Research article Special Issues

A physics-informed neural network approach for the one-dimensional wave equation: data-driven solution with Fibonacci polynomial activation functions

  • Published: 21 September 2026
  • MSC : 65M70, 68T07, 35L05, 11B39

  • In this study, a data-driven computational framework based on Physics-Informed Neural Networks (PINNs) was proposed for the numerical solution of the one-dimensional wave equation. Conventional numerical methodologies, including finite difference and finite element schemes, necessitated intricate discretization processes and became computationally onerous for high-resolution simulations. The proposed PINN framework reinterprets the problem as a supervised learning task that learns the underlying physical behavior directly from data in a mesh-free manner, using training sets generated from the governing equation together with the initial and boundary conditions. The central contribution of this study is the integration of Fibonacci polynomials as activation functions within the network architecture. The continuous and structurally rich mathematical properties of Fibonacci polynomials enhance the representational capacity of the network relative to conventional activation functions such as Tanh, improving learning dynamics, training stability, and accuracy in capturing the oscillatory nature of wave phenomena. The performance of the model was evaluated through error analysis, utilizing standard metrics such as Mean Squared Error (MSE) and Relative-L2 error, in comparison to known reference solutions. The proposed Fibonacci-PINN was directly compared with a standard Tanh-based PINN under identical training conditions. The findings demonstrated that the Fibonacci-PINN consistently attains reduced prediction error in comparison to the standard Tanh-PINN across all three numerical illustrations examined, thereby evidencing enhanced approximation precision with diminished computational demands. In contradistinction to conventional discretization-based methodologies, the model engenders smooth, continuous functional outputs, thereby facilitating efficacious visualization of wave propagation. In this study, we demonstrate the efficiency and flexibility of combining artificial neural networks with structurally rich mathematical activation functions as a viable alternative.

    Citation: Ali Algan, Faruk Düşünceli. A physics-informed neural network approach for the one-dimensional wave equation: data-driven solution with Fibonacci polynomial activation functions[J]. AIMS Mathematics, 2026, 11(9): 30886-30903. doi: 10.3934/math.20261223

    Related Papers:

  • In this study, a data-driven computational framework based on Physics-Informed Neural Networks (PINNs) was proposed for the numerical solution of the one-dimensional wave equation. Conventional numerical methodologies, including finite difference and finite element schemes, necessitated intricate discretization processes and became computationally onerous for high-resolution simulations. The proposed PINN framework reinterprets the problem as a supervised learning task that learns the underlying physical behavior directly from data in a mesh-free manner, using training sets generated from the governing equation together with the initial and boundary conditions. The central contribution of this study is the integration of Fibonacci polynomials as activation functions within the network architecture. The continuous and structurally rich mathematical properties of Fibonacci polynomials enhance the representational capacity of the network relative to conventional activation functions such as Tanh, improving learning dynamics, training stability, and accuracy in capturing the oscillatory nature of wave phenomena. The performance of the model was evaluated through error analysis, utilizing standard metrics such as Mean Squared Error (MSE) and Relative-L2 error, in comparison to known reference solutions. The proposed Fibonacci-PINN was directly compared with a standard Tanh-based PINN under identical training conditions. The findings demonstrated that the Fibonacci-PINN consistently attains reduced prediction error in comparison to the standard Tanh-PINN across all three numerical illustrations examined, thereby evidencing enhanced approximation precision with diminished computational demands. In contradistinction to conventional discretization-based methodologies, the model engenders smooth, continuous functional outputs, thereby facilitating efficacious visualization of wave propagation. In this study, we demonstrate the efficiency and flexibility of combining artificial neural networks with structurally rich mathematical activation functions as a viable alternative.



    加载中


    [1] A. Raina, S. Natesan, A physics-informed neural network framework for tumor-immune interactions, metastatic invasion, and haptotaxis systems, Math. Methods Appl. Sci., 49 (2026), 4450–4475. https://doi.org/10.1002/mma.70355 doi: 10.1002/mma.70355
    [2] H. P. Wang, Q. Ye, Z. H. Zhang, J. G. Liu, Application of multivariate bilinear neural network method to a spatial symmetric nonlinear dispersive wave model in (2+1)-dimensions, Math. Methods Appl. Sci., 49 (2026), 9093–9114. https://doi.org/10.1002/mma.70516 doi: 10.1002/mma.70516
    [3] J. Muhammad, A. H. Tedjani, E. Hussain, U. Younas, Exploring the exact solutions to the nonlinear systems with neural networks method, Sci. Rep., 15 (2025), 36818. https://doi.org/10.1038/s41598-025-21095-2 doi: 10.1038/s41598-025-21095-2
    [4] F. Düşünceli, E. Çelik, Fractional approach for diffusion equations arising from oil pollution using the fractional natural decomposition method, Int. J. Quantum Chem., 125 (2025), e27529. https://doi.org/10.1002/qua.27529 doi: 10.1002/qua.27529
    [5] G. Seriani, S. P. Oliveira, Numerical modeling of mechanical wave propagation, Riv. Nuovo Cimento, 43 (2020), 459–514. https://doi.org/10.1007/s40766-020-00009-0 doi: 10.1007/s40766-020-00009-0
    [6] A. M. Attiya, E. M. Eldesouki, Numerical analysis for temporal and spectral responses of electromagnetic waves in spatially homogeneous time varying medium, Sci. Rep., 14 (2024), 15234. https://doi.org/10.1038/s41598-024-64874-z doi: 10.1038/s41598-024-64874-z
    [7] N. Bhangale, K. B. Kachhia, Fractional electromagnetic waves in plasma and dielectric media with Caputo generalized fractional derivative, Rev. Mex. Fís., 66 (2020), 848–855. https://doi.org/10.31349/revmexfis.66.848 doi: 10.31349/revmexfis.66.848
    [8] M. J. Alam, A. Ramady, M. S. Abbas, K. El-Rashidy, M. T. Azam, M. M. Miah, Numerical investigation of the wave equation for the convergence and stability analysis of vibrating strings, AppliedMath, 5 (2025), 18. https://doi.org/10.3390/appliedmath5010018 doi: 10.3390/appliedmath5010018
    [9] T. De Ryck, S. Mishra, Numerical analysis of physics-informed neural networks and related models in physics-informed machine learning, Acta Numer., 33 (2024), 633–713. https://doi.org/10.1017/S0962492923000089 doi: 10.1017/S0962492923000089
    [10] Z. Tao, H. Wang, F. Liu, Lnn-pinn: A unified physics-only training framework with liquid residual blocks, Comput. Phys. Commun., 326 (2026), 110237. https://doi.org/10.1016/j.cpc.2026.110237 doi: 10.1016/j.cpc.2026.110237
    [11] Y. Zhang, F. Liu, Noether-constrained physics-informed neural networks for the nonlinear Schrödinger equation, Phys. Lett. A, 589 (2026), 131802. https://doi.org/10.1016/j.physleta.2026.131802 doi: 10.1016/j.physleta.2026.131802
    [12] M. Qasim, T. Shahzad, F. Yao, M. Z. Baber, N. Ahmed, Nonlinear water wave dynamics of data-driven soliton solutions for the Kakutani–Matsuuchi model in Ocean Engineering, Ocean Eng., 365 (2026), 127401. https://doi.org/10.1016/j.oceaneng.2026.127401 doi: 10.1016/j.oceaneng.2026.127401
    [13] M. Z. Baber, F. Yao, M. Qasim, Rich spectrum of data-driven soliton phenomena by using the advanced artificial neural networking, Chaos, Soliton. Fract., 210 (2026), 118736. https://doi.org/10.1016/j.chaos.2026.118736 doi: 10.1016/j.chaos.2026.118736
    [14] M. Qasim, A. Shafee, F. Yao, M. Z. Baber, Dynamics of soliton solutions for the (3+1)-dimensional CTFZK equation in plasma physics using an advanced neural networking approach, Z. Angew. Math. Phys., 77 (2026), 27. https://doi.org/10.1007/s00033-025-02682-9 doi: 10.1007/s00033-025-02682-9
    [15] M. Qasim, A. Shafee, F. Yao, M. Z. Baber, Y. Yildirim, B. Ceesay, et al., Lump and breather interaction with different soliton solutions for the generalized doubly dispersive equation by embedded the neural networks, Sci. Rep., 16 (2026), 20665. https://doi.org/10.1038/s41598-026-51557-0 doi: 10.1038/s41598-026-51557-0
    [16] D. Sana, Approximating the wave equation via physics-informed neural networks: Various forward and inverse problems, Internship report, Friedrich-Alexander-Universität Erlangen-Nürnberg, 2022. Available from: https://dcn.nat.fau.eu/wp-content/uploads/FAUMoD_DaniaSana-InternReport_PINN.pdf.
    [17] S. Alkhadhr, M. Almekkawy, Wave equation modeling via physics-informed neural networks: Models of soft and hard constraints for initial and boundary conditions, Sensors, 23 (2023), 2792. https://doi.org/10.3390/s23052792 doi: 10.3390/s23052792
    [18] A. F. Ihsan, On the neural network solution of one-dimensional wave problem, J. RESTI (Rekayasa Sistem dan Teknologi Informasi), 5 (2021), 1106–1112. https://doi.org/10.29207/resti.v5i6.3565 doi: 10.29207/resti.v5i6.3565
    [19] A. R. Kambekar, M. C. Deo, Wave simulation and forecasting using wind time history and data-driven methods, Ships Offshore Struct., 5 (2010), 253–266. https://doi.org/10.1080/17445300903439223 doi: 10.1080/17445300903439223
    [20] K. D. Dwivedi, Rajeev, Numerical solution of fractional order advection reaction diffusion equation with Fibonacci neural network, Neural Process. Lett., 53 (2021), 2687–2699. https://doi.org/10.1007/s11063-021-10513-x doi: 10.1007/s11063-021-10513-x
    [21] İ. Karabayır, O. Akbilgic, N. Taş, A novel learning algorithm to optimize deep neural networks: evolved gradient direction optimizer (EVGO), IEEE Trans. Neural Networks Learn. Syst., 32 (2021), 685–694. https://doi.org/10.1109/TNNLS.2020.2979121 doi: 10.1109/TNNLS.2020.2979121
    [22] E. Seyyarer, F. Ayata, T. Uçkan, A. Karci, Applications and comparison of optimization algorithms used in deep learning, Comput. Sci., 5 (2020), 90–98.
    [23] A. F. Horadam, E. M. Horadam, Roots of recurrence-generated polynomials, Fibonacci Quarterly, 20 (1982), 219–226. https://doi.org/10.1080/00150517.1982.12429991 doi: 10.1080/00150517.1982.12429991
    [24] M. Asci, E. Gurel, Bivariate Gaussian Fibonacci and Lucas polynomials, Ars Comb., 109 (2013), 461–472.
    [25] E. Özkan, M. Taştan, A. Aydoğdu, Fibonacci sayılarının ailesinde 3-Fibonacci polinomları, Erzincan Univ. J. Sci. Technol., 12 (2019), 926–933. https://doi.org/10.18185/erzifbed.512100 doi: 10.18185/erzifbed.512100
    [26] P. D. Brubeck, Y. Nakatsukasa, L. N. Trefethen, Vandermonde with Arnoldi, SIAM Rev., 63 (2021), 405–415. https://doi.org/10.1137/19M130100X doi: 10.1137/19M130100X
    [27] L. N. Trefethen, Approximation theory and approximation practice, Society for Industrial and Applied Mathematics (SIAM), Philadelphia, 2013.
  • Reader Comments
  • © 2026 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(59) PDF downloads(21) Cited by(0)

Article outline

Figures and Tables

Figures(6)  /  Tables(9)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog