1 Basic concepts

1.1 Determinants

A square matrix possesses an associated determinant. Unlike a matrix, which is an array of numbers, a determinant has a single value.

A two by two matrix C = c 11 c 12 c 21 c 22 has an associated determinant

det ( C ) = c 11 c 12 c 21 c 22 = c 11 c 22 c 21 c 12

(Note square or round brackets denote a matrix, straight vertical lines denote a determinant.)

A three by three matrix has an associated determinant

det ( C ) = c 11 c 12 c 13 c 21 c 22 c 23 c 31 c 32 c 33

Among other ways this determinant can be evaluated by an “expansion about the top row”:

det ( C ) = c 11 c 22 c 23 c 32 c 33 c 12 c 21 c 23 c 31 c 33 + c 13 c 21 c 22 c 31 c 32

Note the minus sign in the second term.

Task!

Evaluate the determinants

det ( A ) = 4 6 3 1 det ( B ) = 4 8 1 2 det ( C ) = 6 5 4 2 1 7 3 2 0

det A = 4 × 1 6 × 3 = 14 det B = 4 × 2 8 × 1 = 0

det C = 6 1 7 2 0 5 2 7 3 0 + 4 2 1 3 2 = 6 × ( 14 ) 5 ( 21 ) + 4 ( 4 3 ) = 185 A matrix such as B = 4 8 1 2 in the previous task which has zero determinant is called a singular matrix. The other two matrices A and C are non-singular . The key factor to be aware of is as follows:

Key Point 1

Any non-singular n × n matrix C , for which det ( C ) 0 , possesses an inverse C 1 i.e.

C C 1 = C 1 C = I where I denotes the n × n identity matrix

A singular matrix does not possess an inverse.

1.2 Systems of linear equations

We first recall some basic results in linear (matrix) algebra. Consider a system of n equations in n unknowns x 1 , x 2 , , x n :

c 11 x 1 + c 12 x 2 + + c 1 n x n = k 1 c 21 x 1 + c 22 x 2 + + c 2 n x n = k 2 + + + = c n 1 x 1 + c n 2 x 2 + + c n n x n = k n

We can write such a system in matrix form:

c 11 c 12 c 1 n c 21 c 22 c 2 n c n 1 c n 2 c n n x 1 x 2 x n = k 1 k 2 k n , or equivalently C X = K .

We see that C is an n × n matrix (called the coefficient matrix), X = { x 1 , x 2 , , x n } T is the n × 1 column vector of unknowns and K = { k 1 , k 2 , , k n } T is an n × 1 column vector of given constants.

The zero matrix will be denoted by O ̲ .

If K O ̲ the system is called inhomogeneous ; if K = O ̲ the system is called homogeneous .

1.3 Basic results in linear algebra

Consider the system of equations C X = K .

We are concerned with the nature of the solutions (if any) of this system. We shall see that this system only exhibits three solution types:

  The system is consistent and has a unique solution for X

  The system is consistent and has an infinite number of solutions for X

  The system is inconsistent and has no solution for X

consider:

det ( C ) 0 or det ( C ) = 0

Case 1 det ( C ) 0

In this case C 1 exists and the unique solution to C X = K is

X = C 1 K

Case 2 det ( C ) = 0

In this case C 1 does not exist.

  1. If K O ̲ the system C A = K has no solutions .
  2. If K = O ̲ the system C X = O ̲ has an infinite number of solutions.

We note that a homogeneous system

C X = O ̲

has a unique solution X = O ̲ if det ( C ) 0 (this is called the trivial solution ) or an infinite number of solutions if det ( C ) = 0 .

Example 1

(Case 1) Solve the inhomogeneous system of equations

x 1 + x 2 = 1 2 x 1 + x 2 = 2

which can be expressed as C X = K where

C = 1 1 2 1 X = x 1 x 2 K = 1 2

Solution

Here det ( C ) = 1 0 .

The system of equations has the unique solution : X = x 1 x 2 = 1 0 .

Example 2

(Case 2a) Examine the following inhomogeneous system for solutions

x 1 + 2 x 2 = 1

3 x 1 + 6 x 2 = 0

Solution

Here det ( C ) = 1 2 3 6 = 0.   In this case there are no solutions.

To see this we see the first equation of the system states x 1 + 2 x 2 = 1 whereas the second equation (after dividing through by 3) states x 1 + 2 x 2 = 0 , a contradiction.

Example 3

(Case 2b) Solve the homogeneous system

x 1 + x 2 = 0

2 x 1 + 2 x 2 = 0

Solution

Here det ( C ) = 1 1 2 2 = 0. The solutions are any pairs of numbers { x 1 , x 2 } such that x 1 = x 2 , i.e. X = α α  where α  is arbitrary .

There are an infinite number of solutions .

1.4 A simple eigenvalue problem

We shall be interested in simultaneous equations of the form:

A X = λ X ,

where A is an n × n matrix, X is an n × 1 column vector and λ is a scalar (a constant) and, in the first instance, we examine some simple examples to gain experience of solving problems of this type.

Example 4

Consider the following system with n = 2 :

2 x + 3 y = λ x 3 x + 2 y = λ y

so that

A = 2 3 3 2  and X = x y .

It appears that there are three unknowns x , y , λ . The obvious questions to ask are: can we find x , y ? what is λ ?

Solution

To solve this problem we firstly re-arrange the equations (take all unknowns onto one side);

( 2 λ ) x + 3 y = 0 (1)

3 x + ( 2 λ ) y = 0 (2)

Therefore, from equation (2):

x = ( 2 λ ) 3 y . (3)

Then when we substitute this into (1)

( 2 λ ) 2 3 y + 3 y = 0 which simplifies to ( 2 λ ) 2 + 9 y = 0.

We conclude that either y = 0 or 9 = ( 2 λ ) 2 . There are thus two cases to consider:

Case 1

If y = 0 then x = 0 (from (3)) and we get the trivial solution . (We could have guessed this solution at the outset.)

Case 2

9 = ( 2 λ ) 2

which gives, on taking square roots:

± 3 = 2 λ  giving λ = 2 ± 3 so λ = 5  or λ = 1.

Now, from equation (3), if λ = 5 then x = + y and if λ = 1 then x = y .

We have now completed the analysis. We have found values for λ but we also see that we cannot obtain unique values for x and y : all we can find is the ratio between these quantities. This behaviour is typical, as we shall now see, of an eigenvalue problem.