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General Inverters, Resonators, and End Couplings 291<br />

Inverter<br />

,--------l 2<br />

0__1 : ,-'''-1-+--1-'-/~o<br />

Yl1 1 Y21 Y21 I Yn<br />

0-0_1_-;..1_1<br />

I 1<br />

L- ~<br />

1---;---1_.L-I~o<br />

Figure 8.13. A reciprocal short·circuit~parameter equivalent circuit when Y12 =Y21. The dashed<br />

lines enclose the inverter portion <strong>of</strong> the network.<br />

number. A sufficient condition for Y21 being an imaginary number is that the<br />

network be lossless. In that case, the maximum possible efficiency is unity,<br />

and (7.64) shows that stability factor K = 1. Then the definition <strong>of</strong> K in (7.57)<br />

reveals that K = I when gil = 0 = gZ2 and YZI =jB, thus proving the sufficient<br />

condition.<br />

Note that susceptances YII and Y" in Figure 8.13 become part <strong>of</strong> the<br />

synchronous reactance in their respective resonators, as seen from the particu.<br />

lar case in Figure 8.12b. The frequency behavior <strong>of</strong> the resulting resonators<br />

will be equated to the ideal LC resonator in Section 8.3.4.<br />

Example 8. 2 Iden tify the inverter in a 3D-degree length <strong>of</strong> a lO0-0hm lossless<br />

transmission line, and resonate each end to make a direct-coupled filter<br />

between the 50-ohm terminations. The ABCD parameters <strong>of</strong> a transmission<br />

line in (4.13)-(4.15) can be converted to Y parameters according to (3.86);<br />

YIl= -jYocotO, and Y21= +jYo/sinO. Therefore, inverter YoI2 =Yo/sinO and<br />

half <strong>of</strong> each resonator must be composed <strong>of</strong> admittance -jYocotO. Figure<br />

8.14 shows the equivalent circuit in impedance terms. The equivalent <strong>of</strong> a<br />

shorted-stub transmission line at each end <strong>of</strong> the inverter must be resonated to<br />

make a direct-coupled filter. In this example, ZOIZ =50 ohms, and the shunt<br />

reactances associated with Yll and Y" are +j57.74 ohms. Capacitors on either<br />

end having the negative <strong>of</strong> the latter value are required, as shown in Figure<br />

8.15. Programs A6-1 and A6-2 may be used to confirm the impedances noted<br />

in Figure 8.15. It can be shown that the voltages across the capacitors have a<br />

:_}t",<br />

,--------------,<br />

I Z012 "Zosine I<br />

i 0 ", )\-----L...i-;1'--,t,,~<<br />

Figure 8.14.<br />

I at W o I<br />

L<br />

J<br />

An equivalent circuit for a lossless transmission line having Zo ohms and (J length.

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