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Table 1.

Comparison of our solutions and Wazwaz [16] solutions by sine-cosine scheme.

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Table 1 Expand

Table 2.

Comparison of our solutions and Wazwaz [16] solutions obtained by the tanh method.

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Table 2 Expand

Fig 1.

Travelling wave profile of .

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Fig 1 Expand

Fig 2.

Effect of nonlinear parameter .

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Fig 2 Expand

Fig 3.

Schematic illustration of dark soliton type amplitude of KP-BBM equation corresponds to the solution .

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Fig 3 Expand

Fig 4.

Schematic illustration of bright soliton type amplitude of KP-BBM equation corresponds to the solution .

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Fig 4 Expand

Fig 5.

Effects of nonlinear parameter .

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Fig 5 Expand

Fig 6.

The phase portrait and associated solution of the planar dynamical system (4.1) are presented for selected parameters as .

The equilibrium point (0, 0) is an unstable saddle.

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Fig 6 Expand

Fig 7.

The phase portrait and associated solution of the planar dynamical system (4.1) are presented for selected parameters as .

The equilibrium point (0,0) is an unstable saddle, while the equilibrium point at (−0.95,0) is characterized as a centre.

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Fig 7 Expand

Fig 8.

The phase portrait and associated solution of the planar dynamical system (4.1) are presented for selected parameters as .

The equilibrium point (0,0) is characterized as a centre.

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Fig 8 Expand

Fig 9.

The phase portrait and associated solution of the planar dynamical system (4.1) are presented for the selected parameter as .

The equilibrium point (0,0) is identified as a centre, while the equilibrium point at (−1.28,0) is characterized as an unstable saddle.

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Fig 9 Expand