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A New Numerical Design Method for Log-periodic Eleven Feed – The Partial Array Method. Jian Yang, Associate Professor Chalmers University of Technology Sweden. Outline. Introduction New Method: the partial array method Optimization Procedure Result of Optimization
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A New Numerical Design Method for Log-periodic Eleven Feed – The Partial Array Method JianYang, Associate Professor Chalmers University of Technology Sweden
Outline • Introduction • New Method: the partial array method • Optimization Procedure • Result of Optimization • Simulations and Measurements • Conclusions
Introduction - The Eleven Feed dipoles • Two unique characteristics over decade bandwidth • Constant beam width; • Fixed phase center location Phase center Ground plane
Introduction - The Eleven Feed • Simple geometry, small volume • Can be located in cryostat; • -10 dB reflection coefficient • Low cross pol. level
Introduction - challenge • Minimizing reflection coefficient is needed. • Challenge: Eleven feed is very large at highest frequency. • New method for global optimization scheme. Photo of the 2-13 GHz Eleven feed
New Method - Partial array method Scaled S-parameters due to scaled geometry • If the log-periodic array is infinite, we have the frequency scaling on s-parameters as: jdipole+n idipole+n jdipole idipole
D6 D5 D4 D3 D2 D1 2 1 2 1 2 1 2 1 1 2 1 1 2 2 Partial Array Method: Scaled S-parameters • example:
D6 D5 D4 D3 D2 D1 2 1 2 1 2 1 2 1 1 2 1 1 2 2 Partial Array Method: far separated mutual couplings very low
Partial Array Method • We can predict the S matrix for the whole array using S parameters in a small part of the array by • Scaling S parameters; • Ignoring mutual coupling between far separated elements.
Partial Array MethodImplementation Port definition port1 port2 S1(3)2(4) dipole4 dipole3
Partial Array Method 0 S= 0
Partial Array Method • Formula
Partial Array Methodfor details J. Yang and P.-S. Kildal, “Optimizing large log-periodic array by computing a small part of it”, appears in IEEE Trans. on Antennas Propag. Special Issue on Antennas for Next Generation Radio Telescopes, vol. 59, no. 3, March 2011.
Example Reflection coefficient of a 14-element log-periodic Eleven antenna array based on simulation of a 6-element array
Optimization ProcedureGenetic Algorithm • Six parameters are optimized: • scaling factor k, • dipole length L, • arm width w, • arm spacing da, • transmission line gap dc, • height above ground plane h.
Optimization • GA is used for minimizing S11 in a 6-element folded dipole array. • Elite crossover, Roulette wheel selection, crossover and mutation are used in GA. • population size: 50; • 5 generations; • Simulation tool is CST MS and the optimization is done by in-house Matlab program. • Computation Time • Each case 1 hours; • Fully optimized 1 week.
Result of Optimization • 14 pairs of folded dipoles with scaling factor 1 .24.
Result of Optimization • The port impedance is 200 Ohms.
Simulated and Measured ResultsReflection coefficient including centre puck
φ : 0-360o with step 1o. θ : 0-180o with step 1o. Frequency: 2–15 GHz with step 0.1 GHz. Spherical near field measurement Radiation Measurement at Technical University of Denmark
Efficiencies based on measured patterns in reflector with subtended semi-angle of 60 deg
Efficiencies based on Simulated patterns in reflector with subtended semi-angle of 60 deg
Radiation Patterns of BOR1 component Simulated Measured
Conclusions • The reflection coefficient is below -10 dB for 2 – 13 GHz. • The radiation pattern is constant for 2 – 13 GHz. • BOR1 efficiency is • > -0.5 dB for most part of 2 – 13 GHz, • > -1.5 for 2 –13 GHz. • Directivity is about 11 dBi. • Aperture efficiency is better than – 3 dB for 2 – 13 GHz.