Page 126 - Numerical Methods for Chemical Engineering
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Applying Gershgorin’s theorem                                       115



                  any vector as a linear combination of the eigenvectors, and in particular, the error associated
                  with the initial guess can be written as
                                      ε [0]  = c 1 w [1]  + c 2 w [2]  + ··· + c N w [N]  (3.74)

                  After the first iteration, the error is


                       ε [1]  = B −1 (B − A)ε [0]  = B −1 (B − A) c 1 w [1]  + c 2 w [2]  +· · · + c N w [N]
                           = c 1 B −1 (B − A)w [1]  + c 2 B −1 (B − A)w [2]  +· · · + c N B −1 (B − A)w [N]
                           = c 1 λ 1 w [1]  + c 2 λ 2 w [2]  +· · · + c N λ N w [N]  (3.75)

                  After the second iteration, the error is

                     ε [2]  = B −1 (B − A)e [1]  = B −1 (B − A) c 1 λ 1 w  [1]  + c 2 λ 2 w  [2]  +· · · + c N λ N w  [N]
                                                      2
                              2
                                        2
                         = c 1 λ w  [1]  + c 2 λ w  [2]  +· · · + c N λ w  [N]       (3.76)
                                                      N
                              1
                                        2
                  After k iterations, the error is
                                                                   k
                                            k
                                                     k
                                   ε [k]  = c 1 λ w [1]  + c 2 λ w [2]  +· · · + c N λ w [N]  (3.77)
                                            1        2             N
                  If all eigenvalues of B −1 (B − A) have moduli less than 1, |λ j | < 1, then
                                                      2     3
                                         1 > |λ j | > |λ j | > |λ j | > ···          (3.78)
                                                                           [k]
                                k
                  and lim k→∞ |c j λ |= 0 for finite {c 1 , c 2 ,..., c N }, so that lim k→∞ 	ε 	= 0. For the B
                                j
                  of (3.71), we write B −1 (B − A) explicitly,
                                                                           
                                          0        (−a 12 /a 11 )  ... (−a 1N /a 11 )
                                       (−a 21 /a 22 )  0      ... (−a 2N /a 22 )
                                                                           
                       B −1               .           .               .            (3.79)
                                           .           .               .    
                           (B − A) = 
                                          .           .               .    
                                      (−a N1 /a NN )(−a N2 /a NN )  ...  0
                  By Gershgorin’s theorem, each eigenvalue λ j of B −1 (B − A) must satisfy the following
                  inequality for some k = 1, 2,..., N:
                                            N                   N
                                           	                1
                                      |λ j |≤  |−a km /a kk |=    |a km |            (3.80)
                                                           |a kk |
                                            m=1                m=1
                                           m =k                m =k
                  Therefore, we can ensure that all |λ j | < 1, if for every k = 1, 2,..., N:
                                           N             N
                                       1
                                             |a km | < 1 ⇒  |a km | < |a kk |        (3.81)
                                      |a kk |
                                           m=1           m=1
                                          m =k          m =k
                  That is, for every row of A, the magnitude of the diagonal element is greater than the sum
                  of the magnitudes of all off-diagonal elements. A matrix for which this property holds is
                  said to be strictly diagonally dominant. For such a matrix, the Jacobi method converges to
                                   [0]
                  a solution from any x .
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