national radio astronomy observatory charlottesville, virginia · 2015. 8. 19. · frequency...
TRANSCRIPT
![Page 1: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/1.jpg)
National Radio Astronomy Observatory
Charlottesville, Virginia
![Page 2: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/2.jpg)
Challenges for FASR:
• Extremely wide bandwidth (100 MHz to 30 GHz)
• Small size of the antenna (diameter of 3 – 5 meters)
• Dual polarization
• “Acceptable” G/T
• Minimize number of moving parts
![Page 3: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/3.jpg)
Gain of Reflector Antennas
ηλπ
2
4 AG =
EBXPSI ηηηηηηη =
EfficiencyError Surface Efficiency Blockage
Efficiencyization Crosspolar EfficiencyError Phase
EfficiencySpillover Efficiencyion Illumincat
E
B
X
P
S
I
======
ηηηηηη
![Page 4: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/4.jpg)
Gain of Reflector Antennas
1X =ηFeed pattern is symmetric (E and H plane patterns are identical )
1P =ηCommon phase center for both planes
Illumination and spillover losses are the principal causes of gain degradation.
There is usually a compromise between the illumination and spillover.
sidelobes. increasedin results Thisfeed. realizable afor low toois then 1, If SI ηη =
Clarricoats, P.J.B. and A.D. Olver, Corrugated Horns for Microwave Antennas, Peter Peregrinus, Ltd., London, UK, 1984, p. 100.
![Page 5: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/5.jpg)
Types of Feeds Presented Here
• Hybrid-Mode
• Dipole Above Ground Plane
• Frequency Independent Structures
![Page 6: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/6.jpg)
Hybrid-Mode Feeds
The Hybrid-Mode Feed offers a means to approach all of the objectives simultaneously.
)ˆ2sinˆ2)(cos(4
ˆ)( 21
2
yxo
xo iiKrJkrUYXiKrAJE φφ +⎟⎠⎞
⎜⎝⎛ −
−=
21
21
1rrat boundary theof admittance and reactance Normalized
⎥⎦
⎤⎢⎣
⎡+=−=⎥
⎦
⎤⎢⎣
⎡−=−=
=
o
o
zz
o
o
o
zo EH
jZZjY
HE
jZZ
jXεµ
µε φφφ
Clarricoats, P.J.B. and A.D. Olver, Corrugated Horns for Microwave Antennas, Peter Peregrinus, Ltd., London, UK, 1984, p. 7.
![Page 7: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/7.jpg)
Hybrid-Mode Feed – Corrugated Waveguide
integer. oddan is m
when 02
tan
0
=⎟⎟⎠
⎞⎜⎜⎝
⎛ ∆=
=
offmY
X
π
Co-polar bandwidth
Position of the phase center and generation of higher order modes Pattern symmetry and
cross-polar characteristics
Impedance matching to the waveguide and mode conversion level Clarricoats, P.J.B. and A.D. Olver, Corrugated Horns for
Microwave Antennas, Peter Peregrinus, Ltd., London, UK, 1984, pp. 99-100.
![Page 8: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/8.jpg)
Hybrid-Mode Feed – Corrugated Waveguide
Large flare angle horn (scalar feed) gives a relatively large bandwidth with nearly constant co-polar radiation characteristics.
Thomas, James, and Greene (1986):
Scalar feed having 2.1:1 bandwidth.
James (1984):
Compact profiled horn having 2.4:1 bandwidth (requires some focus adjustment)
Clarricoats, P.J.B. and A.D. Olver, Corrugated Horns for Microwave Antennas, Peter Peregrinus, Ltd., London, UK, 1984, p. 21.
![Page 9: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/9.jpg)
Hybrid-Mode Feed - Corrugated Waveguide
Absorber Lined Horn
band. over the dB 0.5 wasloss Ohmic launcher.)deby wavegui limitedfrequency (upper eddemonstrat was
GHz 12-4 fromOperation cone. theofpart upper thelined 0.56 and 1.4 reflector.horn ain
operation mode HE balancednearly edDemonstrat
(1986) Ostertag and Cheng, Knop,
11
=′′=′ εε
Knop, C.M., Y.B. Cheng, and E.L. Ostertag, “On the Fields in a Conical Horn Having an Arbitrary Wall Impedance,” IEEE Trans. Ant. and Propag., Vol. 34, Sept. 1986, pp. 1092-1098.
![Page 10: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/10.jpg)
Hybrid-Mode Feed – Surface-Wave Antenna
Dielectric Waveguide (rod)
( ) ( )( )
( )nYX
nn
Yn
∆−=−
∆+∆
=∆
=
∆>>
2)(
Thus,
2121;
21X
thenunity, from n, amount, small aonly by differsindex refractive theif and 1kr If 1
This condition is frequency independent if the dielectric is free from dispersion over the operational bandwidth.
Unless delta-n is sufficiently large it is impossible to effectively launch the dominant mode of the dielectric waveguide – loose energy in the launcher.
Corrugated waveguide: Lower cross-pol over 2.5:1 bandwidth.
Dielectric waveguide: higher cross-pol over a much wider band.BW= 4:1
Clarricoats, P.J.B. and A.D. Olver, Corrugated Horns for Microwave Antennas, Peter Peregrinus, Ltd., London, UK, 1984, p. 9.
Johnson, R. C. Antenna Engineering Handbook,, 3rd
ed., McGraw-Hill, New York, 1993, p. (12-21).
![Page 11: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/11.jpg)
Hybrid-Mode Feeds
Disadvantages for FASR:
• Big and bulky (corrugated)
• High machining cost (corrugated)
• Bandwidth not large enough
• Polarizer bandwidth about 2.5:1
• Loss associated with dielectric material
![Page 12: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/12.jpg)
Dipole Above a Ground PlaneConventional half-wave dipole
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (4-12).
![Page 13: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/13.jpg)
Dipole Above a Ground PlaneConventional half-wave dipole
BW=1.09:1Stutzman, W. and G. Thiele, Antenna Theory and Design, Wiley, New York, 1981, pp. 199-200.
![Page 14: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/14.jpg)
Dipole Above a Ground PlaneFat Dipole
BW= 1.18:1Stutzman, W. and G. Thiele, Antenna Theory and Design, Wiley, New York, 1981, p. 203.
![Page 15: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/15.jpg)
Dipole Above a Ground Plane
Sleeve Dipole
BW= 1.67:1Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (4-21).
![Page 16: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/16.jpg)
Dipole Above a Ground Plane
Folded, Fat Dipole
BW= 1.53:1
![Page 17: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/17.jpg)
Dipole Above a Ground Plane
Short Backfire Antenna
Ehrenspeck, H.W. “The Short Backfire Antenna,” Proc. of the IEEE, v. 53, Aug. 1965, pp.1138-1140.
BW= 1.35:1Srikanth, S. and G. Behrens, “A New Short Backfore Antenna as a Prome Focus Feed for the GBT”, GBT Memo. #187, May 13, 1998.
![Page 18: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/18.jpg)
Dipole Above a Ground Plane
Disadvantages for FASR:
• Bulky
• Narrow bandwidth
• Large spillover
![Page 19: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/19.jpg)
Frequency Independent Antennas
Provided the antenna is made of practically perfect conductors and dielectrics, the impedance, polarization, pattern, etc. are invariant to a change in scalethat is in proportion to the change in wavelength.
If the shape of the antenna is determined entirely by angles (invariant to scale), the performance would have to be independent of frequency.
Truncation of the shape from that of infinite extent should also give goodperformance (current should decrease with distance from the terminals).
Ω===⇒ 5.1882
Designary Complement-Self ηMETALAIR ZZ
Operational bandwidth:
• lowest frequency limited by the maximum dimension
• upper frequency limited by the input terminal region
• bandwidths can be 10:1 or greater.
![Page 20: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/20.jpg)
Frequency Independent Antennas
Log Periodic
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-30).
![Page 21: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/21.jpg)
Frequency Independent Antennas
Spirals
Stutzman, W. and G. Thiele, Antenna Theory and Design, Wiley, New York, 1981, p. 284.
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-25).
![Page 22: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/22.jpg)
Frequency Independent Antennas
Absorber Loaded Cavity
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-18).
![Page 23: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/23.jpg)
Frequency Independent Antennas
Conical Log-Spiral
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-33).
![Page 24: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/24.jpg)
Frequency Independent Antennas
Sinuous
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-56).
![Page 25: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/25.jpg)
Frequency Independent Antennas
Sinuous
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-60).
![Page 26: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/26.jpg)
Frequency Independent Antennas
Sinuous
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-61).
![Page 27: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/27.jpg)
Frequency Independent Antennas
Sinuous Antenna on a Cone
Johnson, R. C. Antenna Engineering Handbook,, 3rd ed., McGraw-Hill, New York, 1993, p. (14-61).
![Page 28: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/28.jpg)
Frequency Independent Antennas
Disadvantages for FASR:
• Integration of feed, LNA and balun
• Could be lossy (affect G/T)
• Dual-polarization
• Gain varies with frequency for fixed position conical
![Page 29: National Radio Astronomy Observatory Charlottesville, Virginia · 2015. 8. 19. · Frequency Independent Antennas Provided the antenna is made of practically perfect conductors and](https://reader035.vdocuments.mx/reader035/viewer/2022070220/61338b41dfd10f4dd73b2820/html5/thumbnails/29.jpg)
Conclusions
For FASR:
• Frequency independent antennas are the only practical option to cover FASR frequency range.
• Use a cavity backed structure for wide instantaneous bandwidth.
• Accept gain reduction associated with fixed position cone.
• Consider sinuous version of frequency independent structures.
• Integration of feed terminals with LNAs and balun.
• Prototyping highly recommended!