Mathematical Methods for Physics and Engineering : A Comprehensive Guide

(Darren Dugan) #1

MATRICES AND VECTOR SPACES


determinant defined by (8.45) and their corresponding cofactors, we write|A|as


the Laplace expansion


|A|=A 21 (−1)(2+1)M 21 +A 22 (−1)(2+2)M 22 +A 23 (−1)(2+3)M 23

=−A 21





A 12 A 13
A 32 A 33




∣+A^22





A 11 A 13
A 31 A 33




∣−A^23





A 11 A 12
A 31 A 32




∣.

We will see later that the value of the determinant is independent of the row


or column chosen. Of course, we have not yet determined the value of|A|but,


rather, written it as the weighted sum of three determinants of order 2. However,


applying again the definition of a determinant, we can evaluate each of the


order-2 determinants.


Evaluate the determinant ∣



A 12 A 13


A 32 A 33


∣∣



∣.


By considering the products of the elements of the first row in the determinant, and their
corresponding cofactors, we find


∣∣


A 12 A 13


A 32 A 33


∣∣



∣=A^12 (−1)


(1+1)|A 33 |+A 13 (−1)(1+2)|A 32 |


=A 12 A 33 −A 13 A 32 ,


where the values of the order-1 determinants|A 33 |and|A 32 |are defined to beA 33 andA 32
respectively. It must be remembered that the determinant isnotthe same as the modulus,
e.g. det (−2) =|− 2 |=−2, not 2.


We can now combine all the above results to show that the value of the

determinant (8.45) is given by


|A|=−A 21 (A 12 A 33 −A 13 A 32 )+A 22 (A 11 A 33 −A 13 A 31 )

−A 23 (A 11 A 32 −A 12 A 31 ) (8.46)

=A 11 (A 22 A 33 −A 23 A 32 )+A 12 (A 23 A 31 −A 21 A 33 )

+A 13 (A 21 A 32 −A 22 A 31 ), (8.47)

where the final expression gives the form in which the determinant is usually


remembered and is the form that is obtained immediately by considering the


Laplace expansion using the first row of the determinant. The last equality, which


essentially rearranges a Laplace expansion using the second row into one using


the first row, supports our assertion that the value of the determinant is unaffected


by which row or column is chosen for the expansion.

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