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Prohle"" 271<br />

_merit is u=0.08; by (7.126), the ratio <strong>of</strong> true to maximum unilateral gain is<br />

bounded between 0.86 and 1.18 (not dB). Input, device, and output gains by<br />

(E.5), (E.14), and (E.6) are 1.31,2.92, and 1.94 dB, respectively. Therefore, the<br />

maximum unilateral transducer gain is 6.17 dB, obtainable when r, = Sfl and<br />

r,=S!,. According to (7.126), the actual transducer gain 0T is bounded<br />

between 5.51 and 6.89 dB. The families <strong>of</strong> circles are shown in Figure 7.23.<br />

Note that the O-dB circles always pass through the chart center. Also, the<br />

centers <strong>of</strong> all input circles lie on the radial to Sfl' and the same is true for<br />

output circles and S!,. The center <strong>of</strong> the input O.5-dB circle is 0.44 from the<br />

Smith chart center, and its radius is 0.32.<br />

7.5.4. Summary <strong>of</strong> Unilateral Scattering Gain. Considerable numerical and<br />

conceptual simplification is available in unilateral amplifier design when the<br />

assumption is valid. The unilateral figure <strong>of</strong> merit helps make this judgment<br />

and provides bounds on the true value <strong>of</strong> transducer gain.<br />

The optimal matching conditions are the source and load terminations <strong>of</strong><br />

Sf, and S!" respectively. Once device bias has been established. its S'I gain<br />

term is an invariant factor in the unilateral gain formula. Two other factors<br />

represent input and output mismatch. Even less-than-optimal matches can still<br />

produce gain relative to the mismatch between 50 ohms and the input or<br />

output scattering parameters.<br />

The trend toward readily available computers and maximum required<br />

performance reduces the attractiveness <strong>of</strong> the unilateral design technique.<br />

However, there are certain conceptual advantages to recommend it, at least as<br />

a first step in amplifier design.<br />

Problems<br />

7.1. Program coefficient equations (7.3)-(7.5) on a hand-held or desktop<br />

personal computer. Use the subroutines in Program A2-1 <strong>of</strong> Appendix<br />

A.<br />

7.2. Verify the values <strong>of</strong> a;, where i= 1,2,3, in Table 7.1.<br />

7.3. Find the impedance corresponding to reflection coefficient SII =<br />

2.2 (-153° by plotting on a Smith chart and by computation. Assume<br />

that SII is normalized to I ohm.<br />

7.4. Consider the input impedance Zin <strong>of</strong> the pi network in Figure 7.8. For<br />

Zi= 1+jO ohms, Zin= 1O.315823-j20.242819 ohms.<br />

(a) Find the bilinear coefficients <strong>of</strong> Z;n as a function <strong>of</strong> Z;.<br />

(b) Use this bilinear relation to show that Zin = 50 + jO when Zi = j50<br />

ohms.

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