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                           CB908/Date
            0521853265c05
                        5.3 METHOD OF SOLUTION
                        ADI Method      0 521 85326 5                              May 20, 2005  12:28 121
                        The ADI method is a line-by-line method in which Equation 5.65 is first solved for
                        all j = constant lines (say). This is called the j-direction sweep. The solution thus
                        obtained may be called the   l+1/2  solution. Now, using this solution, Equation 5.65
                        is again solved for i = constant lines to generate the   l+1  solution. This is called
                        the i-direction sweep. The implementation details are as follows. For the j sweep,
                        Equation 5.65 is written as
                                                l+1/2         l+1/2         l+1/2
                                (AP i, j + Sp i, j )   = AE i, j    + AW i, j    + SJ i, j ,  (5.66)
                                                i, j          i+1, j        i−1, j
                        where

                                         SJ i, j = AN i, j   l  + AS i, j   l  + Su i, j .  (5.67)
                                                       i, j+1       i, j−1
                        Now, dividing by coefficient of   i, j , Equation 5.66 for fixed j can also be written as

                                   l+1/2      l+1/2     l+1/2
                                       = a i      + b i      + c i ,  i = 2,..., IN − 1,   (5.68)
                                   i          i+1       i−1
                        where a i = AE i, j /(AP i, j + Sp i, j ), b i = AW i, j /(AP i, j + Sp i, j ), and c i = SJ i, j /
                        (AP i, j + Sp i, j ).
                           It is clear that Equation 5.68 can be solved using TDMA for each j = 2to
                         JN − 1 to complete the j sweep. To execute the i sweep, Equation 5.65 is again
                        written as
                                                 l+1          l+1          l+1
                                  (AP i, j + Sp i, j )   = AN i, j    + AS i, j    + SI i, j ,  (5.69)
                                                 i, j         i, j+1       i, j−1
                        where
                                                      l+1/2         l+1/2
                                        SI i, j = AE i, j    + AW i, j    + Su i, j .      (5.70)
                                                      i+1, j         i−1, j
                        Equation 5.69 can again be cast in the form of Equation 5.68 and subsequently
                        solved for each i = constant line by TDMA. The two sweeps complete one iteration.
                        Thus, in the ADI method, the domain is swept twice per iteration. In spite of this,
                        the procedure proves to be much faster than the GS procedure. In Chapter 9, some
                        additional methods for convergence enhancement are described.


                        5.3.2 Evaluation of Residuals

                        The convergence of the iterative procedure is checked by evaluating the imbalance
                        in Equation 5.12. Thus, for each  , we evaluate

                                           ⎡                                  ⎤ 0.5
                                                                             2


                                      R   =  ⎣       AP   P −     A k   k − D  ⎦  .        (5.71)
                                             all nodes         k
                        When the maximum value of R   among all  s is less than the convergence criterion
                                   −5
                        (typically 10 ), the iteration is stopped. Often, R   is normalized with a reference
                        quantity specific to a problem having units of AP  .
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