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Unit 15: Tensors in Cartesian Coordinates




          Thus, formula (4) defines the vectorial object y. As a result, we have vector y determined by a  Notes
          linear operator F and by vector x. Therefore, we write
                                           y = F(x)                                ...(7)
          and say that y is obtained by applying linear operator F to vector x. Some people like to write (7)
          without parentheses:
                                           y = Fx.                                ....(8)
          Formula (8) is a more algebraic form of formula (7). Here the action of operator F upon vector
          x is designated like a kind of multiplication. There is also a matrix representation of formula (8),
          in which x and y are represented as columns:

                                     y 1  F 1 1  F 2 1  F 3 1  x 1
                                      2
                                                     2
                                     y   F 1 2  F 2 2  F 3 2  x .                 ...(9)
                                     y 3  F 1 3  F 2 3  F 3 3  x 3
          Exercise 15.6: Derive (9) from (4).
          Exercise 15.7: Let  be some real number and let x and y be two vectors. Prove the following
          properties of a linear operator (7):
          (1)  F(x + y) = F(x) + F(y),
          (2)  F( x) = F(x).
          Write these equalities in the more algebraic style introduced by (8). Are they really similar to
          the properties of multiplication?
          Exercise 15.8: Remember that for the product of two matrices
                                      det(AB) = detA detB.                        ...(10)
          Also remember the formula for det(A ). Apply these two formulas to (3) and derive
                                        –1
                                        det F =  detF.                            ...(11)
                                                  
          Formula (10) means that despite the fact that in various bases linear operator F is represented by
          various matrices, the determinants of all these matrices are equal to each other. Then we can
          define the determinant of linear operator F as the number equal to the determinant of its matrix
          in any one arbitrarily chosen basis e , e , e :
                                       1
                                            3
                                          2
                                         det F = det F.                           ...(12)
          Exercise  15.9  (for  deep  thinking).  Square  matrices  have  various  attributes:  eigenvalues,
          eigenvectors,  a characteristic  polynomial, a  rank (maybe  you remember some others). If  we
          study these attributes for the matrix of a linear operator, which of them can be raised one level
          up and considered as basis-independent attributes of the linear operator itself? Determinant (12)
          is an example of such attribute.

          Exercise 15.10: Substitute the unit matrix for  F  into (1) and verify that  F  is also a unit matrix in
                                                                    i 
                                               i
                                                                    j
                                               j
          this case. Interpret this fact.
          Exercise 15.11: Let x = e  for some basis e , e , e  in the space. Substitute this vector x into (7) and
                             i
                                           1
                                             2
                                               3
          by means of (4) derive the following formula:
                                               3
                                                 j
                                        F(e ) =   F e .                          ...(13)
                                                  j
                                                 i
                                           i
                                              j 1
                                               
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