Mutual Coupling Between Broadside Printed Dipoles Embedded in Stratified Anisotropic Dielectrics - PowerPoint PPT Presentation

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Mutual Coupling Between Broadside Printed Dipoles Embedded in Stratified Anisotropic Dielectrics

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Microstrip antenna arrays [4]. Frequency Selective Structures (FSS) [5] ... (direction of the optical axis) has the largest impact on the mutual coupling. – PowerPoint PPT presentation

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Title: Mutual Coupling Between Broadside Printed Dipoles Embedded in Stratified Anisotropic Dielectrics


1
Mutual Coupling Between Broadside Printed Dipoles
Embedded in Stratified Anisotropic Dielectrics
  • Benjamin D. Braaten
  • Robert M. Nelson
  • David A. Rogers

North Dakota State University
2
Topics
  • Problem Definition
  • Spectral domain immittance functions
  • Results
  • Discussion
  • Conclusion

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3
Problem Definition
  • Consider

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4
Interests
  • The previous problem is of interest in many
    fields.
  • Microstrip antenna arrays 4.
  • Frequency Selective Structures (FSS) 5
  • Radio Frequency Identification (RFID) 6
  • IC based antennas
  • Radar

4 David M. Pozar and Daniel H. Schaubert,
Microstrip Antennas The analysis and Design of
Microstrip Antennas and Arrays, IEEE Press,
Piscataway, NJ, 1995. 5 A.L.P.S. Campos an A.G.
d'Assuncao, Scattering parameters of a
frequency selective surface between anisotropic
dielectric layers for incident co-polarized plane
waves, IEEE Antennas and Propagation Society
International Symposium, 2001, Vol. 4, July 8-13,
2001, p. 382-385. 6 K. Finkenzeller, RFID
HandbookFundamentals and Applications in
Contactless Smart Cards and Identification, John
Wiley and Sons, West Sussex, England, 2003.
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5
The new spectral domain immittance functions
Start with the following Hertz vector potentials
Electric Hertz potential
and
Magnetic Hertz potential
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6
The new spectral domain immittance functions
  • Next, only the y-direction of the Hertz vector
    potential is needed.

and
  • This is because the optical axis is in the
    y-direction
  • and
  • this component satisfies the higher order TE and
    TM tangential boundary conditions.

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7
The new spectral domain immittance functions
Now define the following expression for the
magnetic and electric field
where the Hertzian vector potentials are
solutions to the following wave equations
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8
The new spectral domain immittance functions
and
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9
The new spectral domain immittance functions
To simplify evaluating the previous expressions,
we define the following Fourier transform
This results in the following relations
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10
The new spectral domain immittance functions
This results in the following simplified
expressions
where
and
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11
The new spectral domain immittance functions
Similarly for
and
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12
The new spectral domain immittance functions
Double layer problem
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13
The new spectral domain immittance functions
Double (and Triple) layer problems
After extensive factoring and manipulation, the
following spectral domain immittance functions
are derived
and
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14
The new spectral domain immittance functions
An example of a spectral domain immittance
function
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15
Solving the new expressions
  • The spectral domain moment method was used to
    solve for the unknown current.
  • PWS functions were used as expansion and basis
    functions.
  • A delta source was used to drive the problem.

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16
Dipole Results
Consider
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Dipole Results
A single anisotropic substrate (d1 1.58 mm)
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Dipole Results
A single anisotropic cover (d1 1.58 mm d2
1.58 mm)
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Dipole Results
Separated by a single anisotropic layer (d1
1.58 mm d2 1.58 mm)
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20
Conclusion
  • New multi-conductor spectral domain immittance
    functions have been summarized.
  • Broadside printed dipoles on a single anisotropic
    substrate have been investigated.
  • It is shown that the permittivity in the
    y-direction (direction of the optical axis) has
    the largest impact on the mutual coupling.
  • Broadside printed dipole with a single
    anisotropic superstrate have been investigated.
  • It is shown that the mutual coupling is
    unaffected by the permittivity in the y-direction
    (direction of the optical axis).

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21
Conclusion
  • Broadside printed dipoles separated by a single
    anisotropic superstrate have been investigated.
  • It is shown that both components of the
    permittivity affect the mutual coupling.

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22
Questions
  • Thank you for listening

North Dakota State University
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