Research article Special Issues

An immersed boundary neural network for solving elliptic equations with singular forces on arbitrary domains

  • Received: 09 August 2020 Accepted: 02 November 2020 Published: 18 November 2020
  • In this paper, we present a deep learning framework for solving two-dimensional elliptic equations with singular forces on arbitrary domains. This work follows the ideas of the physical-inform neural networks to approximate the solutions and the immersed boundary method to deal with the singularity on an interface. Numerical simulations of elliptic equations with regular solutions are initially analyzed in order to deeply investigate the performance of such methods on rectangular and irregular domains. We study the deep neural network solutions for different number of training and collocation points as well as different neural network architectures. The accuracy is also compared with standard schemes based on finite differences. In the case of singular forces, the analytical solution is continuous but the normal derivative on the interface has a discontinuity. This discontinuity is incorporated into the equations as a source term with a delta function which is approximated using a Peskin's approach. The performance of the proposed method is analyzed for different interface shapes and domains. Results demonstrate that the immersed boundary neural network can approximate accurately the analytical solution for elliptic problems with and without singularity.

    Citation: Reymundo Itzá Balam, Francisco Hernandez-Lopez, Joel Trejo-Sánchez, Miguel Uh Zapata. An immersed boundary neural network for solving elliptic equations with singular forces on arbitrary domains[J]. Mathematical Biosciences and Engineering, 2021, 18(1): 22-56. doi: 10.3934/mbe.2021002

    Related Papers:

  • In this paper, we present a deep learning framework for solving two-dimensional elliptic equations with singular forces on arbitrary domains. This work follows the ideas of the physical-inform neural networks to approximate the solutions and the immersed boundary method to deal with the singularity on an interface. Numerical simulations of elliptic equations with regular solutions are initially analyzed in order to deeply investigate the performance of such methods on rectangular and irregular domains. We study the deep neural network solutions for different number of training and collocation points as well as different neural network architectures. The accuracy is also compared with standard schemes based on finite differences. In the case of singular forces, the analytical solution is continuous but the normal derivative on the interface has a discontinuity. This discontinuity is incorporated into the equations as a source term with a delta function which is approximated using a Peskin's approach. The performance of the proposed method is analyzed for different interface shapes and domains. Results demonstrate that the immersed boundary neural network can approximate accurately the analytical solution for elliptic problems with and without singularity.


    加载中


    [1] I. J. Goodfellow, Y. Bengio, A. Courville, Deep Learning, MIT Press, Cambridge, 2016.
    [2] G. Shrivastava, S. Karmakar, M. K. Kowar, P. Guhathakurta, Application of artificial neural networks in weather forecasting: a comprehensive literature review, Int. J. Comput. Appl., 51 (2012), 17-29.
    [3] Q. Zhong, Y. Liu, X. Ao, B. Hu, J. Feng, J. Tang, et al., Financial Defaulter Detection on Online Credit Payment via Multi-view Attributed Heterogeneous Information Network, Proc. Web Conf. 2020, (2020), 785-795.
    [4] M. Lam, Neural network techniques for financial performance prediction: integrating fundamental and technical analysis, Decis. Support Syst., 37 (2004), 567-581. doi: 10.1016/S0167-9236(03)00088-5
    [5] G. Youyang, COVID-19 Projections Using Machine Learning, 2020. Available from: https: //covid19-projections.com/about.
    [6] J. Han, A. Jentzen, E. Weinan, Solving high-dimensional partial differential equations using deep learning, Proc. Natl. Acad. Sci., 115 (2018), 8505-8510. doi: 10.1073/pnas.1718942115
    [7] J. Sirignano, K. Spiliopoulos, DGM: A deep learning algorithm for solving partial differential equations, J. Comput. Phys., 375 (2018), 1339-1364. doi: 10.1016/j.jcp.2018.08.029
    [8] K. Xu, E. Darve, The neural network approach to inverse problems in differential equations, preprint, arXiv: 1901.07758.
    [9] M. Raissi, P. Perdikaris, G. E. Karniadakis, Physics-informed neural networks: A deep learning framework for solving forward and inverse problems involving nonlinear partial differential equations, J. Comput. Phys., 378 (2019), 686-707. doi: 10.1016/j.jcp.2018.10.045
    [10] C. Michoski, M. Milosavljevic, T. Oliver, D. Hatch, Solving irregular and data-enriched differential equations using deep neural networks, preprint, arXiv: 1905.04351.
    [11] K. Gurney, An introduction to neural networks, CRC press, Boca Raton, 1997.
    [12] A.G. Baydin, B.A. Pearlmutter, A.A. Radul, J.M. Siskind, Automatic differentiation in machine learning: a survey, preprint, arXiv: 1502.05767.
    [13] S. Marsland, Machine learning: an algorithmic perspective, CRC press, Boca Raton, 2015.
    [14] S. Pattanayak, Pro deep learning with tensorflow: A mathematical approach to advanced artificial intelligence in python, Apress, New York, 2017.
    [15] G. Zaccone, R. Karim, Deep learning with tensorFlow: Explore neural networks and build intelligent systems with python, Packt Publishing Ltd, Birmingham, 2018.
    [16] M. A. Nielsen, Neural networks and deep learning, Determination press, San Francisco, 2015.
    [17] Z. Mao, A. D. Jagtap, G. E. Karniadakis, Physics-informed neural networks for high-speed flows, Comput. Methods Appl. Mech. Eng., 360 (2020), 112789.
    [18] L. Sun, H. Gao, S. Pan, J. X. Wang, Surrogate modeling for fluid flows based on physics-constrained deep learning without simulation data. Comput. Methods Appl. Mech. Eng., 361 (2020), 112732.
    [19] M. Raissi, A. Yazdani, G. E. Karniadakis, Hidden fluid mechanics: Learning velocity and pressure fields from flow visualizations, Sci., 367 (2020), 1026-1030. doi: 10.1126/science.aaw4741
    [20] J. Berg, K. Nyström, A unified deep artificial neural network approach to partial differential equations in complex geometries, Neurocomputing, 317 (2018), 28-41.
    [21] E. Weinan, B. Yu, The deep Ritz method: a deep learning-based numerical algorithm for solving variational problems, Commun. Math. Stat., 6 (2018), 1-12. doi: 10.1007/s40304-018-0127-z
    [22] C. Anitescu, E. Atroshchenko, N. Alajlan, T. Rabczuk, Artificial neural network methods for the solution of second order boundary value problems, Comput. Mater. Continua, 59 (2019), 345-359. doi: 10.32604/cmc.2019.06641
    [23] L. Lu, X. Meng, Z. Mao, G. E. Karniadakis, DeepXDE: A deep learning library for solving differential equations, preprint, arXiv: 1907.04502.
    [24] A. Koryagin, R. Khudorozkov, S. Tsimfer, PyDEns: A python framework for solving differential equations with neural networks, preprint, arXiv: 1909.11544.
    [25] J. Han, M. Nica, A.R. Stinchcombe, A derivative-free method for solving elliptic partial differential equations with deep neural networks, preprint, arXiv: 2001.06145.
    [26] Y. Zang, G. Bao, X. Ye, H. Zhou, Weak adversarial networks for high-dimensional partial differential equations, J. Comput. Phys., (2020), 109409.
    [27] C. S. Peskin, Flow patterns around heart valves: a numerical method, J. Comput. Phys., 10 (1972), 252-271. doi: 10.1016/0021-9991(72)90065-4
    [28] C. S. Peskin, Numerical analysis of blood flow in the heart, J. Comput. Phys., 25 (1977), 220-252. doi: 10.1016/0021-9991(77)90100-0
    [29] Y. Kim, C. S. Peskin, Penalty immersed boundary method for an elastic boundary with mass, Physics of Fluids, 19(5) (2007), 053103.
    [30] Y. Mori, C. S. Peskin, Implicit second-order immersed boundary methods with boundary mass, Comput. Methods Appl. Mech. Eng., 197 (2008), 2049-2067. doi: 10.1016/j.cma.2007.05.028
    [31] Y. Kim, C. S. Peskin, 2-D parachute simulation by the immersed boundary method, SIAM J. Sci. Comput., 28 (2006), 2294-2312. doi: 10.1137/S1064827501389060
    [32] S. Lim, A. Ferent, X. S. Wang, C. S. Peskin, Dynamics of a closed rod with twist and bend in fluid, SIAM J. Sci. Comput., 31 (2008), 273-302. doi: 10.1137/070699780
    [33] P. J. Atzberger, C. S. Peskin, A Brownian dynamics model of kinesin in three dimensions incorporating the force-extension profile of the coiled-coil cargo tether, Bull. Math. Biol., 68 (2006), 131.
    [34] P. J. Atzberger, P. R. Kramer, C. S. Peskin, Stochastic immersed boundary method incorporating thermal fluctuations, Proc. Appl. Math. Mech., 7 (2007), 1121401-1121402. doi: 10.1002/pamm.200700197
    [35] T. G. Fai, B. E. Griffith, Y. Mori, C. S. Peskin, Immersed boundary method for variable viscosity and variable density problems using fast constant-coefficient linear solvers I: Numerical method and results, SIAM J. Sci. Comput., 35 (2013), B1132-B1161.
    [36] C. S. Peskin, The immersed boundary method, Acta Numerica, 11 (2002), 479-517.
    [37] R. Mittal, G. Iaccarino, Immersed boundary methods, Annu. Rev. Fluid Mech., 37 (2005), 239-261.
    [38] R. J. Leveque, Z. Li, The immersed interface method for elliptic equations with discontinuous coefficients and singular sources, SIAM J. Numer. Anal., 31 (1994), 1019-1044. doi: 10.1137/0731054
    [39] D. A. Fournier, H. J. Skaug, J. Ancheta, J. Ianelli, A. Magnusson, M. N. Maunder, et al., Ad model builder: using automatic differentiation for statistical inference of highly parameterized complex nonlinear models, Optim. Methods Software, 27 (2012), 233-249.
    [40] M. Abadi, A. Agarwal, P. Barham, E. Brevdo, Z. Chen, C. Citro, et al, Tensorflow: Large-scale machine learning on heterogeneous distributed systems, preprint, arXiv: 1603.04467.
    [41] R. Byrd, P. Lu, J. Nocedal, C. Zhu, A limited memory algorithm for bound constrained optimization. SIAM J. Sci. Comput., 16 (1995), 1190-1208.
    [42] W. Qi, M. Yue, Z. Kun, T. Yingjie, A Comprehensive Survey of Loss Functions in Machine Learning, Ann. Data Sci., 1 (2020), 1-26.
    [43] F. Zhengqing, L. Goulin, G. Lanlan, Sequential quadratic programming method for nonlinear least squares estimation and its application, Math. Probl. Eng., 2019(2019).
    [44] J. Alberty, C. Carstensen, S. A. Funken, Remarks around 50 lines of Matlab: short finite element implementation. Numer. algorithms, 20 (1999), 117-137.
    [45] F. Civan, C. M. Sliepcevich, Solution of the Poisson equation by differential quadrature. Int. J. Numer. Methods Eng., 19 (1983), 711-724.
    [46] J. Hua, J. Lou, Numerical simulation of bubble rising in viscous liquid. J. Comput. Phys., 222 (2007), 769-795.
    [47] M. Uh, S. Xu, The immersed interface method for simulating two-fluid flows. Numer. Math. Theory, Methods Appl., 7 (2014), 447-472.
  • Reader Comments
  • © 2021 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(5071) PDF downloads(372) Cited by(5)

Article outline

Figures and Tables

Figures(22)  /  Tables(18)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog