Research Article
An Application of Homotopy Perturbation Method to Fractional-Order Thin Film Flow of the Johnson–Segalman Fluid Model
Table 3
Solution and residual error for
keeping
fixed in lifting.
| | | | | | | Res error | | Res error | | Res error |
| | 0.1 | 0.999905 | −7.23543 × 10−27 | 0.99905 | −6.29219 × 10−22 | 0.9905 | −6.30818 × 10−17 | | 0.2 | 0.99982 | −3.63823 × 10−27 | 0.9982 | −4.18657 × 10−22 | 0.982 | −4.18849 × 10−17 | | 0.3 | 0.999745 | −2.86435 × 10−27 | 0.99745 | −2.5807 × 10−22 | 0.9745 | −2.57976 × 10−17 | | 0.4 | 0.99968 | −1.51698 × 10−27 | 0.9968 | −1.46438 × 10−22 | 0.968 | −1.46541 × 10−18 | | 0.5 | 0.999625 | −8.70705 × 10−28 | 0.99625 | −7.53253 × 10−23 | 0.9625 | −7.52476 × 10−18 | | 0.6 | 0.99958 | −4.61286 × 10−28 | 0.9958 | −3.40645 × 10−23 | 0.958 | −3.37798 × 10−18 | | 0.7 | 0.999545 | −4.34662 × 10−28 | 0.99545 | −1.28478 × 10−23 | 0.9545 | −1.25942 × 10−18 | | 0.8 | 0.99952 | −4.00347 × 10−29 | 0.9952 | −3.70343 × 10−24 | 0.952 | −3.64878 × 10−19 | | 0.9 | 0.999505 | −1.66647 × 10−29 | 0.99505 | −1.07941 × 10−24 | 0.9505 | −8.14999 × 10−20 | | 1. | 0.9995 | 9.95937 × 10−30 | 0.995 | −8.78476 × 10−26 | 0.95 | −8.71776 × 10−21 |
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