Practical_Antenna_Handbook_0071639586

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540 p a r t V I I : t u n i n g , T r o u b l e s h o o t i n g , a n d D e s i g n A i d s against the unwanted emission of harmonics and other spurious products of the signal generation and amplification process, so shielding of the ATU may not be seen as an imperative. However, every tuned circuit in the path between transmitter and antenna helps reduce these undesired emissions across some frequency ranges, so total shielding of the ATU circuitry is always the best practice. Baluns A balun is a transformer that matches a balanced load (such as a horizontal dipole or Yagi antenna) to an unbalanced resistive source (such as a transmitter output or a coaxial feedline). The baluns discussed in this section are lumped-Âcircuit implementations typically wound on ferrite cores, but baluns can also be formed from sections of transmission line properly interconnected. The latter type is included in the review of distributed matching networks near the end of Chap. 4. Toroid Impedance-ÂMatching Transformers The toroidal transformer is capable of providing a broadband match between antenna and transmission line, or between transmission line and transmitter or receiver. The other matching methods (shown thus far) are frequency-Âsensitive and must be readjusted whenever the operating frequency is changed by even a small percentage. Although this problem is of no great concern to fixed-Âfrequency radio stations, it is of critical importance to stations that operate on a variety of frequencies or widely separated bands of frequencies. Figure 24.7A shows a trifilar transformer that provides a 1:1 impedance ratio, but it will transform an unbalanced transmission line (e.g., coaxial cable) to a balanced signal required to feed a dipole antenna. Although it provides no impedance transformation, it does tend to balance the feed currents in the two halves of the antenna. This fact makes it possible to obtain a more symmetrical figure eight dipole radiation pattern in the horizontal plane. Many station owners make it standard practice to use a balun at the antenna feedpoint when using coaxial (unbalanced) transmission line, even if the feedpoint impedance is close to the Z 0 of the cable. The balun shown in Fig. 24.7B is designed to provide unbalanced to balanced transformation in conjunction with a 4:1 impedance transformation. Thus, a 300-ÂW folded R 2 R unbalanced R 1 L 1 L 2 R balanced R 2 = 4R 1 Figure 24.7A Balun 1:1. Figure 24.7B Balun 1:4.

C h a p t e r 2 4 : a n t e n n a T u n e r s ( A T U s ) 541 16:1 9:1 R 1 4:1 R 2 1.5:1 Figure 24.7D Commercial tapped transformer. Figure 24.7C Tapped multiple-Âimpedance BALUN. dipole feedpoint impedance will be transformed to 75-ÂW unbalanced. This type of balun is often included inside ATUs. L 1 and L 2 have equal turns. Another multiple-Âimpedance transformer is shown in Fig. 24.7C. In this case, the operator can select impedance transformation ratios of 1.5:1, 4:1, 9:1 or 16:1. A commercial version of this type of transformer, shown in Fig. 24.7D, is manufactured by Palomar Engineers; it’s intended for feeding vertical HF antennas. It will, however, work well in other impedance-Âtransformation applications, too. Figures 24.7B and 24.7C are specific examples of what can be accomplished using a toroidal core of the right material and power-Âhandling capability in conjunction with an autoformer winding, where both input and output loads are referenced to a common ground. If ground isolation is important, there is no reason completely separate windings can’t be used, in a configuration analogous to a link-Âcoupled coil. Ferrite Core Inductors The word ferrite refers to any of several examples of a class of materials that behave similarly to powdered iron compounds and are used in radio equipment as the cores for inductors and transformers. Although the materials originally employed were of powdered iron (and indeed the name ferrite still implies iron), many modern materials are composed of other compounds. According to literature from Amidon Associates, ferrites with a relative permeability, or µ r , of 800 to 5000 are generally of the manganese-Âzinc type of material, and cores with relative permeabilities of 20 to 800 are of nickel-Âzinc. The latter are useful in the 0.5-Â to 100-ÂMHz range. Toroid Cores In electronics parlance, a toroid is a doughnut-Âshaped object made from a ferrite material and used as the form for winding an inductor or transformer. Many different core material formulations are available for the designer to choose from, based on the expected frequency range and power levels of the application. Unlike just about any other lumped component available to the experimenter, most toroids carry little or no information about themselves on their surface. In general, blindly grabbing an arbitrary toroid from the junk box will lead to a failed project. Toroids must be selected carefully—with the use of a test jig, if necessary.

C h a p t e r 2 4 : a n t e n n a T u n e r s ( A T U s ) 541<br />

16:1<br />

9:1<br />

R 1<br />

4:1<br />

R 2<br />

1.5:1<br />

Figure 24.7D Commercial<br />

tapped transformer.<br />

Figure 24.7C Tapped multiple-Âimpedance BALUN.<br />

dipole feedpoint impedance will be transformed to 75-ÂW unbalanced. This type of balun<br />

is often included inside ATUs. L 1 and L 2 have equal turns.<br />

Another multiple-Âimpedance transformer is shown in Fig. 24.7C. In this case, the operator<br />

can select impedance transformation ratios of 1.5:1, 4:1, 9:1 or 16:1. A commercial<br />

version of this type of transformer, shown in Fig. 24.7D, is manufactured by Palomar<br />

Engineers; it’s intended for feeding vertical HF antennas. It will, however, work well in<br />

other impedance-Âtransformation applications, too.<br />

Figures 24.7B and 24.7C are specific examples of what can be accomplished using a<br />

toroidal core of the right material and power-Âhandling capability in conjunction with an<br />

autoformer winding, where both input and output loads are referenced to a common<br />

ground. If ground isolation is important, there is no reason completely separate windings<br />

can’t be used, in a configuration analogous to a link-Âcoupled coil.<br />

Ferrite Core Inductors<br />

The word ferrite refers to any of several examples of a class of materials that behave<br />

similarly to powdered iron compounds and are used in radio equipment as the cores for<br />

inductors and transformers. Although the materials originally employed were of powdered<br />

iron (and indeed the name ferrite still implies iron), many modern materials are<br />

composed of other compounds. According to literature from Amidon Associates, ferrites<br />

with a relative permeability, or µ r , of 800 to 5000 are generally of the manganese-Âzinc<br />

type of material, and cores with relative permeabilities of 20 to 800 are of nickel-Âzinc.<br />

The latter are useful in the 0.5-Â to 100-ÂMHz range.<br />

Toroid Cores<br />

In electronics parlance, a toroid is a doughnut-Âshaped object made from a ferrite material<br />

and used as the form for winding an inductor or transformer. Many different core<br />

material formulations are available for the designer to choose from, based on the expected<br />

frequency range and power levels of the application.<br />

Unlike just about any other lumped component available to the experimenter, most<br />

toroids carry little or no information about themselves on their surface. In general,<br />

blindly grabbing an arbitrary toroid from the junk box will lead to a failed project. Toroids<br />

must be selected carefully—with the use of a test jig, if necessary.

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