https://docs.google.com/document/d/1QE3SLNu1ADZUg34K4p5T-y7gU0G_V_P2/edit?usp=sharing&ouid=109474854956598892099&rtpof=true&sd=true
Matrices and Determinants
Matrices, Algebra of matrices, Types of matrices, Determinants & matrices of order two & three. Properties of determinants, Eva lua tion of determinants, Area of triangles using determinants. Adjoint & evaluation of inverse of a squa re matrix using determina nts & e l ementary transformations, Test of consistency & solution of simultaneous linear
equations in two or three variables using determinants and matrices.
Matrices and determinants are two very important tools in the hands of a mathematician. These have wide application in algebra, trigonometry, co-ordinate geometry & calculus. Problems can be handled in a much simplified way and lot-
many calculations are cut short.
DETERMINANTS OF 2ND & 3RD ORDER
C H A P T E R
CHAPTER INCLUDES :
Determinants of 2 nd
& 3rd order
Minors and Cofactors
a1
The symbol a2
b1
b2 is called a determinant of order 2. It has two rows and
Properties for evaluation of determinants
two columns. a b – a b
a1 b1
is called expansion of determinant . These
Determinant of
1 2 2 1
a2 b2
cofactors
idea can be extended to higher order determinants.
Determinant of 3rd order
Multiplication of determinants
Area of triangle
System of linear
a11
The symbol Δ = a21
a31
a12 a22 a32
a13 a23 a33
= | aij | is called the determinant of 3rd order
equations
Cramer's rule
Matrices
and its value is equal to the number:
Types of matrices
Algebra of matrices
(−1)1+1a
a22
a23
+ (−1)1+2a
a21
a23
+ (−1)1+3 a
a21
a22
Adjoint of matrix
11 a32
a33
12 a31
a33
13 a31
a32
Inverse of matrix
= a (a a
a a
) − a (a a
a a
) + a (a a
a a
) ...(A)
Solution of
11 22 33
23 32
12 21 33
31 23
13 21 32
31 22
simultaneous linear equations
is called expansion of determinant Δ along its first row. In fact, expansion can be carried along any row or column in a simmilar way.
Solved examples
MINORS AND CO-FACTORS OF DETERMINANT
In the determinant Δ, the minor of the element aij (where i denotes number of row and j the number of columns,
i.e., element common to ith row and jth column) is obtained by removing the ith row and jth column and it is given by
Mij
and
For example, M12 =
a21 a31
a23 a33
cofactor of a
is defined as C
= (–1)i + j M , for example, C
= (–1)1+2
a21
a23
or C12
ij
= − a21
a31
ij ij
a23 .
a33
12 a31
a33
We can also express Δ as follows :
Δ = a11 C11 + a12 C12 + a13 C13 or Δ = a21 C21 + a22 C22 + a23 C23 or Δ = a31 C31 + a32 C32 + a33 C33
Notations for operations performed on rows/columns of determinants
Ri (i = 1, 2, 3) and Cj (j = 1, 2, 3) are used to denote ith row and jth column respectively.
The interchange of ith row and jth row : Ri ←→ Rj
The addition of m times the element of ith row to the corresponding elements of jth row :
Rj ⎯→ Rj + mRi
The addition of m times the element of jth row and n times the element of kth row to the corresponding element of ith row :
Ri ⎯→ Rj + mRj + nRk
(Similar operation can be performed with respect to columns of Δ)
PROPERTIES FOR EVALUATION OF DETERMINANTS
The value of determinant is not changed when all rows and columns are interchanged i.e.,
a1 b1 c1 a1 a2 a3
a2 b2 c2 = b1 b2 b3
a3 b3 c3 c1 c2 c3
If any two rows (or any two columns) of a determinant are interchanged, the sign of the determinant is
changed, but its value remains same (numerically),
a1
a2
b1
b2
c1
c2 = −
c1
c2
b1
b2
a1
a2
a3
b3
c3
c3
b3
a3
If all the elements of the same row (or the same column) are multiplied by a number, then the determinant (its value) becomes multiplied by the number
ma1 a2 a3
mb1 b2 b3
mc1 c2
c3
a1
= m a2
a3
b1 c1
b2 c2
b3 c3
If any two rows (or columns) are identical or their respective elements are proportional the the value of a determinant is zero.
a1 ma1
a2 ma2
a3 ma3
c1
c2 = 0
c3
The value of a determinant does not change when any row (or column) is multiplied by a number or an expression and is added to or subtracted from any other row (or column)
a1 b1
c1 a1
b1 + m1c1 c1
a2 b2
c2 = a2
b2 + m1c2 c2
a3 b3
c3 a3
b3 + m1c3 c3
If every element of some row (or column) is the sum of two numbers, then determinant can be expressed as the sum of two determinants of the same order; one containing only the first number in place of sum, the other only the second number. The remaining element of both determinant are the same as in the given determinant.
a1 + α1 + β1
b1
c1
a1
b1
c1
α1
b1
c1
β1
b1
c1
a2 + α2 + β2
b2
c2
=
a2
b2
c2
+ α2
b2
c2
+ β2
b2
c2
a3 + α3 + β3
b3
c3
a3
b3
c3
α3
b3
c3
β3
b3
c3
(In this example, we have shown it for sum of three numbers)
Remarks :
The value of determinant remains unaltered under an operation of the form Ri ⎯→ Ri + mRj + nRk (j, k ≠ i). These operation enable us to convert maximum elements into zeros for making evaluation of determinant simpler.
If a determinant Δ(x) becomes zero on putting x = α, then x – α is a factor of Δ(x).
Determinant which have all elements equal to zero except the diagonal elements is equal to the product of the diagonal elements i.e.
a 0 0
0 b 0 = abc
0 0 c
Also
a α β a
0 b γ = α
0 0 c β
0 0
b 0 = abc
γ c
0 a
Determinant − a 0
b − c
b
c = 0. (note that upper triangular is reflected along diagonal with opposite sign)
0
Without expanding the determinant, prove that
a + b b + c c + a
b + c c + a a + b
c + a a + b b + c
a b c
= 2 b c a
c a b
Solution :
LHS =
2(a + b + c) 2 (a + b + c) 2(a + b + c)
b + c c + a a + b
c + a a + b b + c
(C1 → C1 + C2 + C3 )
a + b + c
= 2 a + b + c
a + b + c
b + c c + a a + b
c + a a + b b + c
(taking 2 common from 1st - column)
= 2
= 2
a
= 2 b c
b c
a
b + c
c + a
b
c + a
a + b (C1 → C1 – C2 )
c
a + b
b + c
a
b + c
c
c + a a (C3 → C3 – C1)
a + b b
c a (C2 → C2 – C3 )
a b
= RHS
DETERMINANT OF CO-FACTORS
If Δ ≠ 0 be the determinant and Δc denotes determinant of cofactors then Δc = Δn-1 (where n > 0) and n is order of determinant Δ. In particular if Δ is determinant of 3rd order
and Δ=
a11 a21 a31
a12 a22 a32
a13 a23 a33
≠ 0 then
Δc =
C11 C21 C31
C12 C22 C32
C13 C23 C33
= Δ2
2. Δ = 0 then Δc = 0
Product of two Determinants
a1 a2
Let D1 = 1 2
c1 c2
a3 α1 α2 α3
3 and D2 = 1 2 3
c3 γ1 γ 2 γ 3
then product of D1 and D2 is defined as follows :
D1 D2 =
∑ai αi
∑bi αi
∑ci αi
∑ai βi
∑bi βi
∑ci βi
∑aiγi
∑biγi
∑ciγi
(Where Σ runs from 1 to 3 i.e. ∑ai αi = a1α1 + a2α2 + a3α3 )
Remark :
1. Since value of determinant remains same when rows and column are interchanged therefore, in finding product of two determinants, we can also multiply rows by columns or column by columns.
2. D1 D2 = D2 D1
Important Observation
a1 a2
If D1 = 1 2
c1 c2
a3 A1 A2 A3
3 and D2 = 1 2 3
c3 C1 C2 C3
where Ai = cofactor of ai Bi = cofactor of bi
and C = cofactor of c
then D
=(D )2
i i 2 1
If t = ar + br + cr, show that
t0 t1
t1 t2
t2 t3
t2
t3 = (a – b)2 (b – c)2 (c – a)2
t4
Solution :
t0 t1
We have t1 t2
t2 t3
t2
t3 =
t4
1
1
1
1
1
1
=
a
b
c
a
b
c
a2
b2
c 2
a2
b2
c 2
1 1 1 2
= a b c
a2 b2 c 2
1 0
= a b − a
a2 b2 − a2
0 2
c − a c 2 − a2
Applying (C2 → C2 – C1, C3 → C3 – C1 )
1
= (b – a)2 (c – a)2 a
a2
0
1
b + a
0 2
1
c + a
= (a – b)2 (c – a)2 [c + a – b – a]2
= (a – b)2 (b – c)2 (c – a)2
AREA OF TRIANGLE
x1
If ABC is a triangle with A(x , y ), B(x ,y ) and C(x , y ) then area of Δ = x2
x3
y1 1
y 2 1
y3 1
The area may come out to be either positive or negative, hence modulus of above would give the magnitude of area.
x1
If x2
x3
y1 1
y 2 1 turns out to be zero, it means points A, B & C are collinear and vice-versa.
y3 1
SYSTEM OF LINEAR EQUATIONS
System of Linear equatins : a11x1 + a12 x2 + ....... + a1n xn = b1 a21x1 + a22 x2 + ....... + a2n xn = b2
an1x1 + an2 x2 + .......+ ann xn = bn
is said to be consistent if it has at least one solution. Otherwise, it is said to be inconsistent.
I. System of homogeneous equations (linear) in three variables.
a1x + b1y + c1 z = 0, a2 x + b2 y + c2 z = 0, a3 x + b3 y + c3 z = 0
Note that x = y = z = 0 (trivial solution) is always a solution. Therefore, this system is always consistent.
a1
Case I : If Δ = a2
a3
b1 c1
b2 c2
b3 c3
≠ 0, there is unique solution x = y = z = 0
Case II : If Δ = 0, the system has infinite number of solutions (existence of non-trivial solutions)
CRAMER'S RULE
Consider the system of equations :
a1 x + b1 y + c1 z = d1, a2 x + b2 y + c2 z = d2, a3 x + b3 y + c3 z = d3
We define
a1
The denominator determinant = Δ = a2
a3
b1 c1
b2 c2
b3 c3
≠ 0 ...(1)
d1 b1 c1
The numerator determinant of x = Δ = d2 b2 c2 (Replace C
of (1) by d , d , d )
x
d3 b3 c3
1 1 2 3
a1 d1 c1
The numerator determinant of y = Δ = a2 d2 c2
a3 d3 c3
a1
and the numerator determinant of z = Δ = a2
a3
b1 d1
b2 d2
b3 d3
Case I :
If Δ ≠ 0
then system is called consistent and have unique solution given by
x = Δ x ,y = Δ y and z = Δ z .(Δ ≠ 0)
Δ Δ Δ
Case II :
If Δ = 0 and but if Δ , Δ , Δ atleast one is non-zero, then system in called inconsistent and have no solution.
Case III :
If Δ = Δ = Δ = Δ = 0, then system have infinite no. of solutions.
⎧ 1 + 2 +
⎪
⎪
⎪
Solve the system ⎨
⎪
y
− 4 − 2 = 1
y z
using determinants.
⎪ 2 + 5 − 2 = 3
⎪⎩ x y z
Solution :
Let
1 = u, 1 = v, 1 = w , then given system can be expressed as u + 2v + w = 2, 3u – 4v – 2w = 1,
x y z
2u + 5v – 2w = 3
1 2
Now the denominator Δ = 3 − 4
2 5
1
− 2 = 45
− 2
2 2
Δ , the numerator of u = 1 − 4
3 5
1
− 2 = 45
− 2
1 2
Δ , the numerator of v = 3 1
2 3
1
− 2 = 15
− 2
1
Δ , the numerator of w = 3
2
2 2
− 4 1
5 3
= 15
Then, u = Δ1 = 45 = 1,
v = Δ2 = 1 , w = Δ3 = 1
Δ 45
Δ 3 Δ 3
∴ Solution of system is given by x = 1, y = 3, z = 3.
MATRICES
A set of mn numbers (real or complex) arranged in the form of a rectangular array having ‘m’ rows and ‘n’ columns is called an m × n matrix. It is usually written as
⎡ a11
⎢ a21
A
a12 a22
...
...
a1n ⎤
a2n ⎥
⎢ Μ Μ
⎢a a
Μ Μ ⎥
... a ⎥
⎣⎢ m1 m 2 mn ⎥⎦
It is represented as A = [aij]m × n. The numbers a11, a12, ... etc. are called elements of the matrix. The element aij
belong to ith row and jth column.
⎡3 2
e.g., A = ⎢5 − 4
7 ⎤
6 ⎥ is a 3 × 3 matrix
⎢⎣4 8 − 12⎥⎦
The number of matrices having 12 elements is
(1)
3
(2)
1
(3)
6
(4)
None of these
Solution : Ans. (3)
The matrix will be any one of the following type 1 × 12, 12 × 1, 2 × 6, 6 × 2, 3 × 4, 4 × 3
TYPES OF MATRICES
Square Matrix :
A matrix having equal number of rows and columns is called a square matrix. If the matrix A has n rows and n
columns, it is said to be square matrix of order n.
Example:
⎡1 2
⎢ 3
⎢⎣3 4
3⎤
⎥
⎥
5⎥⎦
is a square matrix of order 3.
The diagonal of this matrix containing the elements 1, 3, 5 is called the leading or principal diagonal.
Trace of matrix :
The sum of the diagonal elements of a square matrix A is called trace of A.
Trace (A) = ∑aii
i =1
= a11 + a22 + a33 ... + ann
Example :
⎡2
A = ⎢0
⎢⎣8
− 7 9⎤
3 ⎥
9 4⎥⎦
Trace (A) = 2 + 3 + 4 = 9
Diagonal Matrix :
A square matrix in which all the elements, except those in the leading diagonal are zero is called a diagonal
matrix. Thus square matrix is called diagonal matrix if aij
= 0 for i ≠ j.
e.g.,
⎡2 0
A = ⎢0 1
⎢⎣0 0
0⎤
⎥
⎥
4⎥⎦
⎡d1 0
or ⎢ 0 d2
⎢⎣ 0 0
0 ⎤
⎥
⎥
d3 ⎥⎦
Above are diagonal matrices of the type 3 × 3. These are in short written as diag [2, 1, 4] or diag [d1, d2 d3]
If the diagonal elements are d1, d2, dn, then it is written as
diag [d1, d2, , dn].
Scalar Matrix :
A diagonal matrix in which all the elements in the leading diagonal are equal is called scalar matrix. It is equal to
KIn for some scalar K.
⎡3 0
e.g., A = ⎢0 3
⎢⎣0 0
0⎤
⎥
⎥
3⎥⎦
⎡K 0
or ⎢ 0 K
⎢⎣ 0 0
0 ⎤
⎥
⎥
K ⎥⎦
In general for a scalar matrix,
a = 0 for i ≠ j and a = K for i = j
Unit or Identity Matrix :
A square matrix in which all the elements in the leading diagonal are 1 and remaining elements are zero is called a unit or Identity Matrix. A unit matrix of order n is usually denoted by In. Thus for an Identity Matrix
a = 1 and a = 0 for i ≠ j
⎡1
e.g., I3 = ⎢0
0 0⎤
1 0⎥ & I = ⎡1 0⎤
⎢
⎢⎣0 0
⎥
1⎥⎦
2 ⎣0 1⎦
Row matrix :
A matrix A which has only one row and n columns is called a row matrix. It is evidently 1 × n matrix. It is also called a row vector.
e.g., A = [1 2 3] is a row matrix of type 1 × 3
Column matrix :
A matrix A which has m rows and only one column is called a column matrix. It is evidently m × 1 matrix. It is also called a column vector.
⎡1⎤
⎢2⎥
e.g., A = ⎢ ⎥ is a column matrix of type 4 × 1
⎢0⎥
⎢4⎥
⎣ ⎦
Null Matrix or Zero Matrix :
A (m × n) matrix in which all the elements are zero is called a zero matrix or null matrix of the type m × n and is denoted by Om × n or O.
⎡0
Thus ⎢0
0⎤ ⎡0
0⎥ , ⎢0
0 0⎤
0 0⎥ , ⎡0
0 0 0⎤
⎢
⎢⎣0
⎥
0⎥⎦
⎢
⎢⎣0
0 0⎥⎦ ⎣ 0 0 ⎦
All the above are zero or null matrices of type 3 × 2, 3 × 3 and 2 × 4 respectively.
Horizontal matrix :
A m × n matrix is called a horizontal matrix if m < n
⎡1 0 2⎤
e.g., A =
⎣ 4 ⎦
Vertical matrix :
A m × n matrix is called a vertical matrix of m > n.
⎡1
e.g., A = ⎢2
⎢⎣3
0⎤
⎥
⎥
5⎥⎦
Triangular matrix :
Let A be a square matrix
⎡a11
⎢a21
A = ⎢a31
⎢ ...
⎢⎣an1
a1n ⎤
a2n ⎥
a3n ⎥
... ⎥
ann ⎥⎦
Any element of A is aij and for i = j we get the diagonal elements. All those elements which are above the principal diagonal are of the type a12, a13, a23, a34, a3n or in general aij where i < j and all those elements which are below
the principal diagonal are of the type a21, a31, an3, so on or in general aij where i > j.
Upper Triangular Matrix : A square matrix (aij) is called an upper triangular matrix if aij = 0 when
i > j. In other words, all elements below the principal diagonal be zero.
Lower Triangular Matrix : A square matrix (aij) is called lower triangular matrix if aij = 0 when i < j. In other words, all the elements above the principal diagonal be zero.
⎡3
for e.g., ⎢0
⎢⎣0
− 2 4 ⎤
2 − 3⎥ &
0 7 ⎥⎦
⎡2 0
⎢ 4
⎢⎣2 8
0⎤
⎥
⎥
6⎥⎦
are upper and lower triangular matrices respectively.
Transpose of a Matrix :
A matrix obtained by interchanging rows and columns of a matrix A is called transpose of A and is denoted by A′
or AT.
Note : If A is a m × n matrix, then A′ is an n × m matrix.
⎡1 2 3⎤ ⎡1 4 7⎤
e.g.,
A = ⎢4 5 6⎥ , then A′ = ⎢2 5 8⎥
⎢
⎢⎣7
⎥
8 9⎥⎦
⎢
⎢⎣3 6
⎥
9⎥⎦
Properties of Transpose
(i) (A′)′ = A (ii) (A + B)′ = A′ + B′
a12
a13
...
a22
a23
...
a32
a33
...
...
...
...
an2
an3
...
(iii) (KA)′ = KA′ (iv) (AB)′ = B′ A′
Symmetric Matrix :
A square matrix A = [a ] is said to be symmetric when a = a for all i and j. In other words, A′ = A
⎡1 4
e.g., ⎢4 2
⎢⎣5 − 6
5 ⎤
− 6⎥ 3 ⎥⎦
is 3 × 3 matrix
Here a12 = a21, a13 = a31, a23 = a32
Skew-symmetric matrix :
A square matrix is said to be skew-symmetric if aij = –aji for all i and j so that all the leading diagonal elements are zero.
In other words A′ = –A
⎡ 0 2
e.g., ⎢− 2 0
⎢⎣ 3 − 5
− 3⎤
⎥
⎥
0 ⎥⎦
is 3 × 3 matrix
here a12 = –a21, a13 = –a31, a23 = –a32
a11 = a22 = a33 = 0
Every square matrix can be uniquely expressed as a sum of a symmetric and skew-symmetric matrix. Let A be the given square matrix, then
A = 1 (A + A′) +
2
1 (A – A′) = P + Q
2
where P is a symmetric matrix and Q is a skew-symmetric matrix.
Singular matrix :
A square matrix A is said to be singular if | A | = 0.
Non-singular matrix :
A square matrix A is said to be non-singular if | A | ≠ 0.
Orthogonal Matrix :
A matrix A is said to be orthogonal if AA′ = I. (Identity matrix)
Equality of Matrices
Two matrices A = [aij]m × n , B = [bij]m × n are said to be equal and written as A = B if and only if
they are of the same order and
each element of A is equal to the corresponding element of B.
⎡1 2 0⎤ ⎡1 2 0⎤
Let A = ⎢3 2
4⎥ , B = ⎢3 2 4⎥
⎣ ⎦ ⎣ ⎦
Here A and B are equal matrices and we write A = B
Find value of x, y, z and w which satisfy the matrix equation
⎡x + 3
2y + x ⎤ ⎡− x − 1 0 ⎤
⎢ z − 1
4w − 8⎥ = ⎢ 3
2w ⎥
Solution :
As the two matrices are equal and are of order 2 × 2, so
x + 3 = –x –1 ...(1)
2y + x = 0 ...(2)
z –1 = 3 ...(3)
4w –8 = 2w ...(4)
on solving above equations, we get
x = –2, y = 1, z = 4, w = 4
ALGEBRA OF MATRICES
Let A and B be two matrices of same order m × n. Then their sum is defined to be the matrix of order m × n
obtained by adding the corresponding elements of A and B
⎡a11
a12 ⎤
⎡b11
b12 ⎤
e.g., If A = ⎢a21
a22 ⎥
and B = ⎢
⎣ 21
⎥ ,
b22 ⎦
then A + B =
⎡a11 + b11
⎢a21 + b21
a12 + b12 ⎤
a22 + b22 ⎥
Properties :
Matrix addition is commutative
If A and B be two m × n matrices, then A + B = B + A
Matrix addition is associative
If A, B and C be three matrices each of order m × n, then (A + B) + C = A + (B + C)
Existence of additive Identity : If O be the m × n matrix each of whose elements is zero, then
A + O = A = O + A for every m × n matrix A.O is called additive Identity.
Existence of additive Inverse:
Let A = [aij]m × n. Then the negative of the matrix A is defined as the matrix [–aij]m × n and is denoted by – A. A + (– A) = 0
e.g., If A = ⎡1 − 2
⎣ 2
0 ⎤
− 5⎥
then –A = ⎡ − 1
⎣
2 0⎤
− 2 ⎦
Cancellation laws hold good for addition : If A, B, C be any three m × n matrices, then
A + B = A + C ⇒ B = C
k(A + B) = kA + kB, where k is scalar.
Subtraction of two matrices
Let A and B be two m × n matrices. Then the difference of A and B is denoted by A – B and is defined by
A – B = A + (–B)
A – B will also be a m × n matrix. In order to find A – B, the elements of B must be subtracted from the corresponding elements of A.
⎡1 2 3⎤ ⎡2 − 1 4⎤
e.g., A = ⎢3
− 1 0⎥ , B = ⎢5 0 6⎥
⎣ ⎦ ⎣ ⎦
⎡1− 2
then A – B = ⎢3 − 5
2 + 1
− 1− 0
3 − 4⎤
0 − 6⎥
⎡ − 1
= ⎢− 2
3 − 1⎤
− 1 − 6⎥
⎡1 4⎤
⎡− 1
− 2⎤
If A = ⎢3
2⎥ , B = ⎢ 0
5 ⎥ , find the matrix D such that A + B –D = 0 i.e., zero matrix.
⎢
⎢⎣2
⎥
5⎥⎦
⎢
⎢⎣ 3
⎥
1 ⎥⎦
Solution :
⎡a b⎤
Let the matrix D be ⎢c
⎢⎣e
⎡ 1− 1− a
⎥
⎥
f ⎥⎦
4 − 2 − b⎤
∴ A + B –D = ⎢3 + 0 − c
⎢⎣2 + 3 − e
2 + 5 − d ⎥
5 + 1− f ⎥⎦
⎡ − a 2 − b⎤ ⎡0 0⎤
= ⎢3 − c 7 − d ⎥ = ⎢0 0⎥ given
⎢
⎢⎣5 − e
⎥
6 − f ⎥⎦
⎢
⎢⎣0
⎥
0⎥⎦
From the definition of equality of matrices,
– a = 0 ⇒ a = 0
2 – b = 0 ⇒ b = 2
3 – c = 0 ⇒ c = 3
7 – d = 0 ⇒ d = 7
5 – e = 0 ⇒ e = 5
6 – f = 0 ⇒ f = 6
⎡0
∴ D = ⎢3
⎢⎣5
2⎤
⎥
⎥
6⎥⎦
which is clearly equal to A + B
Multiplication of Matrix by a scalar
The product of a matrix A by a scalar k is a matrix whose each element is k times the corresponding elements of A.
⎡a1
Thus k ⎢a2
b1 c1 ⎤
b2 c2 ⎥ =
⎡ ka1
⎢ka2
kb1 kb2
kc1 ⎤ kc2 ⎥
Properties of Scalar Multiplication
If A and B be any two m × n matrices and k is any scalar, then
k(A + B) = kA + kB
If A is any m × n matrix and a and b are any two scalars, then (a + b)A = aA + bA
If A be any m × n matrix and k be any scalar, then (– k)A = – (kA) = k(– A)
Multiplication of Matrices
Let A = [aij] be a m × n matrix and B = [bjk] be a n × p matrix such that number of columns in A is equal to number of rows in B. Then product of matrices A and B denoted by AB is a matrix of m × p matrix.
⎡a1 b1 c1 ⎤
⎡ l l ⎤
⎢a b c ⎥
⎢ 1 2 ⎥
For instance, let A = ⎢ 2 2 2 ⎥
and B = ⎢m1 m2 ⎥
⎢a3 b3 c3 ⎥
⎢ n n ⎥
⎢
⎣a4 b4
⎥
4 ⎦ 4 × 3
⎣ 1 2 ⎦3×2
then matrix AB is a matrix of order 4 × 2
AB =
⎡ a1l1 + b1m1 + c1n1
⎢a2l1 + b2m1 + c2n1
⎢a3l1 + b3m1 + c3n1
a1l2 + b1m2 + c1n2 ⎤
a2l2 + b2m2 + c2n2 ⎥
a3 l2 + b3m2 + c3 n2 ⎥
⎢a l + b m + c n
a l + b m + c n ⎥
⎣ 4 1 4 1 4 1
4 2 4 2 4 2 ⎦
In other words, product AB is a matrix C = [Cik]m × p
= ∑aij bjk j =1
Properties :
If AB = O (null matrix), it does not necessarily imply that A or B is a null matrix.
⎡1 1⎤ ⎡ 1 − 1⎤
For instance, if A = ⎢1 1⎥ and B = ⎢− 1 1 ⎥ , then the product AB is a null matrix, although neither A
⎣ ⎦ ⎣ ⎦
nor B is a null matrix.
Multiplication of matrices is not always commutative
AB may or may not be equal to BA
Multiplication of matrices is associative
(AB)C = A(BC)
If A, B, C are m × n, n × p and p × q matrices respectively.
Multiplication of matrices is distributive w.r.t. addition of matrices:
If A is a m × n matrix and B and C are both n × p matrices, then
A(B + C) = AB + AC
Multiplication of Matrix by Unit matrix, I
AI = IA = A if conformability for multiplication is satisfied.
Multiplication of Matrix by Null Matrix :
OA = AO = O where O = null matrix
Whenever AB and BA both exist and are matrices of same order, it is not necessary that AB = BA
⎡1 0 ⎤ ⎡0 1⎤
e.g., A = ⎢0
− 1⎥ , B = ⎢1 0⎥
⎣ ⎦ ⎣ ⎦
⎡1 0 ⎤ ⎡0 1⎤ ⎡ 0 1⎤
then AB = ⎢0
− 1⎥ ⎢1
0⎥ = ⎢− 1 0⎥
⎣ ⎦ ⎣ ⎦ ⎣ ⎦
⎡0
BA = ⎢
⎣
1⎤ ⎡1
⎥ ⎢
⎦ ⎣
0 ⎤ ⎡0
− 1⎥ = ⎢
− 1⎤
⎥
⎦
Thus AB ≠ BA
⎡0 1 2⎤
⎡ 1 − 2⎤
If A = ⎢1 2
3⎥ and B = ⎢− 1
0 ⎥ , then
⎢
⎢⎣2 3
⎥
4⎥⎦
⎢
⎢⎣ 2
⎥
− 1⎥⎦
find AB. Is BA defined ?
Solution :
Matrix A is of the order 3 × 3 and matrix B is of the order 3 × 2. Since the number of columns of A = number of rows of B (each being = 3).
∴ Product AB is defined.
AB =
⎡0 1
⎢ 2
⎢⎣2 3
2⎤
⎥
⎥
4⎥⎦
⎡ 1
⎢− 1
⎢⎣ 2
− 2⎤
⎥
⎥
− 1⎥⎦
⎡0.1+ 1. − 1+ 2.2
= ⎢1.1+ 2. − 1+ 3.2
⎢⎣2.1+ 3. − 1+ 4.2
0. − 2 + 1.0 + 2. − 1⎤
1. − 2 + 2.0 + 3. − 1⎥
2. − 2 + 3.0 + 4. − 1⎥⎦
⎡3
⎢
= ⎢
⎢⎣7
− 2⎤
− 5⎥
− 8⎥⎦
Again, since number of columns of B ≠ number of rows of A.
∴ Product BA is not possible.
ADJOINT OF MATRIX
Let A = [aij] be a square matrix.
Let B = [Aij] where Aij is the cofactor of the element aij in the det. A.
Then adjoint of matrix A is transpose B′ of matrix B and is denoted by adj. A.
Find the adjoint of the matrix
⎡1
A = ⎢1
⎢⎣2
1 1 ⎤
2 − 3⎥
− 1 3 ⎥⎦
Solution :
First we have to find cofactors A , A , ... etc. A = (–1)1+1
1 − 3
2 − 3
− 1 3 = 3
A12
A13
= (–1)1+2 2
= (–1)1+3 1
2
3 = –9
2 = –5
− 1
Similarly, we can find all cofactors A21, A22, A23, A31, A32, A33
⎡ A11
Adj A = ⎢A12
⎢⎣A13
A21 A22 A23
A31 ⎤ A32 ⎥
A33 ⎥⎦
⎡ 3 − 4
= ⎢− 9 1
⎢⎣− 5 3
− 5⎤
⎥
⎥
1 ⎥⎦
INVERSE OF A SQUARE MATRIX
A square matrix A is said to be invertible if there exists a square matrix B such that AB = BA = In (identity matrix) Here B = A–1 or A = B–1.
The necessary and sufficient condition for a square matrix A to possess the inverse is that |A| ≠ 0.
Adj (A)
Inverse of matrix A is denoted by A–1 and A–1 =
| A |
⎡1
If A = ⎢2
⎢⎣1
− 1 1⎤
− 1 0⎥ , find A2 and show that A2 = A–1
0 0⎥⎦
Solution :
A2 = A.A
⎡1 − 1
= ⎢2 − 1
⎢⎣1 0
1⎤ ⎡1
⎥ ⎢
⎥ ⎢
0⎥⎦ ⎢⎣1
− 1 1⎤
− 1 ⎥
0 0⎥⎦
⎡0
A2 = ⎢0
⎢⎣1
0 1⎤
− 1 ⎥
− 1 1⎥⎦
... (i)
| A | = 1 ... (ii)
A11
− 1
= (– 1)1+1 0
0 = 0
0
A12
− 2
= (– 1)1+2 1
0 = 0
0
Similarly we can find A13, A21, A22, A23, A31, A32, A33
⎡0
Adj. A = ⎢0
⎢⎣1
0 1⎤
− 1 ⎥
− 1 1⎥⎦
A−1 =
Adj. A
| A |
⎡0
= ⎢
⎢⎣1
0 1⎤
− 1 ⎥
− 1 1⎥⎦
... (iii)
So from (i) and (iii), A2 = A–1
Important Results :
A.(adj. A) = (adj A). A = | A | In, where A is any square matrix of order n.
AA–1 = A–1A = I
(A–1)–1 = A
Inverse of a square matrix, if it exists, is unique
The reciprocal of the product of two matrices is the product of their reciprocals taken in the reverse order. (AB)–1 = B–1A–1.
| adj A | = | A |n–1
| A. (adj A) | = | A |n
(adj AB) = (adj B).(adj A)
adj (A′ ) = (adj A)′
If A is non-singular square matrix, then adj. (adj A) = |A|n–2A
1
If A is a non-singular matrix, then |A–1| = |A|–1 = | A |
det (kA) = k n (det A) if A is of order n × n.
det (An) = (det A)n if n is a +ve integer.
The operation of transposing and inverting are commutative
i.e., (A′ )–1 = (A–1)′
SOLUTION OF SIMULTANEOUS LINEAR EQUATIONS USING MATRICES
Consider a system of n linear equations in n unknowns x1 x2, ..., xn. i.e.,
ai1 x1 + ai2 x2 + ... + ain xn = bi , i = 1, 2, 3 ..., n
If b1 = b2 = ... = bn = 0, then the system of equations is called a system of homogenous linear equations and if atleast one of b1, b2, ..., bn is non-zero, then it is called a system of non-homogeneous linear equations.
These equations can be written in the form of a single matrix equation of AX = B
Where
⎡a11
a12
… a1n ⎤
⎡ x1 ⎤
⎡ b1 ⎤
⎢a21
a22
… a2n ⎥
⎢x ⎥
⎢b ⎥
⎢ ⎥ ⎢ 2 ⎥
⎢ 2 ⎥
A = ⎢ …
⎢ …
… … … ⎥
… … … ⎥
, X = ⎢…⎥
⎢…⎥
and B = ⎢…⎥
⎢…⎥
⎢ ⎥ ⎢ ⎥ ⎢ ⎥
⎢⎣an1
an 2
… ann ⎥⎦n × n
⎢⎣xn ⎥⎦
n ×1
⎢⎣bn ⎥⎦n ×1
When system of equations is non-homogeneous
If | A | ≠ 0, then system of equations is consistent and has a unique solution given by X = A–1 B.
If | A | = 0, and (adj A).B ≠ 0, then system of equations is inconsistent and has no solution.
| A | = 0, and (adj A).B = 0, then system of equations is consistent and has infinite number of solutions.
When system of equations is homogeneous
If | A | ≠ 0, system of equations have only one solution i.e. x = y = z = 0
If | A | = 0, system of equations have infinite number of solutions.
SOLVED EXAMPLES
Example : 1
Write down in matrix form the system of equations
2x – y + 3z = 9, x + y + z = 6, x – y + z = 2 and solve it
Solution :
The given system of equations can be written in matrix form as AX = B
⎡2
Where A = ⎢1
− 1 3⎤
1 1⎥ ,
⎡x ⎤ X = ⎢y ⎥ ,
⎡9⎤
B = ⎢6⎥
⎢ ⎥ ⎢ ⎥ ⎢ ⎥
⎢⎣1 − 1 1⎦⎥ ⎢⎣z ⎥⎦ ⎢⎣2⎥⎦
We have | A | = – 2 ≠ 0 i.e. A is non-singular and therefore A–1 exists
⎡− 1 1
A−1 = adj A = ⎢ 0 1
2 ⎤
−1 ⎥
| A |
⎢
⎢⎣ 1
2 2 ⎥
−12 −3 2⎥⎦
∴ X = A–1 B =
⎡− 1 1
⎢ 0
2 ⎤ ⎡9⎤
−1 ⎥ ⎢6⎥
⎢ 2 ⎥ ⎢ ⎥
⎢⎣ 1 −12 −3 2⎥⎦ ⎢⎣2⎥⎦
⎡x ⎤ ⎡1⎤
X = ⎢y ⎥ = ⎢2⎥
⇒ ⎢ ⎥ ⎢ ⎥
⎢⎣z ⎥⎦ ⎢⎣3⎥⎦
i.e., (x, y, z) ≡ (1, 2, 3).
Example 2 :
Solve the system of equations x + 3y – 2z = 0
2x – y + 4z = 0
x – 11y + 14z = 0
Solution :
The given system of equations in the matrix form are written as below
⎡1 3
− 2⎤ ⎡x⎤ ⎡0⎤
⎢2 − 1
4 ⎥ ⎢y ⎥ = ⎢0⎥
⎢ ⎥ ⎢ ⎥ ⎢ ⎥
⎢⎣1
− 11
14 ⎥⎦ ⎢⎣z⎥⎦
⎢⎣0⎥⎦
AX = 0
| A | = 1(–14 + 44) – 3(28 – 4) –2(– 22 + 1)
= 30 – 72 + 42 = 0 (i)
and therefore the system has infinitely many solutions. Taking first two equations,
x + 3y = 2z (ii)
2x – y = – 4z (iii)
and solving in terms of z, we get
x = −10z , y = 8 z
... (iv)
7 7
Put these values of x and y in third equation x – 11y + 14z = 0, its value comes to be equal to zero.
Now if z = 7k, then x = – 10k, y = 8k where k is any arbitrary constant.
So then required solutions are
x = –10k, y = 8k & z = 7k
⎡ 4 2
Express the matrix A as the sum of a symmetric and a skew-symmetric matrix, where A = ⎢ 1 3
⎢⎣− 5 0
− 3⎤
− 6⎥
− 7⎥⎦
Solution :
⎡ 4
A′ = ⎢ 2
⎢⎣− 3
1 − 5⎤
3 ⎥
− 6 − 7⎥⎦
⎡ 8 3
Then A + A′ = ⎢ 3 6
⎢⎣− 8 − 6
− 8 ⎤
6 ⎥ and
− 14⎥⎦
⎡ 0 1
A – A′ = ⎢ − 1 0
⎢⎣− 2 6
2 ⎤
− 6⎥ 0 ⎥⎦
∴ A =
1 (A + A′ ) +
2
1 (A – A′ )
2
⎡ 4 1.5
− 4⎤ ⎡ 0 0.5 1 ⎤
⎡ 4 2 − 3⎤
= ⎢1.5 3
− 3⎥ + ⎢− 0.5 0
− 3⎥ = ⎢ 3 − 6⎥
⎢⎣− 4 − 3
− 7⎥⎦
⎣⎢ − 1
3 0 ⎥⎦
⎢⎣− 5 0
− 7⎥⎦
❑ ❑ ❑
Popular posts from this blog
Physics-30.24-Physics-Solids and Semiconductors
UNIT 24 - SOLIDS AND SEMICONDUCTORS 1. SOLID STATE ELECTRONICS (SEMICONDUCTORS) (A) Energy bands in solids: (i) In solids, the group of closely lying energy levels is known as energy band. (ii) In solids the energy bands are analogous to energy levels in an atom. (iii) In solids the atoms are arranged very close to each other. In these atoms there are discrete energy levels of electrons. For the formation of crystal these atoms come close together, then due to nucleus-nucleus, electron-electron and electron-nucleus interactions the discrete energy levels of atom distort and consequently each energy level spits into a large number of closely lying energy levels. (iv) The number of split energy levels is proportional to the number of atoms interacting with each other. If two atoms interact then each energy level splits into two out of which one will be somewhat above and another will be somewhat below the main energy level. In solids the number of atoms is very large ( 1023). Hence eac...
Physics-31.Rotational Mechanics
5.1 DEFINITION OF CENTRE OF MASS Centre of mass: Every physical system has associated with it a certain point whose motion characterizes the motion of the whole system. When the system moves under some external forces than this point moves as if the entire mass of the system is concentrated at this point and also the external force is applied at his point of translational motion. This point is called the centre of mass of the system. Centre of mass of system of n point masses or n particles is that point about which moment of mass of the system is zero, it means that if about a particular origin the moment of mass of system of n point masses is zero, then that particular origin is the centre of mass of the system. The concept of centre of mass is a pure mathematical concept. If there are n particles having mass m1, m2 ….m n and are placed in space (x1, y1, z1), (x2, y2, z2) ……….(x n, y n, z n) then centre of mass of system is defined as (X, Y, Z) where = Y = and Z = where...
Comments
Post a Comment