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570 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<br />

The angle of transmission coefficient and angle of reflection coefficient scales are shown<br />

in circle C in Fig. 26.4C. These scales report the relative phase angle between reflected<br />

and incident waves at each point on the line resulting from a given load impedance.<br />

Recall from transmission line theory (see Chap. 4) that a short circuit (R = 0) at the<br />

load end of the line results in the reflected voltage headed back toward the generator<br />

being 180 degrees out of phase with the incident voltage at the reflection point, and<br />

an open line (i.e., infinite impedance) results in the reflected voltage headed back<br />

Âtoward the generator being in phase (i.e., 0 degrees) with the incident voltage at the<br />

load. On the Smith chart, a short circuit at the load corresponds to the left-Âhand end<br />

of the pure resistance line, where 180 degrees is printed on circle C. Similarly, an open<br />

circuit at the load corresponds to the right-Âhand end of the pure resistance line, where<br />

0 degrees is printed. Note that the upper half-Âcircle is calibrated 0 to +180 degrees,<br />

and the bottom half-Âcircle is calibrated 0 to –180 degrees, reflecting how the load impedance<br />

is transformed into either inductive or capacitive reactance, respectively, depending<br />

on how far back from the load the observation point has moved along the<br />

transmission line.<br />

Radially Scaled Parameters<br />

There are six scales laid out on four lines (D through G in Fig. 26.4C and in expanded<br />

form in Fig. 26.5) at the bottom of the Smith chart. These scales are called the radially<br />

scaled parameters—and they are not only very important but often overlooked. With<br />

these scales, we can determine such factors as VSWR (both as a ratio and in decibels),<br />

return loss in decibels, voltage or current reflection coefficient, and the power reflection<br />

coefficient.<br />

As discussed in detail in Chap. 4, the reflection coefficient G is defined as the ratio<br />

of the reflected signal to the incident (or forward) signal. For voltage or current:<br />

VREF<br />

Γ = (26.6)<br />

V<br />

FWD<br />

and<br />

IREF<br />

Γ = (26.7)<br />

I<br />

FWD<br />

Power is proportional to the square of voltage or current, so:<br />

2<br />

Γ<br />

PWR<br />

= Γ (26.8)<br />

or<br />

Γ<br />

PWR<br />

= P P<br />

REF<br />

FWD<br />

(26.9)<br />

Example 26.2 10W of microwave RF power is applied to a lossless transmission line;<br />

2.8W of the 10W total incident power is reflected from the mismatched load. Calculate<br />

the reflection coefficient.

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