Theory and Modern Applications
From: A reliable technique for fractional modified Boussinesq and approximate long wave equations
(x,t) | \(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{ADM}} \vert \) | \(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{VIM}} \vert \) | \(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{LADM}} \vert \) | \(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{CRFDTM}} \vert \) | \(\vert {u}_{\mathrm{Exact}} - {u}_{{q}\text{-}\mathrm{HATM}}^{ ( {3} )} \vert \) |
---|---|---|---|---|---|
(0.1,0.1) | 8.02989 × 10−6 | 1.23033 × 10−4 | 7.10000 × 10−9 | 2.77556 × 10−17 | 2.77556 × 10−17 |
(0.1,0.3) | 7.38281 × 10−6 | 3.69597 × 10−4 | 6.50000 × 10−9 | 2.77556 × 10−17 | 2.77556 × 10−17 |
(0.1,0.5) | 6.79923 × 10−6 | 4.92780 × 10−4 | 5.90000 × 10−9 | 3.33067 × 10−16 | 3.33067 × 10−16 |
(0.2,0.1) | 3.23228 × 10−5 | 1.69274 × 10−5 | 2.82000 × 10−8 | 2.77556 × 10−17 | 2.77556 × 10−17 |
(0.2,0.3) | 297172 × 10−5 | 1.89210 × 10−4 | 2.59000 × 10−8 | 4.16334 × 10−17 | 4.16334 × 10−17 |
(0.2,0.5) | 2.73673 × 10−5 | 1.55176 × 10−4 | 2.41000 × 10−8 | 3.60822 × 10−17 | 3.60822 × 10−17 |
(0.3,0.1) | 7.32051 × 10−5 | 1.12345 × 10−5 | 6.33670 × 10−8 | 1.38778 × 10−17 | 1.38778 × 10−17 |
(0.3,0.3) | 6.73006 × 10−5 | 6.55176 × 10−5 | 5.85000 × 10−8 | 2.77556 × 10−17 | 2.77556 × 10−17 |
(0.3,0.5) | 6.19760 × 10−5 | 2.12346 × 10−5 | 5.40000 × 10−8 | 3.19189 × 10−16 | 3.19189 × 10−16 |
(0.4,0.1) | 1.31032 × 10−4 | 7.36513 × 10−5 | 1.12400 × 10−7 | 1.38778 × 10−17 | 1.38778 × 10−17 |
(0.4,0.3) | 1.20455 × 10−4 | 9.5016 × 10−5 | 1.03900 × 10−7 | 2.77556 × 10−17 | 2.77556 × 10−17 |
(0.4,0.5) | 1.10919 × 10−4 | 8.23160 × 10−4 | 9.61000 × 10−8 | 3.19189 × 10−16 | 3.19189 × 10−16 |
(0.5,0.1) | 2.06186 × 10−4 | 5.55176 × 10−5 | 1.75500 × 10−7 | 0 | 0 |
(0.5,0.3) | 1.89528 × 10−4 | 3.21715 × 10−6 | 1.62200 × 10−7 | 5.55112 × 10−17 | 5.55112 × 10−17 |
(0.5,0.5) | 1.74510 × 10−4 | 2.00176 × 10−5 | 1.5010 × 10−7 | 3.19189 × 10−16 | 3.19189 × 10−16 |