A 100[Ω] -lossless line is 0.24λ long, and is terminated in a load impedance
Z_{L} = 140 + j130 [\Omega] . By using the Smith chart, find
(a) voltage reflection coefficient,
(b) input impedance,
(c) standing wave ratio, and
(d) location of the first voltage maximum from the load.
(a) Normalized load impedance is
Z_{L} = (140 + j130) / 100 = 1.4 + j1.3.
The intersection of the r = 1.4 circle and the x = 1.3 circle is marked as A on the Smith chart in Fig. 9.16.
From the Smith chart we find that
(1) \frac{\overline{OA} }{\overline{OD} } = 0.5 = \left|\Gamma \right|, and
(2) point A is located at 0.188λ on the wtg scale.
Noting that the wtg of 1λ corresponds to 4π[rad] , the phase angle of point A is calculated as follows:
Φ = (0.25 – 0.188) × 4π = 0.78[rad].
Thus, \Gamma = 0.5 e^{j 0.78}.
(b) Move from point A to point C along the circle of |Γ| = 0.5, in the clockwise
direction, by increasing the wtg by 0.24λ .
At point C, we read r = 0.40 and x = −0.42 .
The input impedance is therefore
Z_{in} = 100 (0.40 – j0.42) = 40 – j42[\Omega ].
(c) The circle of |Γ| = 0.5 crosses the positive \Gamma_{R}-axis at point B, where we read r = 3.0 and x = 0 .
Thus, the standing wave ratio is S = 3.0 .
(d) A voltage maximum occurs at a distance \ell ^{\prime} . from the load, at which
z_{in}(\ell^{\prime }) = r^{\prime } + j0 (r^{\prime } \gt 1) . This point is marked as B. The difference in wtg between points B and A is equal to \ell ^{\prime} , that is,
\ell ^{\prime} = (0.25 − 0.188)λ = 0.062λ.