Cosy MUTO, JH5ESM

Written in Japanese on 29 Dec., 2005

English translated on 30 Dec., 2005

In this article, a loading antenna design is briefly discussed by the means of Smith chart.

The method is quite simple and useful in actual design.

The concept of Smith chart is out of the range from this document, so the readers not familiar with this should study it elsewhere in the world :p

Consider a horizontal 3.5/10MHz element shown in Fig.1. It is a monopole element so that an opposite element is required for a dipole realization.

L_{1}, L_{2} and L_{H} represent 10MHz λ/4 element, 3.5MHz element and 10MHz adjuster, respectively.

Fig.1 A dual-band loading antenna.

In this example, L_{1} and L_{2} length are 7.42[m] and 4.2[m], respectively. The latter comes from my antenna space limitation.

The loading inductor value and adjuster length are the subject to be determined.

Since the elements L_{1} and L_{2} have already been determnied, plot these electrical length at 3.5MHz on the Smith chart.

L_{1} is 0.087λ at 3.5MHz, so plot a counter clockwise arc from 0[Ω] to 0.087λ position as shown in Fig.2.

L_{2} is 0.049λ at 3.5MHz, so plot a clockwise arc from ∞[Ω] (open end) by 0.049λ.

Fig.2 Calculation of the loading inductance.

Then, the loading inductance value can be easily obtained.

The reactance of 0.087λ element from the feeding point is 0.61Z_{0}, and that of 0.049λ element from open end is 3.15Z_{0}.

Therefore, the reactance of the loading inductor becomes approximately 2.6Z_{0}, where Z_{0} designates characteristics impedance of the element wire.

Let Z_{0} be 500[Ω], the loading inductor is then determined as 59[μH].

The element L_{1} itself resonates on higher frequency band and the loading inductor and lower band element L_{2} are redundant on that band.
The aim of the adjuster is to cancel out
the loading inductor and lower band element at the higher band.

Fig.3 Calculation of the adjuster.

Plot a clockwise arc from ∞[Ω] (open end) by the electrical length of L_{2}
at higer frequency band. In this case, 4.2[m] element corresponds
to 0.141λ at 10MHz band (green arc plot in Fig.3).

Next, calculate the loading inductor reactance at higher frequency band and plot a clockwise arc from L_{2}
reactance position by that value (blue arc plot in Fig.3). The
resultant position implies the impedance seen from the far end of
higher band element.

The adjuster length L_{H}
can be easily obtained by the electrical length from the above
mentioned point to ∞ [Ω] point (red arc plot in Fig.3).

In accurate, the impedance of the loading inductor and lower band
element should be converted into admittance and then canceled out by
the capacitive adjuster admittance.

That's the end of the design.

The antenna tuning is made by the following procedures:

- Disconnect higher band element (L
_{1}) and all the other component. - Tune to the higher band.
- Connect the loading inductor, lower band element and the adjuster. Then tune to the lower band by adjusting L
_{2}. - Tune to the higher band again by the adjuster L
_{H}.

The Smith Chart page on Spread Spectrum Scene has a lot of information on Smith chart.

"A
Great Smith Chart -- 264k .zip file format" file, at the "Some Smith
Chart Examples" section on that page is a 300 dpi GIF format Smith
chart.

Characteristic impedance of a horizontal single wire (Fig.4) is determined by the following equation;

Z_{0} = 138 log_{10} (4h/d) [Ω]

Figure 5 show some calculation results for specific wire size and height.

Fig.4 A horizontal single wire above the ground.

Fig.5 Characteristic impedance of a horizontal single wire.