 512 cubic units (3) 64 cubic units (4) 24 cubic units

12. Consider the vectors \vec{a},\vec{b},\vec{c},\vec{d} such that (\vec{a}\times \vec{b})\times (\vec{c}\times \vec{d}) = \vec{0} . Let P*{1} and P*{2} be the planes determined by the pairs of vectors \vec{a},\vec{b} and \vec{c},\vec{d} respectively. Then the angle between P*{1} and P*{2} is

    (1) 0^{\circ} (2) 45^{\circ} (3) 60^{\circ} (4) 90^{\circ}

13. If \vec{a}\times (\vec{b}\times \vec{c}) = (\vec{a}\times \vec{b})\times \vec{c} , where \vec{a},\vec{b},\vec{c} are any three vectors such that \vec{b}\cdot \vec{c}\neq 0 and \vec{a}\cdot \vec{b}\neq 0 then \vec{a} and \vec{c} are

    (1) perpendicular (2) parallel (3) inclined at an angle \frac{\pi}{3} (4) inclined at an angle \frac{\pi}{6}

14. If \vec{a} = 2\hat{i} +3\hat{j} -\hat{k}, \vec{b} = \hat{i} +2\hat{j} -5\hat{k}, \vec{c} = 3\hat{i} +5\hat{j} -\hat{k}, then a vector perpendicular to \vec{a} and lies in the plane containing \vec{b} and \vec{c} is

    (1) -17\hat{i} +21\hat{j} -97\hat{k} (3) -17\hat{i} -21\hat{j} +97\hat{k}

15. The angle between the lines \frac{x - 2}{3} = \frac{y + 1}{-2},z = 2 and \frac{x - 1}{1} = \frac{2y + 3}{3} = \frac{z + 5}{2} is

    (1) \frac{\pi}{6} (2) \frac{\pi}{4} (3) \frac{\pi}{3} (4) \frac{\pi}{2}

16. If the line \frac{x - 2}{3} = \frac{y - 1}{-5} = \frac{z + 2}{2} lies in the plane x + 3y - \alpha z + \beta = 0 , then (\alpha ,\beta) is (1) (-5,5) (2) (-6,7) (3) (5, -5) (4) (6, -7)

17. The angle between the line \vec{r} = (\hat{i} +2\hat{j} -3\hat{k}) + t(2\hat{i} +\hat{j} -2\hat{k}) and the plane \vec{r}\cdot (\hat{i} +\hat{j}) + 4 = 0 is

    (1) 0^{\circ} (2) 30^{\circ} (3) 45^{\circ} (4) 90^{\circ}

18. The coordinates of the point where the line \vec{r} = (6\hat{i} -\hat{j} -3\hat{k}) + t(-\hat{i} +4\hat{k}) meets the plane \vec{r}.(\hat{i} +\hat{j} -\hat{k}) = 3 are

    (1) (2,1,0) \qquad (2) (7, -1, -7) \qquad (3) (1,2, -6) \qquad (4) (5, -1,1)

19. Distance from the origin to the plane 3x - 6y + 2z + 7 = 0 is

    (1) 0 (2) 1 (3) 2 (4) 3

20. The distance between the planes x + 2y + 3z + 7 = 0 and 2x + 4y + 6z + 7 = 0 is

    (1) \frac{\sqrt{7}}{2\sqrt{2}} (2) \frac{7}{2} (3) \frac{\sqrt{7}}{2} (4) \frac{7}{2\sqrt{2}}

21. If the direction cosines of a line are \frac{1}{c}, \frac{1}{c}, \frac{1}{c} , then

    (1) c = \pm 3 (2) c = \pm \sqrt{3} (3) c > 0 (4) 0< c< 1

22. The vector equation \vec{r} = (\hat{i} -2\hat{j} -\hat{k}) + t(6\hat{j} -\hat{k}) represents a straight line passing through the points

    (1) (0,6, -1) and (1, -2, -1) (2) (0,6, -1) and (-1, -4, -2) (3) (1, -2, -1) and (1,4, -2) (4) (1, -2, -1) and (0, -6,1)

23. If the distance of the point (1,1,1) from the origin is half of its distance from the plane x + y + z + k = 0 , then the values of k are

    (1) \pm 3 (2) \pm 6 (3) -3,9 (4) 3, -9

24. If the planes \vec{r}.(2\hat{i} -\lambda \hat{j} +\hat{k}) = 3 and \vec{r}.(4\hat{i} +\hat{j} -\mu \hat{k}) = 5 are parallel, then the value of \lambda and \mu are

    (1) \frac{1}{2}, -2 (2) -\frac{1}{2},2 (3) -\frac{1}{2}, -2 (4) \frac{1}{2},2

25. If the length of the perpendicular from the origin to the plane 2x + 3y + \lambda z = 1 , \lambda > 0 is \frac{1}{5} , then the value of \lambda is

    (1) 2\sqrt{3} (2) 3\sqrt{2} (3) 0 (4) 1

Fig. 6.9: Diagram illustrating scalar triple product as volume of parallelepiped

1. For a given set of three vectors \vec{a},\vec{b} and \vec{c} , the scalar (\vec{a}\times \vec{b})\cdot \vec{c} is called a scalar triple product of \vec{a},\vec{b},\vec{c} .

2. The volume of the parallelepiped formed by using the three vectors \vec{a},\vec{b} , and \vec{c} as co-terminus edges is given by \left|(\vec{a}\times \vec{b})\cdot \vec{c}\right| .

3. The scalar triple product of three non-zero vectors is zero if and only if the three vectors are coplanar.

4. Three vectors \vec{a},\vec{b},\vec{c} are coplanar, if, and only if there exist scalars r,s,t\in \mathbb{R} such that atleast one of them is non-zero and r\vec{a} +s\vec{b} +t\vec{c} = \vec{0} .

5. If \vec{a},\vec{b},\vec{c} and \vec{p},\vec{q},\vec{r} are any two systems of three vectors, and if \vec{p} = x*{1}\vec{a} +y*{1}\vec{b} +z_{1}\vec{c}

6. For a given set of three vectors \vec{a},\vec{b},\vec{c} , the vector \vec{a}\times (\vec{b}\times \vec{c}) is called vector triple product.

7. For any three vectors \vec{a},\vec{b},\vec{c} we have \vec{a}\times (\vec{b}\times \vec{c}) = (\vec{a}\cdot \vec{c})\vec{b} -(\vec{a}\cdot \vec{b})\vec{c} .

8. Parametric form of the vector equation of a straight line that passes through a given point with position vector \vec{a} and parallel to a given vector \vec{b} is \vec{r} = \vec{a} +t\vec{b} , where t\in \mathbb{R} .

9. Cartesian equations of a straight line that passes through the point (x*{1},y*{1},z*{1}) and parallel to a vector with direction ratios b*{1},b*{2},b*{3} are \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} .

10. Any point on the line \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} is of the form (x*{1} + t b*{1},y*{1} + t b*{2},z*{1} + t b*{3}),t\in \mathbb{R} .

11. Parametric form of vector equation of a straight line that passes through two given points with position vectors \vec{a} and \vec{b} is \vec{r} = \vec{a} +t(\vec{b} - \vec{a}),t\in \mathbb{R} .

12. Cartesian equations of a line that passes through two given points (x*{1},y*{1},z*{1}) and (x*{2},y*{2},z*{2}) are \frac{x - x*{1}}{x*{2} - x*{1}} = \frac{y - y*{1}}{y*{2} - y*{1}} = \frac{z - z*{1}}{z*{2} - z_{1}} .

13. If \theta is the acute angle between two straight lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} , then

    \cos \theta = \left| \frac{\vec{b} \cdot \vec{d}}{|\vec{b}| |\vec{d}|} \right|

14. Two lines are said to be coplanar if they lie in the same plane.

15. Two lines in space are called skew lines if they are not parallel and do not intersect

16. The shortest distance between the two skew lines is the length of the line segment perpendicular to both the skew lines.

17. The shortest distance between the two skew lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} is

    \delta = \frac{\left|(\vec{c} - \vec{a})\cdot(\vec{b}\times \vec{d})\right|}{\left|\vec{b}\times \vec{d}\right|},\mathrm{where}\left|\vec{b}\times \vec{d}\right|\neq 0.

18. Two straight lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} intersect each other if \left(\vec{c} -\vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

19. The shortest distance between the two parallel lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{b} is d = \frac{\left|\left(\vec{c} - \vec{a}\right)\times\vec{b}\right|}{\left|\vec{b}\right|}} where |\vec{b}|\neq 0

20. If two lines \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} intersect, then

    \begin{vmatrix} x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

21. A straight line which is perpendicular to a plane is called a normal to the plane.

22. The equation of the plane at a distance p from the origin and perpendicular to the unit normal vector \vec{d} is \vec{r}\cdot \vec{d} = p (normal form)

23. Cartesian equation of the plane in normal form is l x + m y + n z = p

24. Vector form of the equation of a plane passing through a point with position vector \vec{a} and perpendicular to \vec{n} is (\vec{r} -\vec{a})\cdot \vec{n} = 0

25. Cartesian equation of a plane normal to a vector with direction ratios a,b,c and passing through a given point (x*{1},y*{1},z*{1}) is a\left(x - x*{1}\right) + b\left(y - y*{1}\right) + c\left(z - z*{1}\right) = 0

26. Intercept form of the equation of the plane \vec{r}\cdot \vec{n} = q , having intercepts a,b,c on the x,y,z axes respectively is \frac{x}{a} +\frac{y}{b} +\frac{z}{c} = 1

27. Parametric form of vector equation of the plane passing through three given non-collinear points is \vec{r} = \vec{a} +s\left(\vec{b} -\vec{a}\right) + t\left(\vec{c} -\vec{a}\right)

28. Cartesian equation of the plane passing through three non-collinear points (x_1, y_1, z_1), (x_2, y_2, z_2), and (x_3, y_3, z_3) is

    \begin{vmatrix} x - x_1 & y - y_1 & z - z_1 \ x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ x_3 - x_1 & y_3 - y_1 & z_3 - z_1 \end{vmatrix} = 0

29. A straight will lie on a plane if every point on the line, lie in the plane and the normal to the plane is perpendicular to the line.

30. The two given non-parallel lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} are coplanar if \left(\vec{c} -\vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

31. Two lines \frac{x - x*{1}}{b*{1}} = \frac{y - y*{1}}{b*{2}} = \frac{z - z*{1}}{b*{3}} and \frac{x - x*{2}}{d*{1}} = \frac{y - y*{2}}{d*{2}} = \frac{z - z*{2}}{d*{3}} are coplanar if

    \begin{vmatrix} x_2 - x_1 & y_2 - y_1 & z_2 - z_1 \ b_1 & b_2 & b_3 \ d_1 & d_2 & d_3 \end{vmatrix} = 0

32. Non-parametric form of vector equation of the plane containing the two coplanar lines \vec{r} = \vec{a} +s\vec{b} and \vec{r} = \vec{c} +t\vec{d} is \left(\vec{r} -\vec{a}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0 or \left(\vec{r} -\vec{c}\right)\cdot \left(\vec{b}\times \vec{d}\right) = 0

33. The acute angle \theta between the two planes \vec{r}\cdot \vec{n}{1} = p{1} and \vec{r}\cdot \vec{n}{2} = p{2} is \theta = \cos^{-1}\left(\frac{|\vec{n}{1}\cdot \vec{n}{2}|}{|\vec{n}_1||\vec{n}_2|}\right)

34. If \theta is the acute angle between the line \vec{r} = \vec{a} +t\vec{b} and the plane \vec{r}\cdot \vec{n} = p , then \theta = \sin^{-1}\left(\frac{|\vec{b}\cdot\vec{n}|}{|\vec{b}||\vec{n}|}\right)

35. The perpendicular distance from a point with position vector \vec{u} to the plane \vec{r}\cdot \vec{n} = p is given by

    \delta = \frac{|\vec{u}\cdot\vec{n} - p|}{|\vec{n}|}

36. The perpendicular distance from a point (x*{1},y*{1},z_{1}) to the plane ax + by + cz = p is

    \delta = \frac{|ax*{1} + by*{1} + cz_{1} - p|}{\sqrt{a^{2} + b^{2} + c^{2}}}.

37. The perpendicular distance from the origin to the plane ax + by + cz + d = 0 is given by

    \delta = \frac{|d|}{\sqrt{a^{2} + b^{2} + c^{2}}}

38. The distance between two parallel planes ax + by + cz + d*{1} = 0 and ax + by + cz + d*{2} = 0 is given by \frac{|d*{1} - d*{2}|}{\sqrt{a^{2} + b^{2} + c^{2}}}.

39. The vector equation of a plane which passes through the line of intersection of the planes \vec{r}\cdot \vec{n}{1} = d{1} and \vec{r}\cdot \vec{n}{2} = d{2} is given by (\vec{r}\cdot \vec{n}{1} - d{1}) + \lambda (\vec{r}\cdot \vec{n}{2} - d{2}) = 0 , where \lambda \in \mathbb{R} is an arbitrary constant.

40. The equation of a plane passing through the line of intersection of the planes a*{1}x + b*{1}y + c*{1}z = d*{1} and a*{2}x + b*{2}y + c*{2}z = d*{2} is given by

    (a*{1}x + b*{1}y + c*{1}z - d*{1}) + \lambda (a*{2}x + b*{2}y + c*{2}z - d*{2}) = 0

41. The position vector of the point of intersection of the line \vec{r} = \vec{a} +t\vec{b} and the plane \vec{r}\cdot \vec{n} = p is obtained by solving for t from (\vec{a} + t\vec{b})\cdot \vec{n} = p.

42. If \vec{v} is the position vector of the image of \vec{u} in the plane \vec{r}\cdot \vec{n} = p , then

    \vec{v} = \vec{u} +\frac{2\left[p - \left(\vec{u}\cdot\vec{n}\right)\right]}{|\vec{n}|^{2}}\vec{n}.

ICT CORNER

Step 1: Open the Browser and type the URL: https://ggbm.at/vchq92pg or Scan the QR Code.

Step 2: A GeoGebra workbook named “12th Standard Mathematics” will open.

Step 3: In the left side of the work book there are many chapters related to your text book. Click on the chapter named “Applications of Vector Algebra”.

Step 4: You can see several work sheets related to the chapter. Select the work sheet “Scalar Triple Product”.

Fig. ICT 1: GeoGebra interface for Scalar Triple Product