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3
Antenna Arrays
• Simple antennas can be combined to
achieve desired directional effects
• Individual antennas are called elements and
the combination is an array
4
Types of Arrays
• Broadside: maximum radiation at right angles to main axis of antenna
• End-fire: maximum radiation along the main axis of antenna
• Phased: all elements connected to source
• Parasitic: some elements not connected to source
– They re-radiate power from other elements
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Yagi-Uda Array
• Often called Yagi array
• Parasitic, end-fire, unidirectional
• One driven element: dipole or folded dipole
• One reflector behind driven element and
slightly longer
• One or more directors in front of driveh
element and slightly shorter
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Stacked Yagis
• Stacking in-phase Yagis with half-
wavelength vertical spacing
• Reduces radiation above and below horizon
• Increases gain in plane of the antenna
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Log-Periodic Dipole Array
• Multiple driven elements (dipoles) of
varying lengths
• Phased array
• Unidirectional end-fire
• Noted for wide bandwidth
• Often used for TV antennas
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Monopole Array
• Vertical monopoles can be combined to
achieve a variety of horizontal patterns
• Patterns can be changed by adjusting
amplitude and phase of signal applied to
each element
• Not necessary to move elements
– Useful for AM broadcasting
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Collinear Array
• All elements along same axis
• Used to provide an omnidirectional
horizontal pattern from a vertical antenna
• Concentrates radiation in horizontal plane
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Broadside Array
• Directional Array
• Uses Dipoles or microstrip or slots
fed in phase and separated by 0.5-0.8
wavelength
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Plane Reflector
• Mount antenna 1/4 wavelength from flat
metallic surface
• Reflected wave and direct wave are in phase
along normal to survace
• Increases radiation in that direction
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Parabolic Reflectors
• All radiation emitted at focus emerges in a
beam parallel to the axis
• Gives a narrow beam
• Suitable mainly at microwave frequencies
because it must be large compared with the
wavelength
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Parabolic Reflector Gain
• As a power ratio (not dB)
• With respect to isotropic
• G = ππππ² D²/ λλλλ²