Radcom Feb 2019 “cable balun” – comment on Radcom “The last word” letter

At Radcom Feb 2019 “cable balun” and
Radcom Feb 2019 “cable balun” – a deeper look I wrote about a novel balun by K3MT.

 

Fig 1

Above is a diagram of the so-called “cable balun”.

My evaluation essentially showed that it was not effective in an example practical scenario where one might want to use a balun, and that of itself, it was not likely to significantly reduce common mode current in most scenarios.

Radcom Mar 2020 published  a letter in “The last word” from the author defending the device citing a NEC model of one scenario, curiously though without explanation, a different topology to the diagram above from the original article. Note also that it is a structure in free space with no discussion of how that is relevant to real world antennas near ground.

Fig 2

The author states it is an NEC4 model, and I have run it in NEC-4.2 but I doubt that it will give significantly different results in NEC-2.

I have made two changes to the model:

  • remove the RP card as it is supplied by 4NEC2 (no effect on the model); and
  • reversed the direction of wire 1 to be consistent with wire 2 for more understandable graphics.

Here is the retyped NEC deck.

CM Typed from Radcom March 2020 pages 97-98. K3MT Letter
CM RSGB CABLE BALUN STUDY
CM AUTHOR: K3MT@JOKALYMPRESS.COM
CM 40 M DIPOLE IN FREE SPACEH
CM 20m LENGTH 5MM DIAMETER
CM 
CM THE DIPOLE
CM THE BALUN
CM THE HALF WAVE FEEDLINE
CM NO GROUND - FREE SPACE
CM 
CM VOLTAGE SOURCE 2V AT CENTER OF DIPOLE
CM 6700 kHz
CM RADIATION PATTERN
CE
GW	1	48	-10.2	0	10.0	0	0	10.0	0.005
GW	2	52	0	0	10.0	10.5	0	10.0	0.005
GW	3	25	0	0	10.0	0	5.4	10.0	0.005
GW	4	25	0	0	9.5	0	5.4	9.5	0.005
GW	5	5	0	5.4	10.0	0	5.4	9.5	0.005
GW	6	100	0	0	9.5	0	0	-10.0	0.005
GE	0
GN	-1
EK
EX	0	1	48	0	2.0	0	0
FR	0	0	0	0	6.700	0
EN

K3MT’s model

Fig 3

Above is a plot of the current distribution of the model given by K3MT to demonstrate the balun performance.

K3MT’s model with longer vertical conductor

To discover whether the common mode current is well controlled by K3MT’s balun, lets extend the vertical conductor (modelling the feed line common mode current path).

Fig 4

Above is a plot of the current distribution of the revised model, it is clear that common mode current on the vertical conductor has increased significantly.

Fig 5

Above is a slice of the antenna pattern which shows significant distortion due to the asymmetry of the antenna system.

K3MT’s model with shorter vertical conductor

If the common mode current is sensitive to vertical conductor length, let’s try a little shorter conductor.

Fig 6

Above is a plot of the current distribution of the revised model, common mode current is significantly lower.

Analysis

Comparing figures 4 and 6 which show a marked variation in common mode current caused by changing the linear length of conductor from feed point to lowest extremity from 3λ/4 to λ/2 hints that the common mode current may be simply responsive to that length and the nature of termination (ie open end or grounded), and that K3MT’s folded section doesn’t of itself control common mode current.

Conclusions

K3MT’s balun in his demonstration scenario has not isolated the nominal radiator (the flat top dipole) from the influence of the common mode feed line conductor.

The model results are applicable to the structure in free space and not directly extensible to an antenna system near ground, much less a grounded transmitter.