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Structure-preserving neural networks for the regularized entropy-based closure of the Boltzmann moment system

arXiv 2404.14312 ↗First posted 22 Apr 2024math.NA cs.LG cs.NAcited by 0

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Abstract (arXiv)

The main challenge of large-scale numerical simulation of radiation transport is the high memory and computation time requirements of discretization methods for kinetic equations. In this work, we derive and investigate a neural network-based approximation to the entropy closure method to accurately compute the solution of the multi-dimensional moment system with a low memory footprint and competitive computational time. We extend methods developed for the standard entropy-based closure to the context of regularized entropy-based closures. The main idea is to interpret structure-preserving neural network approximations of the regularized entropy closure as a two-stage approximation to the original entropy closure. We conduct a numerical analysis of this approximation and investigate optimal parameter choices. Our numerical experiments demonstrate that the method has a much lower memory footprint than traditional methods with competitive computation times and simulation accuracy.

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References · 8

  1. 2021Convex optimizationcited by 2,515
  2. 2016Input Convex Neural Networkscited by 414
  3. 2021Machine learning moment closure models for the radiative transfer equation I: directly learning a gradient based closurecited by 9
  4. 2020Integrating Machine Learning with Physics-Based Modelingcited by 8
  5. 2020Learning Thermodynamically Stable and Galilean Invariant Partial Differential Equations for Non-equilibrium Flowscited by 7
  6. 2021Machine learning moment closure models for the radiative transfer equation II: enforcing global hyperbolicity in gradient based closurescited by 7
  7. 2021Machine learning moment closure models for the radiative transfer equation III: enforcing hyperbolicity and physical characteristic speedscited by 6
  8. 2024Hyperbolic Machine Learning Moment Closures for the BGK Equationscited by 4

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