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Slot, Horn and Complementary Antennas Slot, Horn and Complementary Antennas

Slot, Horn and Complementary Antennas - PowerPoint Presentation

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Slot, Horn and Complementary Antennas - PPT Presentation

EEE 212 Figures are from Kraus Antenna book And Balanis Antennas Complementary Antennas Dipole Slot Stub and slot look at currents Dipole Current and Voltage Distribution Voltage ID: 1017875

plane horn complementary slot horn plane slot complementary pyramidal sectoral field screen impedance antennas phase antenna pattern patterns dipole

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1. Slot, Horn and Complementary AntennasEEE 212Figures are from Kraus’ Antenna bookAnd Balanis’ Antennas

2. Complementary AntennasDipole Slot

3. Stub and slot – look at currents

4. Dipole Current and Voltage DistributionVoltageCurrent

5. Slot Current and Voltage DistributionVoltageCurrent

6. Slot antenna feeds

7. Vertically and Horizontally polarized slots Sheet with slot radiates equally on both sides of the sheet.

8. Boxed-In SlotRadiates only from one side

9. Waveguide-Fed SlotRadiation only from one side

10. Slotted Waveguide

11. Complementary AntennasSlot and Dipole

12. Radiation Patterns of Slot and Dipole

13. Complementary AntennasDipoleSlothttps://www.feko.info/applications/white-papers/microstrip-fed-slot-antenna/microstrip-fed-slot-antenna/viewhttp://www.cisco.com/c/en/us/products/collateral/wireless/aironet-antennas-accessories/prod_white_paper0900aecd806a1a3e.html

14. Babinet’s PrincipleSlot antenna problems can be reduced to solving complementary wire antennas

15. Babinet’s PrincipleIt also holds when there’s diffraction.The field at any point behind the plane having a screen if added to the field at the same point when the complementary screen is substituted is equal to the field at the point when no screen is present.

16. Booker’s extension of Babinet’s principleBabinet’s principle is extended by Booker to take into account vector nature of EM Field.If the screen is perfectly conducting, the complementary screen has infinite permeabilityMetals are good conductors, but there’s no perfectly permeable materials -> equivalently use metal but interchange electric and magnetic fields everywhere

17. Booker’s ExtensionDipole is vertical because we’re interchanging electric and magnetic fieldsBabinet’s principle:

18. Impedance of complementary screensWe will look at Babinet’s principle applicationPropagation of waves through space can be represented by a transmission-line analogyImpedance of the line is 377OhmsImpedance of screen is Y1Impedance of complementary screen is Y2

19. Impedance of Screen

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21.

22. Impedance of Complementary ScreenBabinet’s Principle ->

23.

24. If the input impedance of a dipole is Zd, find the impedance of the slot

25. If the input impedance of a dipole is Zd, find the impedance of the slot

26. Examples

27. Another example

28. Horn antennasEEE 212

29. Horn AntennasAre flared-out waveguidesThey produce uniform phase front with a larger aperture -> higher directivityDr. Bose constructed a pyramidal horn in 1897

30. Sir Jagadish Chandra Bose1858-1937

31. The receiver (left) used a galena point contact crystal rectifier inside the horn antenna and a galvanometer to detect the waves.60GHz Receiver and Transmitter used by Sir Jagadish Chandra Bose in Bose Institute, Kolkata

32. Types of Horn Antennas

33. Types of Horn Antennas

34. The fields at the aperture of the E-plane sectoral hornExpressions are similar to the field distribution of a waveguide, except quadratic phase term. The necessity of the quadratic term can be illustrated geometrically.

35. Quadratic Phase TermWe assume that the cylindrical waves are radiated from a wire at the apex of the apertureThe constant phase fronts are cylindricalThe phase at the aperture varies because the wave has traveled different distances from the apex to the apertureThe difference in path of travel can be obtained from the geometry

36. HornWe look at the horn’s cross-sectionDeviation from constant phaseHorn Length as a function of phase deviationHorn Flare angle as a function of phase deviation

37. HornWe look at the horn’s cross-section

38.

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41. Comparison of rectangular horn patternsDonald Rhodes experimentally investigated horn patterns as a function of radial length RFlare angle

42. Experimentally obtained optimum dimensions of rectangular hornFrom Rhode’s experiments optimal dimensions were selected for E and H flare as a function of flare angle

43. Rectangular Horn patternsMinor lobesMinor lobesDue to E-field distribution in E and H plane

44. Types of Horn Antennas

45. Types of Horn Antennas

46.

47. Radiated Field of an E-plane sectorial horn

48. 3D Pattern of E-plane Sectoral HornE-plane narrower than H-plane

49.

50. Normalized pattern in E-planeC, S are Fresnel Integrals, tabulated in Appendix IV, Balanis

51. E and H plane patterns of an E-plane sectoral horn

52. Find normalized E-field intensity for any E-plane sectoral hornDetermine value of s from given b1 and rho1Search for that s on the next figure and find the strength of the electric fieldAdd 20log10[(1+cos )/2]

53. E-plane universal patterns for E-plane sectoral and pyramidal horns

54.

55.

56. E and H plane patterns of an E-plane sectoral horn

57. Directivity of E-plane sectoral horn13.9c

58. Normalized Directivity of E-plane Sectoral Horn

59. Another Way to Calculate Directivity of E-plane sectoral horn

60.

61.

62.

63.

64.

65. Pyramidal Horn

66. Pyramidal Horn E-plane

67. Pyramidal Horn H-plane

68. Pyramidal Horn 3-D Pattern

69. Radiation Pattern E-plane

70. Radiation Pattern H-plane

71. Pyramidal Horn Construction

72. Pyramidal Horn Directivity

73. Pyramidal Horn Directivity

74.

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78.

79.

80.

81. Homework13.213.313.21