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242 Linear Amplifter <strong>Design</strong> Tools<br />

Figure 7.5.<br />

R,w<br />

The bilinear transformation w=T+Rp,<br />

(Y = I/Z) always map circles and lines into circles and lines. For bilinear<br />

transformations in linear networks, there is a much more useful decomposition<br />

<strong>of</strong> the standard bilinear form in (7.1); this is<br />

Z-Z<br />

w=T+R Z<br />

+ Z<br />

;' (7.38)<br />

In (7.38), T locates the center <strong>of</strong> the branch-image circle, the magnitude <strong>of</strong> R<br />

scales its size, and the angle <strong>of</strong> R determines its rotation with respect to the<br />

w-plane coordinate system. The branch-image Smith chart has a complex<br />

normalizing impedance (Z,), as explained in Section 7.1.2. This is illustrated in<br />

Figure 7.5.<br />

The significance <strong>of</strong> (7.38) and Figure 7.5 stems from the bilinear theorem in<br />

Section 7.2.2. The small, rotated Smith chart represents the entire right-half<br />

plane .<strong>of</strong> any linear network branch impedance, admittance, or scattering<br />

parameter. The w plane represents the network's response function, expressed<br />

as a scattering, impedance, or admittance parameter. So the w plane might be<br />

the Zin plane, the Yin plane, the S\2 plane, etc. The small branch-image circle<br />

mayor may not fall within the w-plane unit circle, should that be a scattering<br />

parameter and therefore relevant.<br />

It is not difficult to find expressions for the complex constants T, R, and<br />

Z,. These relationships are obtained by putting (7.38) into the form <strong>of</strong> (7.1)<br />

and comparing the coefficients <strong>of</strong> Z. Thus (7.38) becomes<br />

It is seen that<br />

and<br />

Z[(T+ R)/Zn + [T- R(ZJZn]<br />

w= Z(I/Zn+ 1 (7.39)<br />

(7.40)<br />

a 1 R=--T.<br />

a,<br />

(7.41)

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