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142 P a r t I I : F u n d a m e n t a l s<br />

Now we know l and the tangent of bl, so we can find b, the phase constant of the line from<br />

trig tables or our scientific calculator.<br />

More likely, we would like to know v F , the velocity factor of the line. Rearranging Eq.<br />

(4.16), we obtain<br />

2<br />

v = π f<br />

F<br />

cβ<br />

(4.49)<br />

Because a shorted or open length of transmission line always exhibits a pure reactance<br />

at the other end, such lines are often used to match an antenna to its transmission<br />

line. A specific reactance, either capacitive or inductive, can be obtained simply by adjusting<br />

the length of the line, or stub.<br />

In most cases, however, not only do we need to cancel out the reactive part of the<br />

feedpoint impedance, we also want to change the resistive part to match the Z 0 of the<br />

feedline. Simply adjusting the length of the stub cannot compensate for both the resistive<br />

and the reactive mismatches. A second adjustable variable is needed. That turns out<br />

to be the distance of the stub back toward the transmitter from the antenna feedpoint.<br />

For a variety of reasons, both electrical and mechanical, stubs are more often found<br />

connected in parallel, across the feedline, than in series with one side of the feedline. In<br />

such cases, it is far easier to work with the reciprocal of the impedances involved. These<br />

admittances, denoted by Y, consist of a shunt conductance G (the purely resistive part of<br />

the admittance) in parallel with a shunt susceptance B, which is the purely reactive part.<br />

Mathematically, if Z = R + jX, then<br />

1 1<br />

Y = = = G + jB<br />

(4.50)<br />

Z R + jX<br />

1<br />

To put into the right form, we multiply both top and bottom by R – jX, the<br />

R + jX<br />

complex conjugate of R + jX. This gives us<br />

Thus,<br />

and<br />

⎡ 1 ⎤⎡R<br />

− jX ⎤ R − jX<br />

⎢ ⎥⎢<br />

⎥ =<br />

2 2<br />

⎣R<br />

+ jX ⎦⎣R<br />

− jX ⎦ R + X<br />

R<br />

G =<br />

R + X<br />

2 2<br />

B = − jX<br />

R + X<br />

2 2<br />

(4.51)<br />

(4.52)<br />

(4.53)<br />

In a small percentage of stub-matching cases, it turns out to be possible to locate the<br />

stub right at the antenna feed terminals. Most often, however, a stub must be located at<br />

some specified distance from the antenna feedpoint.<br />

Without the use of paper or online Smith charts, stub matching is far more difficult<br />

than it needs to be. Chapter 26 includes a detailed example of stub matching using a<br />

Smith chart.

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