Research Article
On Fractional Newton-Type Method for Nonlinear Problems
Table 2
First-order FNR and second-order FNR results for
with Riemann–Liouville derivative and initial estimation
.
| | | | | | |
| 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 | 4.68492e − 09 | 4.77773e − 09 | 16 | N-R | 0.98 | 4.00000000 | 6.74956e − 09 | 6.72255e − 09 | 15 | N-R | 0.96 | 3.99999999 | 9.31417e − 09 | 2.26436e − 08 | 20 | N-R | 0.96 | 3.99999999 | 6.15820e − 09 | 1.54268e − 08 | 21 | N-R | 0.94 | 3.99999999 | 8.41656e − 09 | 3.90606e − 08 | 28 | N-R | 0.94 | 3.99999998 | 9.57249e − 09 | 4.39009e − 08 | 28 | N-R | 0.92 | 3.99999997 | 9.83530e − 09 | 7.65395e − 08 | 35 | N-R | 0.92 | 3.99999997 | 8.10233e − 09 | 6.42359e − 08 | 38 | N-R | 0.9 | 3.99999994 | 9.40993e − 09 | 1.18506e − 07 | 49 | N-R | 0.9 | 3.99999994 | 9.37709e − 09 | 1.18142e − 07 | 47 | N-R | 0.88 | 3.99999991 | 9.61954e − 09 | 1.88983e − 07 | 65 | N-R | 0.88 | 3.99999990 | 9.84849e − 09 | 1.92880e − 07 | 64 | N-R | 0.86 | 3.99999986 | 9.60193e − 09 | 2.89676e − 07 | 86 | N-R | 0.86 | 3.99999985 | 9.96806e − 09 | 2.99047e − 07 | 85 | N-R | 0.84 | 3.99999978 | 9.53412e − 09 | 4.36870e − 07 | 114 | N-R | 0.84 | 3.99999978 | 9.64049e − 09 | 4.40927e − 07 | 113 | N-R | 0.82 | 3.99999966 | 9.94288e − 09 | 6.80455e − 07 | 150 | N-R | 0.82 | 3.99999966 | 9.91663e − 09 | 6.78992e − 07 | 149 | N-R | 0.8 | 3.99999949 | 9.98970e − 09 | 1.02156e − 06 | 199 | N-R | 0.8 | 3.99999950 | 9.78692e − 09 | 1.00502e − 06 | 199 | N-R | 0.78 | 3.99999924 | 9.96299e − 09 | 1.51847e − 06 | 265 | N-R | 0.78 | 3.99999924 | 9.98659e − 09 | 1.52126e − 06 | 264 | N-R | 0.76 | 3.99999888 | 9.90426e − 09 | 2.24483e − 06 | 354 | N-R | 0.76 | 3.99999887 | 9.98421e − 09 | 2.25855e − 06 | 353 | N-R | 0.74 | 3.99999833 | 9.92379e − 09 | 3.33049e − 06 | 473 | N-R | 0.74 | 3.99999833 | 9.94614e − 09 | 3.33603e − 06 | 473 | N-R | 0.72 | 3.99999551 | 2.29296e − 08 | 8.98833e − 06 | 500 | N-R | 0.72 | 3.99999548 | 2.30961e − 08 | 9.03519e − 06 | 500 | N-R | 0.7 | 3.99998762 | 5.73722e − 08 | 2.47620e − 05 | 500 | N-R | 0.7 | 3.99998750 | 5.81547e − 08 | 2.49976e − 05 | 500 |
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