Presentation is loading. Please wait.

Presentation is loading. Please wait.

Main beam representation in non-regular arrays

Similar presentations


Presentation on theme: "Main beam representation in non-regular arrays"— Presentation transcript:

1 Main beam representation in non-regular arrays
Christophe Craeye1, David Gonzalez-Ovejero1, Eloy de Lera Acedo2, Nima Razavi Ghods2, Paul Alexander2 1Université catholique de Louvain, ICTEAM Institute 2University of Cambridge, Cavendish Laboratory CALIM 2011 Workshop, Manchester, July 25-29, 2011 2d calibration Workshop, Algarve, Sep 26, 2011

2 2 parts Preliminary: Patterns of apertures – a review
Next: analysis of aperture arrays with mutual coupling Algarve meeting, 2011

3 a b r Algarve meeting, 2011

4 Fourier-Bessel series
Algarve meeting, 2011

5 Zernike series Algarve meeting, 2011
NB: the Zernike function is a special case of the Jacobi Function Algarve meeting, 2011

6 CALIM 2011 Zernike functions Picture from Wikipedia

7 Radiation pattern Hankel transform Algarve meeting, 2011

8 F.T. of Bessel Algarve meeting, 2011

9 FT of Zernike Algarve meeting, 2011

10 Sparse polynomial Algarve meeting, 2011

11 Context: SKA AA-lo CALIM 2011
Type of element Bowtie Spiral Log-periodic Non-regular: max effective area with min nb. elts w/o grating lobes. Parameter Specification Low frequency 70 MHz High frequency 450 MHz Nyquist sampling frequency 100 MHz Number of stations 50 => 250 Antennas per station 10.000 CALIM 2011

12 Problem statement Goal: pattern representation for all modes of operation at station level. Too many antennas vs. number of calibration sources Calibrate the main beam and first few sidelobes Suppress far unwanted sources using interferometric methods (open). Compact representations of patterns, inspired from radiation from apertures, including effects of mutual coupling Algarve meeting, 2011

13 Specific to SKA AAlo Fairly circular stations (hexagonal would be OK)
Relatively dense Weak amplitude tapering – some space tapering Irregular => all EEP’s very different Even positions are not 100 % reliable (within a few cm) Correlation matrix not available Nb. of beam coefficients << nb. Antennas Restrict to main beam and first few sidelobes Even assuming identical EEP’s and find 1 amplitude coefficient per antenna is way too many coefficients Algarve meeting, 2011

14 Outline Limits of traditional coupling correction Array factorization
Array factors: series representations Reduction through projection Scanning Algarve meeting, 2011

15 Embedded element pattern
CALIM 2011 Embedded element pattern Z L Impedance isolated elt Array impedance matrix To get voltages in uncoupled case: multiply voltage vector to the left by matrix

16 Embedded element pattern
CALIM 2011 Embedded element pattern Z L After correction, we are back to original problem, with (zoomable, shiftable) array factor Gupta, I., and A. Ksienski (1983), Effect of mutual coupling on the performance of adaptive arrays, IEEE Trans. Antennas Propag., 31(5), 785–791.

17 Isolated Embedded Corrected
CALIM 2011 Mutual coupling correction Half-wave dipole Isolated Embedded Corrected

18 Isolated Embedded Corrected
CALIM 2011 Mutual coupling correction Bowtie antenna l=1.2 m, l=3.5 m Isolated Embedded Corrected

19 Mutual coupling correction
CALIM 2011 Mutual coupling correction Bowtie antenna l=1.2 m, l=1.5 m Isolated Embedded Corrected SINGLE MODE assumption not valid for l < l/2 ~

20 Multiple-mode approach
CALIM 2011 Multiple-mode approach Macro Basis Functions (Suter & Mosig, MOTL, 2000, cf. also Vecchi, Mittra, Maaskant,…) a b g d MBF 1 MBF 2 MBF 3 MBF 4

21 Array factorisation … CALIM 2011 Z L s n Antenna index C111 C211 C311
MBF 1 MBF 2 Coefficients for IDENTICAL current distribution

22 Array factorisation … CALIM 2011 Z L s n Antenna index C111 C211 C311
MBF 1 MBF 2 Coefficients for IDENTICAL current distribution

23 Example array CALIM 2011 - Array radius = 30λ0.
- Number of elements = 1000. λ0 - Distance to ground plane = λ0/4. - No dielectric. λ0 Z = 200Ω

24 Random arrangement CALIM 2011 Random configuration ~ 35 dB E-plane
H-plane

25 Quasi-random arrangement
CALIM 2011 Quasi-random arrangement

26 Radius of Influence H-plane ICEAA 2011 1000 elements 100 elements

27 CALIM 2011 Aperture sampling (1)

28 (several definitions possible)
CALIM 2011 Aperture sampling (2) Define a local density (several definitions possible)

29 CALIM 2011 Aperture scanning (1)

30 CALIM 2011 Aperture scanning (2)

31 Patterns versus size of array
CALIM 2011 Patterns versus size of array

32 Coherent & incoherent regimes
CALIM 2011 Coherent & incoherent regimes ~ ~ 0.3 Number of sidelobes in “coherent” regime

33 Aperture field representation
CALIM 2011 Aperture field representation b a

34 Pattern representation
CALIM 2011 Pattern representation Angle from broadside

35 Polynomial decomposition
CALIM 2011 Polynomial decomposition

36 Fourier-Bessel decomposition
CALIM 2011 Fourier-Bessel decomposition =

37 Fourier-Bessel decomposition
CALIM 2011 Fourier-Bessel decomposition = A. Aghasi, H. Amindavar, E.L. Miller and J. Rashed-Mohassel, “Flat-top footprint pattern synthesis through the design of arbitrarily planar-shaped apertures,” IEEE Trans. Antennas Propagat., Vol. 58, no.8, pp , Aug

38 Zernike-Bessel decomposition
CALIM 2011 Zernike-Bessel decomposition Y. Rahmat-Samii and V. Galindo-Israel, “Shaped reflector antenna analysis using the Jacobi-Bessel series,” IEEE Trans. Antennas Propagat., Vol. 28, no.4, pp , Jul

39 CALIM 2011 Polynomial Fourier-Bessel Zernike-Bessel Fast functions Good 1st order weaker at low orders weak direct convergence fast direct convergence

40 CALIM 2011 Array factor with apodization

41 CALIM 2011 Array factor with apodization

42 Apodization function w(r) extracted
CALIM 2011 Apodization function w(r) extracted

43 Approximate array factor extracted
CALIM 2011 Approximate array factor extracted 20 % error on amplitudes l/4 error on positions (at 300 MHz)

44 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

45 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

46 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

47 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

48 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

49 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

50 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

51 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

52 Residual error with Z-B approach
CALIM 2011 Residual error with Z-B approach

53 CALIM 2011 Density function The number of terms tells the “resolution” with which density is observed

54 Array of wideband dipoles
Algarve meeting, 2011

55 AF convergence Over just main beam
Algarve meeting, 2011

56 AF convergence Main beam + 1st sidelobe
Algarve meeting, 2011

57 Project on 1, 2, 3 MBF patterns at most
AF convergence Project on 1, 2, 3 MBF patterns at most Algarve meeting, 2011

58 Pattern projections Power radiated by MBF pattern 0
NB: can be projected on more than 1 (orthogonal) MBFs

59 Full pattern Algarve meeting, 2011

60 Error w/o MC Algarve meeting, 2011

61 Error after pattern projection
Only 1 pattern used here (pattern of “primary”) Algarve meeting, 2011

62 l =0.0 Algarve meeting, 2011

63 l =0.1 Algarve meeting, 2011

64 l =0.2 Algarve meeting, 2011

65 l =0.3 Algarve meeting, 2011

66 l =0.4 Algarve meeting, 2011

67 l =0.5 Algarve meeting, 2011

68 l =0.6 Algarve meeting, 2011

69 Variation of maximum Real Imaginary Algarve meeting, 2011

70 Conclusion Representation based on array factorization
Projection of patterns of MBF on 1 or 2 of them Representation of array factors with functions use for apertures (done here with 1 array factor) Array factor slowly varying when shifted upon scanning (to be confirmed with more elements and other elt types) Algarve meeting, 2011


Download ppt "Main beam representation in non-regular arrays"

Similar presentations


Ads by Google