34794672-Fundamental-Formulas-of-Physics-Vol-1-Tqw-darksiderg_1

Page 109

§ 18.5

87

BASIC MATHEMATICAL FORMULAS

If the transformation which takes the

into the z; directly is

Xk

n

Zi

= ~ CikX k

is

Zt = CXt,

C = AB and Zt = ABXt

then

(3)

k~1

18.5. Transposed matrix. If A = II a ij II IS m by N, the transposed matrix A' = II a ji II is N by m. For a product C = AB, the transposed matrix is C' = B'A'. For xt, Yt, zt the column matrices of § 18.4 with a single column, the transposed matrices will be row matrices with a single row. We denote them by X, -V, Z. Then the transformations of § 18.4 may be written in terms of row matrices as ~

~

~

Y=XB',

~

~

z= YA',

~

~

~

Z=XC', or Z=XB'A',

sinceC'=B'A'

18.6. Inverse matrix. The unit matrix is a square matrix with ones on the main diagonal and the remaining ele1Dents zero. Its elements are 0ik = 0 if i ~ k, and = 1 if i = k. A square matrix is singular if its determinant is zero. Each nonsingular square matrix has a reciprocal matrix A-I such that AA-l

= Iloik II

and

A-IA

= 110;k II

(1)

Let I A I denote the determinant I aik I, and A ik the cofactor of aik or product of (-1 )i+ k by the determinant obtained from I aik I by striking out the ith row and kth column. (See § 1.8.) Then explicitly A-I has as elements

a

-1

A TAT

_

ki

ik -

(2)

18.7. Symmetry. For square matrices symmetry and skew-symmetry are defined as for tensors in § 7.10. Orthogonal and unitary, or Hermitian orthogonal matrices are defined in § 7.1 1. 18.8. Linear equations. The set of n linear equations in n unknowns

X k,

n

~aik,xk=bi' i=I,2, ... ,n

(1)

k~1

determine

a

Bt = II Bi II

square matrix A = II aile II and two column matrices and xt = II Xi II· In matrix form we m;iy write

AXt

=

Bt

(2)


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