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Original Article

Tri-prong scheme for regularized long wave equationFootnote

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Pages 68-77 | Received 03 Apr 2013, Accepted 31 Aug 2014, Published online: 27 Mar 2018

Figures & data

Figure 1d 4th- order approximation solution by present technique when h = 0.4476 in Example 4.1.

Figure 1e 4th-order approximation solution by standard VIM in Example 4.1.

Figure 4 Error analysis of solution of Eq. Equation(13) by finite difference method.

Figure 5a Absolute error for the 3rd-order approximation by standard VIM for u3(x,t) in Example 4.3.

Figure 5b Absolute error for the 3rd-order approximation by present technique when h = 0.2712 in Example 4.3.

Figure 6 Error analysis of solution of Example 4.3 by finite difference method.

Figure 1a Absolute error for the 4th-order approximation by standard VIM in Example 4.1.

Figure 1b Absolute error for the 4th-order approximation by present technique when h = 0.4476 in Example 4.1.

Figure 1c Exact solution for Example 4.1.

Figure 1f The plot of numerical results for u4(x,t) by standard VIM and present technique in comparison with the exact solution at t = 3 s, in Example 4.1.

Figure 2 Error analysis of solution of Eq. Equation(7) by finite difference method.

Figure 3a Absolute error for the 3rd-order approximation by standard VIM for u3(x,t) in Example 4.2.

Figure 3b Absolute error for the 3rd-order approximation by present technique when h = 0.025 in Example 4.2.

Figure 7 Travelling wave solution of Eq. Equation(1) for different values of parameters.

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