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Antenna Design

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Basic Definitions of Antennas 

​Antennas can transmit as well as receive radio waves in a particular 

frequency range 

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Properties of Antennas 


• A receiving antenna converts electromagnetic radiation (radio waves) 

into an alternating current or voltage. 

• A transmitting antenna converts an alternating current or voltage into 

electromagnetic radiation (radio waves). 

• Antennas are transducers that convert the electromagnetic wave from 

free progressive waves into pipeline bound waves -or vice versa.

free progressive waves into pipeline bound waves or vice versa. 

• All antennas have directional qualities. They do not radiate power 

equally in all directions. 

• The gain of an antenna increases with the amount of its directivity. 

​• Antenna gain and directivity are strongly related to each other. 



Polarization of Antennas 

​• The polarization of an antenna is the orientation of the electric field of the radio 

wave with respect to the earth‘s surface. 

• Polarization can be vertical, horizontal or circular. 

• It is determined by the physical structure of the antenna and by its orientation. 

R. Fochler 2013 

• It has nothing in common with the term „Antenna directionality“ 


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​• A linear polarized antenna (vertical or horizontal) radiates in one 

plane containing the direction of propagation. 


• In a circular polarized antenna, the plane of polarization rotates in a 

circle making one complete revolution during one period of the wave. 


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Types of Antennas 

• The physical construction of a antenna determines the 
directionality of the antenna. 
• The simpliest form would be a whip antenna, consisting of a single 
straight wire or rod. Such antennas are omni directional, radiating in 
all horizontal directions with the same power. 
​• The whip antenna is a „resonating“ antenna, therefore the length of 
the whip antenna is determined by the length of the radio waves 
used. 
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The dipole is a very common antenna and it is half a wavelength long. 

This antenna works best when the waves arrive broadside. 

 

Due to smaller housing sizes, the length of transmitter-and receiver 

antennas are usually matched to ¼ of a wave length. 

 
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The higher the frequency range, the shorter the antennas! 

 

• Yagi -Uda antenna 

​A dipole which shows a narrow directivity and a high antenna gain through an 

array of directors and reflectors. The number of directors and theire length 

determine the bandwidth and the frequency range of the antenna. 

 
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• Logarithmic Periodical Dipole antennas (Log Periodicals) 

​Array of dipoles connected with each other via a feeder line. The length and 

spaceings of the elements increase logarithmically from one end to the other. 

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• More complex forms , variations of the dipole 

​Dipoles may be used as standalone antennas themselves, but 

they are also employed as a feed antenna (driven element) in 

many more complex antenna types, such as: 

-Yagi antenna, 

-Parabolic antenna, 

-Log periodic antenna, 

-Ground plane antenna 

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Antenna patterns 

​• Constructive elements can change the directivity of antennas 

• To describe these qualities of directivity, there are 2 common forms to 

line out the beamwidth in a plot 

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                                                                                         horizontal 
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​ 


Evolution and Propagation 

​Magnetic field evolution of a vertical oriented Dipole 


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Antenna Gain 

• An antenna's gain is a key performance figure which combines the 

antenna’s directivity and electrical efficiency. 

• As a transmitting antenna, the figure describes how well the antenna 

converts electrical input power into radio waves headed in a specified 

direction. 

direction. 

-Gain is needed for long distance radio links 

• As a receiving antenna, the figure describes how well the antenna 

converts radio waves arriving from a specified direction into electrical 

power. 

-Gain is needed to overcome long cable runs 


• The ideal omnidirectional radiation from a point source would be an 

isotropic antenna. 

• Antenna gain is usually expressed with reference to an isotropic 

radiator. (dBi) 

• Antennas cannot create gain 

• Gain is achieved by radiating more energy in some directions than 

others.

  • Total radiated power cannot be more than the power input to the 

antenna 

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• Active elements like boosters can increase the gain of an antenna 

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Antenna Cable 

​To remain quality and strength of a radio signal when converting from free-field into 

cable bound signal, it is essential to use antenna cable and connectors that meet 

certain specifications. 

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Antenna Cable Specifications 

• Nominal Impedance 

-usually 50ohms 

• Velocity of propagation 

-between 65 – 87% (of SOL) 

• Capacitance 

 -between 75 – 95pF/m 

• DC resistance 

-inner conductor: 4-20ohms, outer conductor: 5-7ohm 

​• Attenuation 

-0,5 – 0,1dB/m 



Cable Attenuation 

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Cable length adjustment 

​Passive antennas connected to 5m RG58 going to the receiver 

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The input gain into the receiver should 

be as close as possible to 0dB! 

 

Passive antennas connected to 20m RG58 going to the receiver

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​The input gain into the receiver should 

be as close as possible to 0dB! 



Active antennas connected to 5m RG58 going to the antenna splitter 


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Active antennas connected to 20m RG58 going to the antenna splitter 

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RF gain attenuation is possible when 

using an antenna splitter PS4000 / APS4! 



Passive antennas connected to 20m RG213 going to the receiver. 


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AB4000W – Antenna Booster 

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ASU4000 – Antenna Supply Unit ​

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• Supplies up to three active elements (RA4000 B/EW, SRA 2 B/EW, AB4000, AB4000 EW) ​

 

​Cable length adjustment 

SRA2 B/EW Antenna + 100m cable RG58​

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Antenna cable calculator 

​Common cable types and their attenuation figures: 


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Last modified at 4/16/2021 8:50 AM by PRO Knowledge Base
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