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C h a p t e r 2 6 : T h e S m i t h C h a r t 569<br />

impedance. For example, using the normalized impedance of Eq. (26.4), the normalized<br />

admittance will be:<br />

1<br />

Y′ =<br />

Z′<br />

1 1.9 − j1.1<br />

= ×<br />

1.9 + j1.1<br />

1.9 − j1.1<br />

1.9 − j1.1<br />

=<br />

3.6 + 1.2<br />

1.9 − j1.1<br />

= = 0.39 − j0.23<br />

4.8<br />

Now compare your answer with the coordinates of the left-Âhand end of the line in Fig.<br />

26.4D. Simply extend the impedance radius through the 1.0,0.0 center point until it<br />

intersects the VSWR circle again. This point of intersection represents the same<br />

normalized load as that found in Eq. (26.4); the only difference is that it is now specified<br />

as a normalized admittance. As you can see, one of the delights of the Smith chart is that<br />

calculations like these are reduced to a quick graphical construction!<br />

<br />

Outer Circle Parameters<br />

The standard Smith chart contains three concentric calibrated circles on the outer perimeter<br />

of the chart. Circle A has already been covered in Fig. 26.4C; it is the pure reactance<br />

circle. The next larger circle B defines the distance in wavelengths as you travel<br />

around the circle. Clockwise motion is toward the generator or transmitter, and counterclockwise<br />

is toward the load or antenna. Circle B is important when transforming an<br />

impedance at one point on a transmission line to the resulting impedance at another<br />

point some distance away.<br />

There are two scales on the wavelength circle (B in Fig 26.4C), and both have their<br />

zero origin at the left-Âhand extreme of the pure resistance line. On both scales one complete<br />

revolution represents a distance of one half-Âwavelength along the line. The scales are<br />

calibrated linearly from 0 through 0.50 such that these two points are identical with<br />

each other on the circle. In other words, starting at the zero point and traveling 360 degrees<br />

around the circle brings one back to zero, which represents one half-Âwavelength,<br />

or 0.5l.<br />

Although both wavelength scales span the same range (0 to 0.50l), they are traversed<br />

in opposite directions. The outer scale is calibrated clockwise and it represents<br />

wavelengths toward the generator; the inner scale is calibrated counterclockwise and<br />

represents wavelengths toward the load. These two scales are complementary at all<br />

points. Thus, 0.12 on the outer scale corresponds to (0.50 minus 0.12) or 0.38 on the<br />

inner scale.

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