Download An Introduction to Matrices, Sets and Groups for Science by G. Stephenson PDF

By G. Stephenson

This extraordinary textual content deals undergraduate scholars of physics, chemistry, and engineering a concise, readable creation to matrices, units, and teams. Concentrating quite often on matrix conception, the ebook is nearly self-contained, requiring at the very least mathematical wisdom and supplying the entire history essential to boost a radical comprehension of the subject.
Beginning with a bankruptcy on units, mappings, and differences, the therapy advances to concerns of matrix algebra, inverse and comparable matrices, and platforms of linear algebraic equations. extra issues comprise eigenvalues and eigenvectors, diagonalisation and features of matrices, and staff concept. every one bankruptcy features a number of labored examples and plenty of issues of solutions, allowing readers to check their knowing and skill to use innovations.

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Extra resources for An Introduction to Matrices, Sets and Groups for Science Students

Example text

14 (12) Now the product BA is also defined in this case since the number of columns of B is equal to the number of rows of A. However, it is readily found that BA (7 = 3 4 5 11 12 ~) . I(b)). This non-commutative property of matrix multiplication may appear even when the two products are defined and are of the same order. To illustrate this we take (14) Then 0), (15) -1 whence again AB # BA. This shows that matrices behave in a different way from numbers by not obeying (in general) the commutative law of multiplication.

All (20) a2! IXZ! = (a 31 Now suppose A and B are two matrices conformable to addition. Then if A and B are partitioned as B=(IlI! 1l2! 1112 ) (21) Ilzz we have A+B=(lXll+llll IX ZI +PZ! z) IX zz (22) +Ilzz provided that for each sub-matrix lX ik the corresponding sub-matrix Ilik is of the same order. 2] titioned in precisely the same way. For example, _1 47) + (_0 _~) 1 ( 11 7 13 ). (23) 9 15 = ( 2 3 58 69 1 2 47 58 3 5 17 We now come to the problem of the multiplication of partitioned matrices.

Similarly we may prove that AI = A. By taking A = I in the results, we find 12 = I and consequently I k = I k- 1 = ... = 12 = I, (58) (59) where k is any positive integer. If A is not square then IA # AI since one or other of these products will not be defined. However, provided the product is defined we can always multiply an (m x n) matrix. by a unit matrix without changing its form. For example, 1 0 (60) o 1 ( o 0 (g) Idempotent and nilpotent matrices A square matrix A which satisfies the relation A2 = A (61) is called idempotent.

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