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11.2 Finite Volume Method                                 211



                                 coefficients  are  derived  depending  on  the  algorithms  selected.
                                 Common algorithms are the central differencing, upwinding, hybrid
                                 differencing,  power-law,  and  QUICK  algorithms.    Understanding
                                 these algorithms and applying them appropriately can improve the
                                 solution accuracy.
                                            From the equations for determining the velocity com-
                                 ponents u and v of any p cell above, the computational approach to
                                 find the solutions should be an iteration process.  The process starts
                                 from  an  initial  guess  of  the  flow  solution  for  the  entire  domain.
                                 The  iteration  process  is  performed  and  terminated  when  a
                                 converged solution is obtained.  One of the efficient processes is
                                 the SIMPLE (Semi-Implicit Method for Pressure-Linked Equation)
                                 method.  The method is briefly explained in the following section.


                                        11.2.2  SIMPLE Method

                                            The SIMPLE method consists of the three main steps as
                                 follows.

                                                                         
                                                                             
                                 Step1  Assume  the  velocity  components u , v  and  the  pressure
                                   
                                 p  for  all  cells  in  the  flow  domain.    Then,  determine  the  new
                                 velocity components u  and v  from,
                                                            
                                                      
                                                    au     u P   P   au nb      p  x     A
                                                                  u
                                                                     
                                                                                u
                                                                  nb
                                 and                av       v PP   av       p  y     A
                                                       
                                                                                v
                                                                  v
                                                                        
                                                                  nb nb

                                 Step 2  Assign  u ,  v  and  p  as  the  corrections  which  are  the
                                 differences between the correct solutions and assumed solutions in
                                 step 1, i.e.,
                                                                    
                                                                                      
                                                   
                                                                 
                                        u       uu    ;    v       vv    ;     p      p   p
                                                
                                 Then, determine the velocity components u and v from,
                                                                      u
                                                      u      u       A  p
                                                                 
                                                        P
                                                               P
                                                                    a P u  x 
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