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From Surface Equivalence Principle to Modular Domain Decomposition Florian Muth* Hermann Schneider* * PhD students CST COMPUTER SIMULATION TECHNOLOGY | www.cst.com Motivation I Challenge: complex/large models Multiple scales


  1. From Surface Equivalence Principle to Modular Domain Decomposition Florian Muth* Hermann Schneider* * PhD students CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  2. Motivation I  Challenge: complex/large models  Multiple scales  Different electromagnetic properties  Full set of M AXWELL ’s equations E.g.: 1.5 GHz GPS antenna ≈ 𝟕𝟔𝟏𝝁 ⇒ 𝟐𝟏 𝟐𝟑 mesh cells (10 lines per wavelength) CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 2

  3. Motivation II  Approach: domain decomposition  Tightly coupled subdomains, full system solve necessary  global iterative solver  Couple existing solvers → modular, black box framework  arbitrary solvers  Coupling via surface currents Global I terative Solver Asymptotic  Integration in commercial software BEM FEM CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 3

  4. Outline  Motivation  Surface Equivalence Principle  Iterative Domain Decomposition  First Results  Conclusion and Outlook CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 4

  5. Surface Equivalence Principle I  Sources and materials enclosed by surface 𝑇 can be replaced by equivalent surface currents 𝐾 𝑡 and 𝑁 𝑡 : Full model Equivalent model for outer domain CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 5

  6. Surface Equivalence Principle I  Sources and materials enclosed by surface 𝑇 can be replaced by equivalent surface currents 𝐾 𝑡 and 𝑁 𝑡 : Full model Equivalent model for inner domain CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 6

  7. Surface Equivalence Principle I  Sources and materials enclosed by surface 𝑇 can be replaced by equivalent surface currents 𝐾 𝑡 and 𝑁 𝑡 : full outer inner model equivalent equivalent CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 7

  8. Surface Equivalence Principle II  Will be utilized for black box DD approach  Coupling of subdomains via surface currents  Subdomains need to provide surface currents only  Resulting in an iterative DD method CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 8

  9. Outline  Motivation  Surface Equivalence Principle  Iterative Domain Decomposition  First Results  Conclusion and Outlook CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 9

  10. Iterative Domain Decomposition Typical Coupled System CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 10

  11. Iterative Domain Decomposition Coupled System + Surface Equivalence Principle source monitor monitor source CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 11

  12. Iterative Domain Decomposition Equivalence Principle Motivated Approach source monitor solve solve GMRES Resulting system solved for surface quantities 𝑦 1 and 𝑦 2 , e.g. by fixpoint iteration or accelerated by GMRES CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 12

  13. Outline  Motivation  Surface Equivalence Principle  Iterative Domain Decomposition  First Results  Conclusion and Outlook CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 13

  14. First Results  Area of application of this project  Small number of user-defined, coupled subdomains  Priority not on scalability, but flexibility  E.g. antenna placement  Model: 1x2 patch antenna array  Academic example  For investigation purposes ≈ 2𝜇 CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 14

  15. First Results Setup  FEM-FEM coupling  Non-overlapping subdomains Air buffer Coupling (wireframe) interface ABC  A bsorbing B oundary C ondition  Broadside radiation  Non-conforming mesh at interface Domain 2 Domain 1 CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 15

  16. First Results E-Field on 1D-Curve X Interface CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 16

  17. First Results Far Field Full model: DD approach: CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 17

  18. First Results GMRES Residual Convergence Norm based on physical quantities Independent of basis  functions Support of different types of  electromagnetic solvers CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 18

  19. First Results S-Parameter Convergence Residual in surface quantities ↔ errors  in quantities of interest? Abs. error < 10 −3 sufficient for typical  engineering applications  Rel. residual < 4 ∙ 10 −2 already enough!? CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 19

  20. First Results Overlap Parameter Study I  DD approach features high flexibility in defining coupling Overlap 𝑒 surfaces  Overlaps can be easily introduced Domain 2 Domain 1 CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 20

  21. 𝑒 First Results Overlap Parameter Study II 𝑒  Major improvement in convergence  No significant performance drawback!  One mesh cell layer overlap: 𝑒 = 4 ∙ 10 −2 𝜇 CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 21

  22. Outline  Motivation  Surface Equivalence Principle  Iterative Domain Decomposition  First Results  Conclusion and Outlook CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 22

  23. Conclusion  DD approach suitable for large and complex setups  Modular, black box framework  arbitrary solvers  Equivalence principle motivated coupling via surface currents  High flexibility in defining coupling surfaces  Promising first results, accelerated convergence due to introduced overlap CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 23

  24. Outlook  Proper definition of the norm  Residual ↔ errors in the quantities of interest  Dependency of convergence on coupling strength of subdomains  Treatment of cross-points ? CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 24

  25. Thank You For Your Attention! Any Questions? CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com 25

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