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Section (21/21)

  1. Importance of E-Polarized Wave Scattering from from Infinitely Thin and Finitely Width Strip Systems.
  2. What will be represented in E-Polarized Wave Scattering from from Infinitely Thin and Finitely Width Strip Systems?
  3. What is Analytical Regularization?
  4. Geometry and Formulation of Problem.
  5. Dirichlet Boundary Problem and Integral Representation of Scattered Field.
  6. Sommerfeld Radiation Conditions.
  7. Fundemental Solution for Helmholtz. Equation, Third Kind of Green Formula for Free Space.
  8. Analytic Continuity of homogeneous Helmholtz Equation: Sobolev Theory.
  9. Dirichlet Boundary Problem and Integral Representation of Scattered Field.
  10. Solution of Integral Equation.
  11. Local Singular Expantion.
  12. Integral Equation Identities due to Strip System.
  13. Reduction of Integral Equation to the Numerical System.
  14. Fourier-Chebyshev Expansions of Equation Terms.
  15. Reducing Integral Equation to the Infinite Linear Algebra System.
  16. Analytical Regularization Method for Infinite Linear Algebra System.
  17. Solution of Problem in Numerically.
  18. Finding Fourier-Chebshev for Matrix.
  19. Solution of Regularized Equation System.
  20. Solution of Regularized Equation System For Multi Strips.
  21. Scattered Field for Arbitrary Point in Space.


    

.: Gebze Institute of Technology Electronics Engineering Department

Mr.Deniz ELMASLI Master's Thesis

.: E-Polarized Wave Scattering from from Infinitely Thin and Finitely Width Strip Systems

Scattered Field for Arbitrary Point in Space

• We will use 3rd Kind of Green Formulation: System which has reduced to

-Arbitrary point in free space:

- Parametric tao point over obstacle:

- Current density over obstacle due to tao point:

- Green's Function:

Taking into account the Dirichlet Boudary Condition:

• RCS formula Radar Cross Section:

 

 

 

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