Physical quantities are divided into two categories – scalar and vector quantities. The quantities which have only magnitude and not any fixed direction are called Scalar quantities. Eg. Mass, volume, density, etc. Quantities that have both magnitude and direction. Such quantities are called vector quantities or vectors. Eg. Displacement, velocity, acceleration, momentum, etc.
Vectors are represented by line segments that are directed such as, the direction of an arrow marked at one end, which denotes direction and the length of the line segment is the magnitude of the vector. Eg.
It denotes two points A and B, such that the magnitude of the vector is the length of the straight line AB and its direction is from A to B. Here, point A is called the initial point of vector
The magnitude or modulus of a vector \overrightarrow{AB} is a positive number(>0) which is the measure of its length and is denoted by |\overrightarrow{AB}|.
Types of Vectors
Zero Vector
A vector whose initial and terminal(end) points coincide with each other, is called a zero vector (or null vector), and denoted as
The vectors
Unit Vector
A vector whose magnitude is unity (=1) is called as unit vector. The unit vector
and
Coinitial Vectors
Two or more vectors having the same initial point or starting point are called coinitial vectors.
Collinear Vectors
If two or more vectors are parallel to each other, irrespective of their magnitudes and directions. Then they will be called collinear vectors.
Equal Vectors
If two vectors
Negative of a Vector
A vector whose magnitude(length) is equal to of given vector (say
For example, vector
Position Vector
Consider a point P in 3D space, having coordinates as (x, y, z) with respect to the origin O(0, 0, 0). And, the vector
Using the distance formula, the magnitude(or length) of
Note: The vector’s definition defined above are such type of vectors that can be subjected to its parallel displacement without changing its magnitude and direction. Such vectors are called free vectors.
Vector Addition
A vector
Triangle law of vector addition
Consider a situation that a person moves from A to B and then from B to C. The net displacement made by the person from point A to point C, is given by the vector and expressed as
This is known as the triangle law of vector addition.
As,
When the sides of a triangle are taken in order, then it leads to zero resultant(no displacement result) as the initial and terminal points get coincided with each other.
Parallelogram Law of Vector Addition
If two vectors
Now, let’s consider the parallelogram ABCD
where,
and then by using the triangle law of vector addition, from triangle ABC, we have
………………….(1) Now, as the opposite sides of a parallelogram are equal and parallel
and Again using triangle law of vector addition, from triangle ADC, we have
…………………………….(2) From (1) and (2), we get commutative property
Note: The magnitude
is not equal to the sum of the magnitude(length) of and .
(ii) Associative property
Using triangle law, from triangle PQR, we have
Using triangle law, from triangle QRS, we have
Using triangle law, from triangle PRS, we have
Using triangle law, from triangle PQS, we have
Hence,
(iii) Additive identity
For any vector
(iv) Additive inverse
For any vector
Problem 1: If
Solution:
We have,
Using, converse of triangle law of addition of vectors, we get
and ae either parallel or collinear. But, Q is a point common to them. So,
and are collinear. Hence, points P, Q, R are collinear.
Problem 2: B, P, Q, R and A are five points in a plane. Show that the sum of vectors
Solution:
Using triangle law addition of vectors in △APB
……………(1) Using triangle law addition of vectors in △AQB
…………………..(2) Using triangle law addition of vectors in △ARB
…………….(3) Adding (1), (2) and (3), we get
Hence, the sum of the vectors is 3
Problem 3: Let O be the centre of a regular hexagon CDEFAB. Find the sum of the vectors
Solution:
As hexagon property states that, the centre of a regular hexagon bisects all the diagonals passing through it.
So,
and
………………..(1)
…………………..(2)
…………………..(3) By adding (1), (2) and (3), we get
Section formula
Here, the points P and Q are the two points represented by the position vectors
Here, we intend to find the position vector
Internally
When R divides PQ internally. If R divides
such that
where m and n are positive values, we specify that the point R divides
internally in the ratio of m : n. Now from triangles ORQ and OPR, we have
Hence, we can conclude that,
m
= n On simplification, we get
When R is the midpoint PQ
then m = n
So, we get
Externally
When R divides PQ externally. If R divides
such that
where m and n are positive values, we say that the point R divides
externally in the ratio of the m : n. Now from triangles ORQ and OPR, we have
Hence, we can conclude that,
On simplification, we get
Problem 1: Find the position vectors of the points which divide the join of the points
Solution:
Let A and B be the given points with the position vectors
and respectively. Let P divide the
in the ratio 2 : 3 internally m = 2 and n = 3
Using internally section formula,
Position vector of P =
Position vector of P =
Position vector of P =
Position vector of P =
Now, Let P divide the
in the ratio 2 : 3 externally m = 2 and n = 3
Using externally section formula,
Position vector of P =
Position vector of P =
Position vector of P =
Position vector of P =
Problem 2: If
Solution:
Let P and Q be points of trisection. Then, AP = PQ = QB = k (constant variable)
PB = PQ + QB = k + k = 2k
P divides AB in the ratio 1 : 2
Using internally section formula, where m=1 and n=2
Position vector of P =
Position vector of P =
Position vector of P =
Now, we can clearly see that Q is the mid-point of PB.
Apply mid-point section formula we have,
Position vector of Q =
Position vector of Q =
Position vector of Q =
Problem 3: If D is the mid-point of the side BC of a triangle ABC, prove that
Solution:
Let A be the origin here and position vectors of B and C be
and respectively. As D is the mid-point of BC.
Applying mid-point section formula, we get
Position vector of D =
As,
Hence, Proved!!
Components of a vector
Let’s take the points A(1, 0, 0), B(0, 1, 0) and C(0, 0, 1) on the x-axis, y-axis and z-axis, respectively. Then,
The vectors,
Lets, consider the position vector
Hence we see that P1P is parallel to z-axis. As
Using triangle law, from triangle OQP1, we have
Using triangle law, from triangle OP1P, we have
Hence, the position vector of P with reference to O is as follows:
Length
The length of vector
, OP12 = OQ2 + QP12 (Using Pythagoras theorem)
OP12 = x2 + y2
and in the right-angled triangle OP1 P, we have
OP2 = OP12 + PP12
OP2 = x2 + y2 + z2
OP =
Hence, the length of vector
If
Sum
Difference
The vectors
, iff a1 = a2, b1 = b2 and c1 = c2
The multiplication of vector by any scalar k is given by
Vector joining two points
If P(x1, y1, z1) and Q(x2, y2, z2) are any two points, then the vector joining P and Q is the vector
Joining the points P and Q with the origin O, and applying triangle law, from the triangle OPQ, we have
Using the properties of vector addition, the above equation become
Hence, the magnitude of
is as follows:
Problem 1: Find the value of x, y and z so that the vectors
Solution:
Two vectors
and are equal iff a1 = a2 , b1 = b2 and c1 = c2
Hence, the values of x = 2, y = 2 and z =1.
Problem 2: Find the magnitude of the vector
Solution:
As, we have
= 7
Problem 3: Find the unit vector of given vector as
Solution:
Let,
= 7 So, the unit vector in the direction of
is given by,
Problem 4: Find the unit vector of given vector as
Solution:
Position vector of P(1,2,3) =
Position vector of Q(4,5,6) =
= –
Now, magnitude of
= 3√3 So, the unit vector in the direction of
is given by,
Problem 5: Show that the vector
Solution:
Let,
and As, we can see
This implies,
Hence,
and are collinear.
Problem 6: If A(2,0,0), B(0,1,0), C (0,0,2) have position vectors, show that △ABC is isosceles triangle.
Solution:
Position vector of A(2,0,0) =
Position vector of B(0,1,0) =
Position vector of C(0,0,2) =
=
Now, magnitude of
=
Now, magnitude of
Clearly, AB = BC.
Hence, △ABC is isosceles triangle.