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1996 -
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Kirt Blattenberger,

BSEE
- KB3UON

RF Cafe began life in 1996 as "RF Tools" in an AOL screen name web space totaling 2 MB. Its primary purpose was to provide me with ready access to commonly needed formulas and reference material while performing my work as an RF system and circuit design engineer. The Internet was still largely an unknown entity at the time and not much was available in the form of WYSIWYG ...

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September 1958 Radio-Electronics Article

September 1958 Radio-Electronics [Table of Contents]These articles are scanned and OCRed from old editions of the Radio & Television News magazine. Here is a list of the Radio-Electronics articles I have already posted. All copyrights are hereby acknowledged. |

Here is a short tutorial on how to design a resistive impedance matching circuit for feeding multiple transmission lines of equal impedance. Both series and parallel feeds are presented. As the author mentions, ideally you would like a lossless transformer for matching, but often a resistive network is acceptable, especially if receive signal power is not an issue and if your transmitter power is sufficient to overcome the resistive losses (and doesn't torch the resistors). It is also possible to match transmission lines of different impedances, but the equation would get messy. Although it would mean even more resistive loss, the simplest way to match unequal impedance lines is to first match to a value most of the lines exhibit, then build a separate resistive transformer for the line(s) that are different to connect between the main match network and the unequal line(s). That sounds confusing even as I write it, but it is correct ;-)

Transmission Line Matching

By Henry A. Kampf

Resistance match three or more lines to one antenna

Connecting three or more transmission lines poses the problem of proper impedance matching to minimize standing waves in the system. Ideally, lines would be matched with rf impedance-matching transformers which do not dissipate energy. Therefore the rf power would be equally divided among all of the lines.

Lines can also be matched properly with ordinary 1/2-watt carbon resistors, if the lines all have the same characteristic impedance and if the power lost in the resistors does not reduce the signal below a usable level. This condition occurs in strong-signal areas where several receivers are connected to a common antenna. Any mismatch can cause standing waves which appear as ghosts on the TV screen. In such areas reduction in signal strength is not important but the match of the rf lines is quite critical. Similar situations occur with test equipment and occasionally in amateur applications.

When matching with resistors, two connections are possible. The series resistor connection is used for lines having
a common ground, such as coaxial cables. The shunt resistor connection can be used with balanced lines Figs. 1 and
2 show how the matching networks are connected and give the formulas for calculating the necessary resistor values.
The symbols used in the equations are: Z_{0} - characteristic impedance of the transmission lines used; N
- total number of lines that are joined; R - resistor value required in the diagrams.

When one of these lines is a signal source, the loss of the network for this signal down to anyone of the other
lines is calculated from the equation L = 20 log (N - 1), where L is the loss in db. This equation is the same :for
either the series or shunt connection. In the examples of Figs. 1 and 2 five lines are joined; therefore, N is 5.
If 300-ohm transmission lines are used, Z_{0} is 300. Substituting these values into the equations we find
that the required resistance R is 180 ohms for the series connection and 500 ohms for the shunt connection. The signal
strength appearing on anyone of the lines will be 12.04 db down from the signal applied to anyone of the other lines.

Fig. 1 - Series connecting coaxial lines. Fig. 2 -
Shunt connecting two-lead lines.

All lines have a common
ground.

Posted September 8, 2014