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HF Helical Antennas: Theory and Practice

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ANTENTOP- 01- 2020, # 024

HF Helical Antennas: Theory and Practice

 

 

Helical antennas with shortened factor more the 10 has unpredictable behavior so it is impossible to make simple plot for such antennas.

 

As you can see from the Figure 8 for feeding helical antennas it is possible use 50 Ohm coaxial cable. However for best match of the helical antenna with transmitter this cable should have electrical length multiplied to half of the resonance wavelength. Some of the simulation antenna program shows the very low input impedance of the short helical antenna. However in my practical measurements I have seen the input impedance in the border of the 30- 60 Ohms (not in the 3- 10 Ohms like the program predicted). I do not argue why it is, bad grounding, losses around or something else... In antenna practice it means that in most of cases you may feed the helical antenna through usual 50- Ohm coaxial cable, is not it?

 

In some cases, the vertical helical antennas initially had input impedance greater than that shown in the plot from Figure 8. Tuning the antenna ground to resonance by length of the counterpoises lowered the input impedance of vertical helical antenna.

 

To reduce influence of coaxial cable connected to shortened helical antenna to parameters of the antenna an RF choke should be installed at the end of the coaxial cable near the antenna feeding terminals. It is may be near 10 ferrite rings installed on the coaxial cable. RF choke made as inductor from coils of coaxial cable as well good choice. Diameter of the coils may be 10- 20- cm and the inductor may contain 5- 20 turns.

 

To increase the efficiency of the helical antenna it is necessary to use wire of the largest possible diameter for the helix, and the diameter of the helix should be the maximum possible for the practical implementation of the antenna. The form of the helix should have low dielectric losses. It is desirable to use even winding of the helix.

 

Q Factor of Helical Antenna

 

Important parameter of helical antenna is the quality (Q) factor. Knowing the Q of the antenna allows approximate the bandwidth and place where the antenna should be installed. The higher the Q of the antenna is the narrower the antenna bandwidth is and the reactive field has high intensity near the antenna during the operation on transmitting. Any subject with RF losses that sitting near the helical antenna will absorb the RF energy when the antenna will transmit. Helical antenna with high shortened factor has narrow bandwidth thereof high Q.

 

 

So helical antenna with high shortened factor will require lots free space nearby otherwise the antenna will heat the subjects that placed near the helical antenna and the RF losses should be present.

 

It is possible easy verified. Just hook- up helical antenna with shortened factor more the 10 to transmitter that provide power more the 50- W. If coaxial cable going to the antenna has ferrite rings at the antenna terminals that the ring will be warm through some times.

 

However the ferrite rings are warm not due the reflected wave on the outer side of the braid. The reactive field near the short helical antenna heat the ferrite rings. Just place the ring near the antenna and the ring (as well as any RF absorption stuff) will be warm.

 

For that reason the ferrite rings should not be used for RF choke with helical antenna with shortened factor more the 5. Usual inductor on 5-20 coils made of the coaxial cable feeding the antenna would be good replacement of the choke with ferrite rings on the coaxial cable.

 

I did measurement of Q of rows of my experimented helical antennas. The antennas were operated at 7- 28- MHz. The antennas had form in diameter 2- 10 cm. Antennas had even winding of the helix.

 

Antennas that were wound on form in 2-5 cm there were wound with wire in diameter of 0.5- mm and more. Antennas that were wound on form in 5- 10 cm there were wound with wire in diameter of 1.0- mm and more. Q factor of the antenna was found as follow:

 

Q=F1/F2.

Where:

 

Q is the quality factor of the antenna;

F1 is the resonance frequency of the antenna;

F2 is the antenna bandwidth.

 

F1, resonance frequency of the antenna, I defined as frequency of the first resonance where SWR of the antenna has minimum value. I used to my home-made RF bridge to measure the resistance of the antenna. The RF -bridge does not show reactance, it shows that sum of the active resistance plus reactance. F2, bandwidth of the antenna I also defined with help of the home- made RF -bridge.

 

 

 

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Last Updated:

January 30, 2021 14:31

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