Research Article
Runge-Kutta Integration of the Equal Width Wave Equation Using the Method of Lines
Table 6
Invariant for the undular bore with
.
| Time | Present method | [34] | | | | | | |
| 100 | 2.49294 | 0.24107 | 0.0236792 | 2.503585 | 0.242143 | 0.023787 | 200 | 2.99292 | 0.307831 | 0.0312025 | 3.003583 | 0.308783 | 0.031279 | 300 | 3.49292 | 0.374669 | 0.0387447 | 3.503573 | 0.375402 | 0.038765 | 400 | 3.99292 | 0.441516 | 0.0462886 | 4.003564 | 0.442020 | 0.046250 | 500 | 4.49292 | 0.508363 | 0.0538328 | 4.503559 | 0.508638 | 0.053735 | 600 | 4.99292 | 0.575211 | 0.0613769 | 5.003568 | 0.575259 | 0.061221 | 700 | 5.49292 | 0.64206 | 0.0689211 | 5.503578 | 0.641880 | 0.068707 | 800 | 5.99292 | 0.708908 | 0.0764653 | 6.003578 | 0.708498 | 0.076192 |
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