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184 Impedance Matching<br />

chart locus from P2 to P, is plotted with a radius that decays with the angle by<br />

the - 2NP exponential term in (6.26); i.e., it spirals inward.<br />

Example 6.5. Consider the lossless (NP= 0) transmission line in Figure 6.11,<br />

terminated by Z2 = 40 + j30 ohms. Suppose that the characteristic impedance is<br />

50 ohms. By (6.24), P2=0.3333 190°; this is plotted in Figure 6.12. By (6.26),<br />

a 45-degree line rotates P2 clockwise by 90 chart degrees to locate input Pia; a<br />

90-degree line rotates P2 clockwise by 180 chart degrees to locate P,b' By<br />

(6.24), Pia = 0.3333 10° corresponds to Z, = 100+jO ohms; similarly, P,b=<br />

0.3333 1_90° corresponds to Z, =40-j30 ohms. If dissipation loss NP had<br />

not been zero, the radius <strong>of</strong> 0.3333 would have decreased with rotation.<br />

Further considerations will involve only lossless transmission lines; so it is<br />

useful to equate "If = jO in (6.23). This reduces to the input impedance<br />

expression for a lossless transmission line:<br />

Z2+jyZO<br />

Z,=ZOZ . Z '<br />

o+JY 2<br />

where definition (4.22) is repeated:<br />

y=tanO.<br />

(6.27)<br />

(6.28)<br />

X=" +0.5<br />

x = -0.5<br />

-1<br />

I I I I I I I I I I I<br />

1.0 0.8 0,6 0.4 0.2 0 0.2' 0.4 0.6 0.8 1.0<br />

_I<br />

Figure 6.12. LossJess transmission line rotation on a Smith chart for Example 6.5.

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