Friis Transformation and Radiation from Dipole

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Week 3

Last updated 5:15 PM on 5/27/26
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12 Terms

1
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Equivalent Circuit of Antenna

ZA = RA + j XA

RA = RR + RL

  • RR - Radiation resistance

  • RL - Loss resistance

  • XA - Antenna reactance

<p>Z<sub>A</sub> = R<sub>A</sub> + j X<sub>A</sub></p><p>R<sub>A</sub> = R<sub>R</sub> + R<sub>L</sub></p><ul><li><p>R<sub>R</sub> - Radiation resistance</p></li><li><p>R<sub>L</sub> - Loss resistance</p></li><li><p>X<sub>A</sub> - Antenna reactance</p></li></ul><p></p>
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Radiation Efficiency

𝜂r = power radiated / (power radiated + power lost) = RR / (RR + RL)

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Power dissipated (as heat) by antenna

PA = ½ * |𝐼|2 * (𝑅𝐿+𝑅𝑅)

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Reflection coefficient

Γ = (𝑍𝐴 − 𝑍𝑂 ) / (𝑍𝐴 + 𝑍𝑂)

where 𝑍𝑂 is the characteristic impedance of transmission line

when 𝑍𝐴 = 𝑍𝑂 → Γ = 0 = perfect match

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VSWR

VSWR = Voltage Standing Wave Ratio = (1 + | Γ |) / (1 − | Γ |)

How well an antenna is matched or how much power it will accept from a source

VSWR of 1 indicates a perfect match

6
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Impedance of Free Space

377

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Antenna Effective Area

A measure of the ability of an antenna to capture energy

Ae = Power delivered to load / Incident power density = 𝐺𝜆2 / 4𝜋

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Aperture Efficiency

𝜂Ae = effective area / physical area

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Antenna Bandwidth

Band of frequencies within which antenna performance characteristics are acceptable

Characteristics:

  • Input impedance

  • Beamwidth

  • Gain

  • Sidelobes

  • VSWR

  • Axial ratio

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Antenna Effective Collecting Area

The effective absorption area (Ae), presented by an antenna, gives an indication of the power collected/absorbed (PR) as in response to an incident plane wave.

PR = PAAe

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Dipole Antennas

  • Common antenna at low frequencies < 1GHz

  • A linear conductor driven at its centre

  • Simplest dipole to analyse is a short (Herzian) dipole

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Dipole Antennas Pattern

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