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On the rational sine-Gordon solution of the forced KdV equation Cover

On the rational sine-Gordon solution of the forced KdV equation

By: Wei Gao and  Carlo Cattani  
Open Access
|Feb 2026

Figures & Tables

Fig. 1

Parametric nature wave behaviors for equation (18) at (a) : τ(t) = sin(t), (b) : τ(t) = cos(t), (c) : τ(t) = tan(t) and (d) : τ(t) = cot(t).
Parametric nature wave behaviors for equation (18) at (a) : τ(t) = sin(t), (b) : τ(t) = cos(t), (c) : τ(t) = tan(t) and (d) : τ(t) = cot(t).

Fig. 2

Parametric nature wave behaviors for equation (20) at (a) : F(t) = sin(t), (b) : F(t) = cos(t), (c) : F(t) = tan(t) and (d) : F(t) = cot(t), and also τ(t) = cos(t).
Parametric nature wave behaviors for equation (20) at (a) : F(t) = sin(t), (b) : F(t) = cos(t), (c) : F(t) = tan(t) and (d) : F(t) = cot(t), and also τ(t) = cos(t).

Fig. 3

Parametric nature wave behaviors for equation (22) at F(t) = sin(t) cos(t) tan(t) is (a)3D, and (b) Contour, respectively, and also τ = cos(t).
Parametric nature wave behaviors for equation (22) at F(t) = sin(t) cos(t) tan(t) is (a)3D, and (b) Contour, respectively, and also τ = cos(t).

Fig. 4

2D wave behavior for equation (22) at F(t) = sin(t) cos(t) tan(t) with 2D, and t = 8.5, and also τ(t) = cos(t), τ(t) = sin(t), respectively.
2D wave behavior for equation (22) at F(t) = sin(t) cos(t) tan(t) with 2D, and t = 8.5, and also τ(t) = cos(t), τ(t) = sin(t), respectively.

Fig. 5

The wave way behavior for equation (25) at τ(t) = cos(t) with a) 3D and b) Contour.
The wave way behavior for equation (25) at τ(t) = cos(t) with a) 3D and b) Contour.
Language: English
Submitted on: Nov 8, 2024
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Accepted on: Dec 2, 2024
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Published on: Feb 2, 2026
Published by: Harran University
In partnership with: Paradigm Publishing Services
Publication frequency: 2 issues per year

© 2026 Wei Gao, Carlo Cattani, published by Harran University
This work is licensed under the Creative Commons Attribution 4.0 License.

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