Research Article
A New Hybrid PRPFR Conjugate Gradient Method for Solving Nonlinear Monotone Equations and Image Restoration Problems
Table 3
Test results of the modified PRP algorithm.
| No. | Dim | Modified PRP algorithm | NI/NF | CPU | GN |
| 1 | 3000 | 38/389 | 0.234375 | 9.84E − 06 | 9000 | 21/250 | 1.6875 | 9.08E − 06 | 30000 | 20/271 | 4.203125 | 9.70E − 06 | 90000 | 10/155 | 3.78125 | 8.09E − 06 | 2 | 3000 | 18/47 | 0.0625 | 9.87E − 06 | 9000 | 18/47 | 0.6875 | 5.67E − 06 | 30000 | 17/44 | 0.90625 | 6.32E − 06 | 90000 | 15/39 | 1.703125 | 7.76E − 06 | 3 | 3000 | 9999/10404 | 10.984375 | 2.83E − 05 | 9000 | 9999/10873 | 190.140625 | 5.01E − 05 | 30000 | 9999/11895 | 435.296875 | 3.15E − 05 | 90000 | 9999/13913 | 839.734375 | 4.85E − 05 | 4 | 3000 | 42/194 | 0.109375 | 5.69E − 09 | 9000 | 66/352 | 3 | 3.37E − 06 | 30000 | 121/748 | 13.28125 | 4.61E − 07 | 90000 | 218/1538 | 41.4375 | 7.05E − 08 | 5 | 3000 | 67/280 | 0.1875 | 5.90E − 06 | 9000 | 90/393 | 3.171875 | 8.05E − 06 | 30000 | 111/541 | 9.453125 | 7.88E − 06 | 90000 | 139/787 | 24.28125 | 6.16E − 06 | 6 | 3000 | 75/517 | 0.265625 | 6.67E − 06 | 9000 | 107/840 | 7.203125 | 3.88E − 06 | 30000 | 165/1487 | 26.96875 | 7.27E − 06 | 90000 | 252/2537 | 77.25 | 8.93E − 06 | 7 | 3000 | 39/138 | 0.046875 | 6.65E − 06 | 9000 | 56/245 | 2.84375 | 6.87E − 06 | 30000 | 89/477 | 7.53125 | 5.70E − 06 | 90000 | 139/869 | 25.09375 | 6.00E − 06 | 8 | 3000 | 1/2 | 0.03125 | 0.00E + 00 | 9000 | 1/2 | 0 | 0.00E + 00 | 30000 | 1/2 | 0.0625 | 0.00E + 00 | 90000 | 1/2 | 0.15625 | 0.00E + 00 | 9 | 3000 | 5544/43870 | 12.765625 | 9.85E − 06 | 9000 | 5832/49309 | 347.203125 | 9.84E − 06 | 30000 | 6424/60507 | 960.546875 | 9.68E − 06 | 90000 | 7445/80662 | 1983.578125 | 9.83E − 06 | 10 | 3000 | 768/4997 | 1.515625 | 9.84E − 06 | 9000 | 881/6108 | 44.8125 | 9.28E − 06 | 30000 | 1043/8118 | 121.359375 | 9.89E − 06 | 90000 | 1343/11835 | 301.625 | 8.92E − 06 | 11 | 3000 | 512/3345 | 1.84375 | 9.85E − 06 | 9000 | 545/3646 | 23.953125 | 9.95E − 06 | 30000 | 1122/7498 | 119.3125 | 9.90E − 06 | 90000 | 1229/8722 | 223.140625 | 9.54E − 06 | 12 | 3000 | 16/48 | 0.078125 | 7.22E − 06 | 9000 | 13/39 | 0.5625 | 8.96E − 06 | 30000 | 11/33 | 1.390625 | 8.41E − 06 | 90000 | 10/30 | 1.671875 | 7.92E − 06 |
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