From Surface Equivalence Principle to Modular Domain Decomposition - - PowerPoint PPT Presentation

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From Surface Equivalence Principle to Modular Domain Decomposition - - PowerPoint PPT Presentation

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


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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

From Surface Equivalence Principle to Modular Domain Decomposition

Florian Muth* Hermann Schneider*

* PhD students

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • Challenge: complex/large models
  • Multiple scales
  • Different electromagnetic properties
  • Full set of MAXWELL’s equations

Motivation I

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≈ 𝟕𝟔𝟏𝝁 ⇒ 𝟐𝟏𝟐𝟑 mesh cells (10 lines per wavelength) E.g.: 1.5 GHz GPS antenna

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • 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
  • Integration in commercial software

Motivation II

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FEM BEM Asymptotic Global Iterative Solver

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • Motivation
  • Surface Equivalence Principle
  • Iterative Domain Decomposition
  • First Results
  • Conclusion and Outlook

Outline

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Surface Equivalence Principle I

Full model

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  • Sources and materials enclosed by surface 𝑇 can be

replaced by equivalent surface currents 𝐾

𝑡 and 𝑁𝑡: Equivalent model for outer domain

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Surface Equivalence Principle I

Full model

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  • Sources and materials enclosed by surface 𝑇 can be

replaced by equivalent surface currents 𝐾

𝑡 and 𝑁𝑡: Equivalent model for inner domain

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Surface Equivalence Principle I

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  • Sources and materials enclosed by surface 𝑇 can be

replaced by equivalent surface currents 𝐾

𝑡 and 𝑁𝑡: full model

  • uter

equivalent inner equivalent

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Surface Equivalence Principle II

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  • 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
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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • Motivation
  • Surface Equivalence Principle
  • Iterative Domain Decomposition
  • First Results
  • Conclusion and Outlook

Outline

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Iterative Domain Decomposition

Typical Coupled System

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Iterative Domain Decomposition

Coupled System + Surface Equivalence Principle

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source monitor source monitor

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Iterative Domain Decomposition

Equivalence Principle Motivated Approach

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solve GMRES source monitor solve Resulting system solved for surface quantities 𝑦 1 and 𝑦 2, e.g. by fixpoint iteration or accelerated by GMRES

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • Motivation
  • Surface Equivalence Principle
  • Iterative Domain Decomposition
  • First Results
  • Conclusion and Outlook

Outline

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • 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

First Results

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≈ 2𝜇

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

First Results

Setup

ABC Domain 2 Domain 1 Air buffer (wireframe) Coupling interface

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  • FEM-FEM coupling
  • Non-overlapping subdomains
  • Absorbing Boundary Condition
  • Broadside radiation
  • Non-conforming mesh at

interface

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

First Results

E-Field on 1D-Curve

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Interface X

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

First Results

Far Field

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Full model: DD approach:

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Norm based on physical quantities

  • Independent of basis

functions

  • Support of different types of

electromagnetic solvers

First Results

GMRES Residual Convergence

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • 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!?

First Results

S-Parameter Convergence

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Domain 2 Domain 1

Overlap 𝑒

  • DD approach features high

flexibility in defining coupling surfaces

  • Overlaps can be easily

introduced

First Results

Overlap Parameter Study I

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

First Results

Overlap Parameter Study II

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𝑒 𝑒

  • Major improvement in convergence
  • No significant performance

drawback!

  • One mesh cell layer overlap:

𝑒 = 4 ∙ 10−2𝜇

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • Motivation
  • Surface Equivalence Principle
  • Iterative Domain Decomposition
  • First Results
  • Conclusion and Outlook

Outline

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

  • 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

Conclusion

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

?

  • Proper definition of the norm
  • Residual ↔ errors in the quantities
  • f interest
  • Dependency of convergence on

coupling strength of subdomains

  • Treatment of cross-points

Outlook

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CST – COMPUTER SIMULATION TECHNOLOGY | www.cst.com

Thank You For Your Attention!

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Any Questions?

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