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Modelling and Simulation of Conical Spiral
Antennas
Motivation
• Most antennas are not able to maintain characteristics across
>2:1 bandwidth
• Consider antennas having true frequency independence
– Beam pattern (width, co-polarisation etc.)
– Impedance
• Higher gain elements
– More 'effective area' per element
– SKA station requires fewer elements to attain Ae/T
– Economic implications (all digital array?)
• We examine conical antennas as example high-gain, frequency-
independent antenna for SKA-low station studies
350 – 2250 MHz
Conical Log Spiral
Cone Angle
Wrap Angle
Strip Width δ
Ref: J. Dyson, “The Unidirectional Equiangular Spiral,” IRE Transactions on Antennas
and Propagation, vol. 7, pp. 329–334, Oct 1959.
Ref: J. Dyson, “The Unidirectional Equiangular Spiral,” IRE Transactions on Antennas and Propagation, vol. 7, pp. 329–334, Oct 1959.
Conical spiral: early work
Beam pattern, impedance and axial ratio
• Antenna characteristics with frequency
– Nearly constant beam pattern
– Low back-lobe at all but lowest frequency
– Relatively small, smooth impedance variation
– Good axial ratio maintained
Beam pattern, impedance and axial ratio
Conical spiral: early work
Mutual coupling
Ref: J. Dyson, “The coupling and mutual impedance between conical log-spiral antennas in simple arrays,” IRE International Convention Record, vol. 10, Mar
1962, pp. 165 – 182.
Conical spiral: early work
• Spiral features
– Low mutual coupling
– Polarisation purity
– Good isolation
Mutual coupling
Conical spiral: early work
Beamwidth
Ref: T. Milligan, Modern antenna design. Wiley-IEEE Press, 2005.
Conical spiral: early work
Beamwidth
• Parameters control beamwidth
• Able to obtain wider beamwidth for better sky coverage
Conical spiral: early work
Dual polarised design derivatives
• Conical Log Spiral (CLS) is a single-polarised antenna while
SKA-low requires a dual-polarised one.
• We are exploring designs for dual-polarised spirals
• One example
– Opposite hand spirals wounded on single former
– Counter-wound Co-axial Conical Log Spiral (C3LS)
antenna
CLS C3LS side view C3LS bottom view
Simulation of antennas
• Simulation of CLS antenna showed independent results which were
similar to previously constructed spiral antennas
– Motivating us to start our prototyping of the antenna.
• C3LS antenna simulation proving difficult
– Two overlapping layers could not be distinguished by simulation
software as two separate layers
– Larger separation and finer meshing gives indication that antenna
pattern might rotate through higher modes as a function of
frequency
• It was decided to
– Prototype C3LS antenna to study it in more detail
– Improve simulation
• Work in progress
Simulation results: CLS
Return Loss (at 188 Ω reference) Impedance
Return loss is less than -10 dB
over operating bandwidth
Impedance is constant through
operating bandwidth
Gain at zenith
>5.5dBi gain over the frequency range
Prototyping of the antennas
• 350-2250 MHz band CLS and C3LS
antenna constructed (1/5 SKA-low scale)
• 3:1 BALUN to feed C3LS
• No BALUN for CLS
• Construction errors
– Maintaining continuity of spiral arm over cone
– Elliptical cone due to material tension
– Non-rigid former for C3LS
• From measurements we found
– Small mechanical errors on top end of spiral
affected radiation and terminal characteristics
– Without BALUN, asymmetry is introduced in
radiation patternBALUN
CLS and C3LS antenna
Measurement of the Prototypes
Chamber measurements Outdoor measurements
• Chamber measurements can be
made only up to 1 GHz
• The floor was not absorbing
• Future measurements to include
foam floor panels
• Outdoor measurements influenced
by reflections and (some) RFI
• Future measurements to include 3 m
high masts and foam floor panels
Radiation Pattern
Simulated First measurements
Radiation pattern of the CLS antenna at 350, 650 and 1000 MHz
Note: Measurements made in chamber
Measured C3LS results
Very recent, still developing antenna & measurement process
Inner spiral Outer spiral
Radiation pattern of the C3LS antenna at 476 MHz
Note: Measurements made in chamber
Continuing work
• Make mechanically robust and accurate antennas for testing
• Build mechanically robust antennas
• Build prototype array for testing and measurement
• Explore other spiral derivatives
– Pyramidal Sinuous
– Modulated Arm Width (MAW)
• Explore other high-gain, frequency-independent antennas for
SKA system design
• Collaborate in lower-gain element development and testing

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Conical spiral antennas

  • 1. Modelling and Simulation of Conical Spiral Antennas
  • 2. Motivation • Most antennas are not able to maintain characteristics across >2:1 bandwidth • Consider antennas having true frequency independence – Beam pattern (width, co-polarisation etc.) – Impedance • Higher gain elements – More 'effective area' per element – SKA station requires fewer elements to attain Ae/T – Economic implications (all digital array?) • We examine conical antennas as example high-gain, frequency- independent antenna for SKA-low station studies 350 – 2250 MHz
  • 3. Conical Log Spiral Cone Angle Wrap Angle Strip Width δ Ref: J. Dyson, “The Unidirectional Equiangular Spiral,” IRE Transactions on Antennas and Propagation, vol. 7, pp. 329–334, Oct 1959.
  • 4. Ref: J. Dyson, “The Unidirectional Equiangular Spiral,” IRE Transactions on Antennas and Propagation, vol. 7, pp. 329–334, Oct 1959. Conical spiral: early work Beam pattern, impedance and axial ratio
  • 5. • Antenna characteristics with frequency – Nearly constant beam pattern – Low back-lobe at all but lowest frequency – Relatively small, smooth impedance variation – Good axial ratio maintained Beam pattern, impedance and axial ratio Conical spiral: early work
  • 6. Mutual coupling Ref: J. Dyson, “The coupling and mutual impedance between conical log-spiral antennas in simple arrays,” IRE International Convention Record, vol. 10, Mar 1962, pp. 165 – 182. Conical spiral: early work
  • 7. • Spiral features – Low mutual coupling – Polarisation purity – Good isolation Mutual coupling Conical spiral: early work
  • 8. Beamwidth Ref: T. Milligan, Modern antenna design. Wiley-IEEE Press, 2005. Conical spiral: early work
  • 9. Beamwidth • Parameters control beamwidth • Able to obtain wider beamwidth for better sky coverage Conical spiral: early work
  • 10. Dual polarised design derivatives • Conical Log Spiral (CLS) is a single-polarised antenna while SKA-low requires a dual-polarised one. • We are exploring designs for dual-polarised spirals • One example – Opposite hand spirals wounded on single former – Counter-wound Co-axial Conical Log Spiral (C3LS) antenna CLS C3LS side view C3LS bottom view
  • 11. Simulation of antennas • Simulation of CLS antenna showed independent results which were similar to previously constructed spiral antennas – Motivating us to start our prototyping of the antenna. • C3LS antenna simulation proving difficult – Two overlapping layers could not be distinguished by simulation software as two separate layers – Larger separation and finer meshing gives indication that antenna pattern might rotate through higher modes as a function of frequency • It was decided to – Prototype C3LS antenna to study it in more detail – Improve simulation • Work in progress
  • 12. Simulation results: CLS Return Loss (at 188 Ω reference) Impedance Return loss is less than -10 dB over operating bandwidth Impedance is constant through operating bandwidth
  • 13. Gain at zenith >5.5dBi gain over the frequency range
  • 14. Prototyping of the antennas • 350-2250 MHz band CLS and C3LS antenna constructed (1/5 SKA-low scale) • 3:1 BALUN to feed C3LS • No BALUN for CLS • Construction errors – Maintaining continuity of spiral arm over cone – Elliptical cone due to material tension – Non-rigid former for C3LS • From measurements we found – Small mechanical errors on top end of spiral affected radiation and terminal characteristics – Without BALUN, asymmetry is introduced in radiation patternBALUN CLS and C3LS antenna
  • 15. Measurement of the Prototypes Chamber measurements Outdoor measurements • Chamber measurements can be made only up to 1 GHz • The floor was not absorbing • Future measurements to include foam floor panels • Outdoor measurements influenced by reflections and (some) RFI • Future measurements to include 3 m high masts and foam floor panels
  • 16. Radiation Pattern Simulated First measurements Radiation pattern of the CLS antenna at 350, 650 and 1000 MHz Note: Measurements made in chamber
  • 17. Measured C3LS results Very recent, still developing antenna & measurement process Inner spiral Outer spiral Radiation pattern of the C3LS antenna at 476 MHz Note: Measurements made in chamber
  • 18. Continuing work • Make mechanically robust and accurate antennas for testing • Build mechanically robust antennas • Build prototype array for testing and measurement • Explore other spiral derivatives – Pyramidal Sinuous – Modulated Arm Width (MAW) • Explore other high-gain, frequency-independent antennas for SKA system design • Collaborate in lower-gain element development and testing