Research Article
On Fractional Newton-Type Method for Nonlinear Problems
Table 1
First-order FNR and second-order FNR results for
with Caputo derivative and initial guess
.
| | | | | | |
| N-R | 1 | 4.00000000 | 1.46549e − 14 | 2.84217e − 14 | 10 | N-R | 1 | 4.00000000 | 8.38330e − 18 | 0.00000e + 00 | 8 | N-R | 0.98 | 4.00000000 | 9.65937e − 09 | 1.23761e − 08 | 17 | N-R | 0.98 | 4.00000000 | 8.93729e − 09 | 1.14804e − 08 | 17 | N-R | 0.96 | 3.99999999 | 6.31251e − 09 | 2.16859e − 08 | 28 | N-R | 0.96 | 3.99999999 | 8.36562e − 09 | 2.82381e − 08 | 27 | N-R | 0.94 | 3.99999997 | 7.76010e − 09 | 5.26373e − 08 | 41 | N-R | 0.94 | 3.99999997 | 8.85140e − 09 | 5.94304e − 08 | 40 | N-R | 0.92 | 3.99999994 | 9.40705e − 09 | 1.13137e − 07 | 58 | N-R | 0.92 | 3.99999995 | 8.97743e − 09 | 1.08442e − 07 | 57 | N-R | 0.9 | 3.99999990 | 9.68422e − 09 | 1.98513e − 07 | 82 | N-R | 0.9 | 3.99999990 | 9.48429e − 09 | 1.94823e − 07 | 80 | N-R | 0.88 | 3.99999984 | 9.37726e − 09 | 3.20376e − 07 | 116 | N-R | 0.88 | 3.99999983 | 9.85311e − 09 | 3.34523e − 07 | 112 | N-R | 0.86 | 3.99999973 | 9.78559e − 09 | 5.41971e − 07 | 162 | N-R | 0.86 | 3.99999973 | 9.66965e − 09 | 5.36477e − 07 | 158 | N-R | 0.84 | 3.99999956 | 9.88726e − 09 | 8.80428e − 07 | 227 | N-R | 0.84 | 3.99999956 | 9.82503e − 09 | 8.75790e − 07 | 222 | N-R | 0.82 | 3.99999930 | 9.84707e − 09 | 1.40112e − 06 | 319 | N-R | 0.82 | 3.99999930 | 9.85142e − 09 | 1.40163e − 06 | 313 | N-R | 0.8 | 3.99999888 | 9.90469e − 09 | 2.23380e − 06 | 448 | N-R | 0.8 | 3.99999888 | 9.93908e − 09 | 2.23999e − 06 | 441 | N-R | 0.78 | 3.99999600 | 2.83959e − 08 | 8.00875e − 06 | 500 | N-R | 0.78 | 3.99999620 | 2.65292e − 08 | 7.59583e − 06 | 500 | N-R | 0.76 | 3.99998275 | 1.10103e − 07 | 3.44952e − 05 | 500 | N-R | 0.76 | 3.99998367 | 1.02423e − 07 | 3.26542e − 05 | 500 | N-R | 0.74 | 3.99993896 | 3.53606e − 07 | 1.22080e − 04 | 500 | N-R | 0.74 | 3.99994240 | 3.26873e − 07 | 1.15193e − 04 | 500 | N-R | 0.72 | 3.99981521 | 9.78747e − 07 | 3.69503e − 04 | 500 | N-R | 0.72 | 3.99982645 | 8.96989e − 07 | 3.47038e − 04 | 500 | N-R | 0.7 | 3.99950671 | 2.40749e − 06 | 9.86099e − 04 | 500 | N-R | 0.7 | 3.99953965 | 2.18121e − 06 | 9.20282e − 04 | 500 |
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