Preconditioner


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Table 1: The size of the matrices A, B, C and D.

IVS model

l

n

m

size of A

size of B

size of C

size of D

Test 2

1503

14

1503 ×1503

1503 × 14

14× 1503

14× 14

Test 3

127760

380

127760×127760

127760× 380

380× 127760

380× 380

Generic information of the test problems, including n and m, are given in Table 1.




Table 2: Numerical results of Schur complement approximation.

Sˆ

Test 1

CPUShur: 9.76e-03

Test 2

CPUShur: 1.71e+01

In Table 2, we reported the results of Schur complement approximation in terms of CPU times.




Table 3: Numerical results for the three preconditioned GMRES methods.

Test




Pα,Sˆ

PT

PD

Test1

Iter

8

23

10




CPU

1.70e-03

5.65e-03

2.66e-03




RES

3.02e-14

3.79e-13

1.72e-12

Test2

Iter
CPU RES

2
1.36
7.94e-22









Table 4: Numerical results for the three preconditioned FGMRES methods.

Test




Pα,Sˆ

PT

PD

Test1

Iter

12

30

29




CPU

2.86e-03

6.79e-03

4.78e-03




RES

2.20e-24

2.00e-11

2.00e-11

Test2

Iter
CPU RES

2
6.12e-01
5.37e-26











Table 5: Numerical results for the three preconditioned BICGSTAB methods.

Test




Pα,Sˆ

PT

PD

Test1

Iter

15

22

15




CPU

3.68e-03

5.59e-03

3.40e-03




RES

3.83e-15

6.75e-15

5.40e-15

Test2

Iter
CPU RES

2
5.94e-01
6.27e-28









In Tables 3, 4 and 5 we report the results for the preconditioned GMRES, FGMRES and BICGSTAB iterative methods. From numerical results listed in Tables, we can


conclude that the Pα,Sˆ preconditioned GMRES, FGMRES and BICGSTAB methods

P P
require less iterations and has faster CPU times than PT and PD in all trials. The PD and T preconditioner do not converge in case of Test 2, whereas the α,Sˆ preconditioner converge in case of both Test 1 and Test 2.


  1. Conclusion


In the present work, we have developed and studied numerically parallel block pre- conditioner for a class of linear systems arising from IVS model. Parallel block precon- ditioner have been proposed based on the approximate Schur complement (Block-Schur) and on a regularization technique. Several numerical experiments have been conducted in parallel on a parallel computer architecture in order to study the performance of the iterative solvers in terms of Krylov subspace methods iterations and computational time.

P P
Numerical results worked out in Section 5 (Tables 3, 4 and 5) reveal that the regular- ized parallel block preconditioned Krylov subspace methods with suitable parameter has great superiority compared with D and T preconditioned Krylov subspace meth- ods in terms of the iterations and CPU times, and illustrate that the regularized parallel block preconditioned Krylov method is a very efficient method for solving (1).
However, I should mention that this new preconditioner involved the parameter α. How to choose the optimal parameters for the regularized preconditioner is a very practical and interesting problem that needs to be further in-depth studied.


References


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  2. E. Anderson, et al., 1999. LAPACK Users; Guide Third., Philadelphia, PA: Society for Industrial and Applied Mathematics.

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  6. V. Duwig, A. Barbu, New MFVISC Code for Copper and Helium in Iron under Irradiation. Research Report D-P124, European Project PERFECT, 2004.

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