Title: Mutual Coupling Between Broadside Printed Dipoles Embedded in Stratified Anisotropic Dielectrics
1Mutual Coupling Between Broadside Printed Dipoles
Embedded in Stratified Anisotropic Dielectrics
- Benjamin D. Braaten
- Robert M. Nelson
- David A. Rogers
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2Topics
- Problem Definition
- Spectral domain immittance functions
- Results
- Discussion
- Conclusion
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3Problem Definition
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4Interests
- 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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5The new spectral domain immittance functions
Start with the following Hertz vector potentials
Electric Hertz potential
and
Magnetic Hertz potential
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6The 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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7The 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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8The new spectral domain immittance functions
and
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9The 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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10The new spectral domain immittance functions
This results in the following simplified
expressions
where
and
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11The new spectral domain immittance functions
Similarly for
and
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12The new spectral domain immittance functions
Double layer problem
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13The 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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14The new spectral domain immittance functions
An example of a spectral domain immittance
function
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15Solving 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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16Dipole Results
Consider
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17Dipole Results
A single anisotropic substrate (d1 1.58 mm)
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18Dipole Results
A single anisotropic cover (d1 1.58 mm d2
1.58 mm)
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19Dipole Results
Separated by a single anisotropic layer (d1
1.58 mm d2 1.58 mm)
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20Conclusion
- 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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21Conclusion
- 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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22Questions
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